aastex.cls0100644000000000000000000020121410376206774011561 0ustar rootroot%% %% This is file `aastex.cls', %% generated with the docstrip utility. %% %% The original source files were: %% %% aasclass.dtx (with options: `class') %% %% This is a generated file; %% altering it directly is inadvisable; %% instead, modify the original source file. %% %% Copyright notice. %% %% These files are distributed %% WITHOUT ANY WARRANTY; without even the implied warranty of %% MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. %% %% \CharacterTable %% {Upper-case \A\B\C\D\E\F\G\H\I\J\K\L\M\N\O\P\Q\R\S\T\U\V\W\X\Y\Z %% Lower-case \a\b\c\d\e\f\g\h\i\j\k\l\m\n\o\p\q\r\s\t\u\v\w\x\y\z %% Digits \0\1\2\3\4\5\6\7\8\9 %% Exclamation \! Double quote \" Hash (number) \# %% Dollar \$ Percent \% Ampersand \& %% Acute accent \' Left paren \( Right paren \) %% Asterisk \* Plus \+ Comma \, %% Minus \- Point \. Solidus \/ %% Colon \: Semicolon \; Less than \< %% Equals \= Greater than \> Question mark \? %% Commercial at \@ Left bracket \[ Backslash \\ %% Right bracket \] Circumflex \^ Underscore \_ %% Grave accent \` Left brace \{ Vertical bar \| %% Right brace \} Tilde \~}% %%% @LaTeX-file{ %%% filename = "aastex.dtx", %%% version = "5.2", %%% date = "2005/06/22", %%% time = "16:23:00 GMT", %%% checksum = "5964", %%% author = "Arthur Ogawa (mailto:ogawa@teleport.com)", %%% revised by = "SR Nova Private Ltd." %%% copyright = "Copyright (C) 2003 American Astronomical Society %%% %%% This work may be distributed and/or modified under the %%% conditions of the LaTeX Project Public License, either version 1.3 %%% of this license or (at your option) any later version. %%% The latest version of this license is in %%% http://www.latex-project.org/lppl.txt %%% and version 1.3 or later is part of all distributions of LaTeX %%% version 2003/12/01 or later. %%% %%% This work has the LPPL maintenance status "maintained". %%% %%% The Current Maintainer of this work is the American Astronomical Society. %%% %%% This work consists of all files listed in the document README. %%% %%% address = "American Astronomical Society %%% USA", %%% telephone = "+1 ???", %%% FAX = "", %%% email = "aastex-help@aas.org", %%% codetable = "ISO/ASCII", %%% keywords = "latex, AAS, journal", %%% supported = "yes", %%% abstract = "formatter for AAS journal submissions", %%% docstring = "The checksum field above generated by ltxdoc", %%% } \NeedsTeXFormat{LaTeX2e}[1995/12/01]% \ProvidesClass{aastex}% [2005/06/22 5.2/AAS markup document class]% \def\substitute@option#1#2{% \ClassWarning{aastex}{% Substyle #1 is deprecated in aastex. Using #2 instead (please fix your document). }\@nameuse{ds@#2}% }% \ClassInfo{aastex}{% Original \protect\LaTeX2.09 style by Chris Biemesderfer (chris@seagoat.com). Adapted to \protect\LaTeXe\space by A. Ogawa (ogawa@teleport.com)% }% \newif\iflong@abstract \global\long@abstractfalse \DeclareOption{10pt}{\newcommand\aas@ptsize{0}}% \DeclareOption{11pt}{\newcommand\aas@ptsize{1}}% \DeclareOption{12pt}{\newcommand\aas@ptsize{2}}% \DeclareOption{landscape}{\OptionNotUsed}% \DeclareOption{eqsecnum}{\AtEndOfClass{\eqsecnum}} \DeclareOption{longabstract}{\global\long@abstracttrue} \DeclareOption{flushrt}{\let\opt@just\just@just}% \let\opt@just\@empty \def\just@just{% \@rightskip\z@skip \rightskip\@rightskip \pretolerance=100\relax }% \DeclareOption{tighten}{\def\opt@tighten{\tightenlines}}% \let\opt@tighten\@empty \DeclareOption{manuscript}{\def\aas@substyle{manuscript}\long@abstractfalse} \DeclareOption{preprint}{\def\aas@substyle{preprint}\long@abstractfalse} \DeclareOption{preprint2}{\def\aas@substyle{preprint2}\@twocolumntrue} \DeclareOption{aasms4}{\substitute@option{aasms4}{manuscript}}% \DeclareOption{aaspp4}{\substitute@option{aaspp4}{preprint}}% \DeclareOption{aas2pp4}{\substitute@option{aas2pp4}{preprint2}}% \DeclareOption{aj_pt4}{\substitute@option{aj_pt4}{preprint}}% \DeclareOption{apjpt4}{\substitute@option{apjpt4}{preprint}}% \def\aas@substyle{manuscript}% \AtEndOfPackage{% \@nameuse{aas@\aas@substyle}% }% \DeclareOption{astro}{\AtBeginDocument{\load@astro}}% \DeclareOption*{\PassOptionsToClass{\CurrentOption}{article}}% \ExecuteOptions{letterpaper,oneside,onecolumn,final}% \ProcessOptions\relax \@namedef{aas@size@manuscript}{% \def\aas@ptsize{2}% \pass@aassize }% \@namedef{aas@size@preprint}{% \ifx\undefined\aas@ptsize\expandafter\@firstoftwo\else\expandafter\@secondoftwo\fi {\def\aas@ptsize{1}}{}% \pass@aassize }% \@namedef{aas@size@preprint2}{% \ifx\undefined\aas@ptsize\expandafter\@firstoftwo\else\expandafter\@secondoftwo\fi {\def\aas@ptsize{0}}{}% \pass@aassize }% \def\pass@aassize{% \expandafter\PassOptionsToClass\expandafter{\expandafter1\aas@ptsize pt}{article}% }% \@nameuse{aas@size@\aas@substyle}% \LoadClass{article}[1995/12/01]% \RequirePackage{latexsym}% \RequirePackage{graphicx}% \RequirePackage{amssymb}% \RequirePackage{natbib}% \newcommand{\bibstyle@aas}{\bibpunct{(}{)}{;}{a}{}{,}} \@citestyle{aas} \RequirePackage{verbatim}% \def\@to{to}% \newcommand\ulap[1]{\vbox\@to\z@{{\vss#1}}}% \newcommand\dlap[1]{\vbox\@to\z@{{#1\vss}}}% \newcommand\let@environment[2]{% \expandafter\let \csname#1\expandafter\endcsname\csname#2\endcsname \expandafter\let \csname end#1\expandafter\endcsname\csname end#2\endcsname }% \newcommand\say[1]{\typeout{<\noexpand#1=\meaning#1>}}% \newcommand\saythe[1]{\typeout{<\noexpand#1=\the#1>}}% \newcommand\tracingplain{% \tracingonline\z@\tracingcommands\z@\tracingstats\z@ \tracingpages\z@\tracingoutput\z@\tracinglostchars\@ne \tracingmacros\z@\tracingparagraphs\z@\tracingrestores\z@ \showboxbreadth5\showboxdepth3\relax %\errorstopmode }% \newcommand\traceoutput{% \appdef\@resetactivechars{\showoutput}% }% \newcommand\nohyphenation{\kern\z@}% \newcommand\offhyphenation{% \lefthyphenmin\maxdimen\emergencystretch8\p@ }% \def\substitute@command#1#2{% \ClassWarning{aastex}{% Command \protect#1\space is deprecated in aastex. Using \protect#2\space instead (please fix your document). }% #2% }% \def\remove@command#1{% \ClassWarning{aastex}{% Command \protect#1\space is deprecated in aastex. Please remove it from your document% }% }% \def\@provide#1{%Implicit #2 \@ifxundefined#1{\def#1}{\def\@tempa}% }% \def\prepdef#1#2{% \@ifxundefined#1{\toks@{}}{\toks@\expandafter{#1}}% \toks@ii{#2}% \edef#1{\the\toks@ii\the\toks@}% }% \def\appdef#1#2{% \@ifxundefined#1{\toks@{}}{\toks@\expandafter{#1}}% \toks@ii{#2}% \edef#1{\the\toks@\the\toks@ii}% }% \def\appgdef#1#2{% \@ifxundefined#1{\toks@{}}{\toks@\expandafter{#1}}% \toks@ii{#2}% \xdef#1{\the\toks@\the\toks@ii}% }% \toksdef\toks@ii=\tw@ \long\def\@ifxundefined#1{\@ifx{\undefined#1}}% \def\@boolean#1#2{% \long\def#1{% #2% \if \expandafter\boolean@true \else \expandafter\boolean@false \fi }% }% \def\@boole@def#1#{\@boolean{#1}}% Implicit #2 \@boole@def\@ifx#1{\ifx#1}% \@boole@def\@ifx@empty#1{\ifx\@empty#1}% \@boole@def\@ifnum#1{\ifnum#1}% \@boole@def\@ifdim#1{\ifdim#1}% \@boole@def\@ifvoid#1{\ifvoid#1}% \long\def\boolean@true#1#2{#1}% \long\def\boolean@false#1#2{#2}% \renewcommand\addpenalty[1]{% \ifvmode \if@minipage \else \if@nobreak \else \ifinner \@tempskipa\lastskip \unskip \@tempcnta\lastpenalty \unpenalty \ifnum#1<\@tempcnta \penalty#1\relax \else \penalty\@tempcnta \fi \vskip\@tempskipa \else \ifdim\lastskip=\z@ \penalty#1\relax \else \@tempskipb\lastskip \vskip-\lastskip \penalty#1% \vskip\@tempskipb \fi \fi \fi \fi \else \@noitemerr \fi }% \renewcommand\addvspace[1]{% \ifvmode \if@minipage \else \ifinner \@tempskipa\lastskip \unskip \ifdim\@tempskipa=\z@ \vskip#1\relax \else \@tempskipb#1\relax \ifdim\@tempskipa<\@tempskipb \vskip\@tempskipb \else \ifdim\@tempskipb<\z@ \ifdim\@tempskipa<\z@ \vskip\@tempskipa \else \advance\@tempskipb\@tempskipa \vskip\@tempskipb \fi \else \vskip\@tempskipa \fi \fi \fi \else \ifdim\lastskip=\z@ \vskip#1\relax \else \@tempskipb#1\relax \@xaddvskip \fi \fi \fi \else \@noitemerr \fi }% \newcommand\maketitle@page{% \maketitle@disarm \begin{titlepage}% \let\footnotesize\small \let\footnoterule\relax \let \footnote \thanks \@maketitle \@thanks \vfil\null \end{titlepage}% \after@maketitle }% \newcommand\maketitle@runin{% \par \maketitle@disarm \begingroup %%%%\renewcommand\thefootnote{\@fnsymbol\c@footnote}% \def\@makefnmark{\rlap{\@textsuperscript{\normalfont\@thefnmark}}}% \long\def\@makefntext##1{% \parindent 1em\noindent \hb@xt@1.8em{% \hss\@textsuperscript{\normalfont\@thefnmark}% }% ##1% }% \if@twocolumn \@ifnum{\col@number=\@ne}{% \global\let\@title@footnote@text\@empty% \twocolumn[\let\@footnotetext\@title@footnotetext\@maketitle]% \@title@footnote@text% }{% \@maketitle }% \else \newpage \global\@topnum\z@ % Prevents figures from going at top of page. \@maketitle \fi %\thispagestyle{plain}% \@thanks \endgroup \after@maketitle }% \def\after@maketitle{% \iflong@abstract % \let\@makecol\@makecol@pptt \let\@outputdblcol\@outputdblcol@pptt \global\columnwidth\textwidth% \global\advance\columnwidth-\columnsep \global\divide\columnwidth\tw@ \global\hsize\columnwidth \global\linewidth\columnwidth \global\@twocolumntrue \global\@firstcolumntrue \col@number \tw@ \@ifnextchar [\@topnewpage\@floatplacement \begin{strip}% separate the abstract text from two-column text \end{strip} \fi %%%\setcounter{footnote}{0}% \global\let\thanks\@gobble \global\let\maketitle\relax \global\let\@maketitle\relax \global\let\@thanks\@empty \global\let\@author\@empty \global\let\@date\@empty \global\let\@title\@empty \global\let\title\relax \global\let\author\relax \global\let\date\relax \global\let\and\relax \global\let\email\@text@email \global\firsttabskip\z@ }% \AtEndOfClass{% \if@titlepage \let\maketitle\maketitle@page \else \let\maketitle\maketitle@runin \fi }% \def\open@footnotetext{% \insert\footins\bgroup % \egroup in \close@footnotetext \interlinepenalty\interfootnotelinepenalty \splittopskip\footnotesep \splitmaxdepth\dp\strutbox \floatingpenalty \@MM \reset@font\footnote@size \hsize\columnwidth \@parboxrestore }% \def\close@footnotetext#1{% \color@begingroup \@makefntext{% \rule\z@\footnotesep\ignorespaces #1\@finalstrut\strutbox }% \color@endgroup \egroup }% \def\@footnotetext{% Implict #1 \open@footnotetext \set@footnotetext{p@footnote}% }% \def\@mpfootnotetext{% Implict #1 \global\setbox\@mpfootins\vbox\bgroup % \egroup in \set@footnotetext \unvbox\@mpfootins \set@footnotetext{p@mpfootnote}% }% \long\def\set@footnotetext#1{%Implicit #2 \protected@edef\@currentlabel{% \csname #1\endcsname\@thefnmark }% \close@footnotetext }% \def\@title@footnotetext#1{% \protected@edef\@tempa{\csname p@footnote\endcsname\@thefnmark}% \expandafter\appgdef \expandafter\@title@footnote@text \expandafter{% \expandafter\insert@footnotetext \expandafter{\@tempa}{#1}}% }% \def\insert@footnotetext#1{%Implicit #2 \open@footnotetext \def\@thefnmark{#1}% \def\@currentlabel{#1}% \close@footnotetext }% \AtBeginDocument{% \ifx\footnote@size\undefined \let\footnote@size\footnotesize \fi }% \long\def\eqnarray@broken{% \stepcounter{equation}\def\@currentlabel{\p@equation\theequation}% \global\@eqnswtrue\m@th\global\@eqcnt\z@ \tabskip\mathindent \let\\=\@eqncr \setlength\abovedisplayskip{\topsep}% \ifvmode\addtolength\abovedisplayskip{\partopsep}\fi \addtolength\abovedisplayskip{\parskip}% \setlength\belowdisplayskip{\abovedisplayskip}% \setlength\belowdisplayshortskip{\abovedisplayskip}% \setlength\abovedisplayshortskip{\abovedisplayskip}% $$% \everycr{}% \halign to\linewidth\bgroup \hskip\@centering$\displaystyle\tabskip\z@skip{##}$\@eqnsel &\global\@eqcnt\@ne \hskip\tw@\arraycolsep \hfil${##}$\hfil &\global\@eqcnt\tw@ \hskip\tw@\arraycolsep $\displaystyle{##}$\hfil\tabskip\@centering &\global\@eqcnt\thr@@\hb@xt@\z@\bgroup\hss##\egroup \tabskip\z@skip \cr }% \long\def\eqnarray@fleqn@fixed{% \stepcounter{equation}\def\@currentlabel{\p@equation\theequation}% \global\@eqnswtrue\m@th\global\@eqcnt\z@ \tabskip\mathindent \let\\=\@eqncr \setlength\abovedisplayskip{\topsep}% \ifvmode\addtolength\abovedisplayskip{\partopsep}\fi \addtolength\abovedisplayskip{\parskip}% \setlength\belowdisplayskip{\abovedisplayskip}% \setlength\belowdisplayshortskip{\abovedisplayskip}% \setlength\abovedisplayshortskip{\abovedisplayskip}% $$% \everycr{}% \halign\@to\linewidth\bgroup \hskip\@centering$\displaystyle\tabskip\z@skip{##}$\@eqnsel &\global\@eqcnt\@ne \hskip\tw@\eqncolsep \hfil${{}##{}}$\hfil &\global\@eqcnt\tw@ \hskip\tw@\eqncolsep $\displaystyle{##}$\hfil\tabskip\@centering &\global\@eqcnt\thr@@\hb@xt@\z@\bgroup\hss##\egroup \tabskip\z@skip \cr }% \ifx\eqnarray\eqnarray@broken \ClassWarningNoLine{aastex}{Repairing broken {eqnarray} definition}% \let\eqnarray\eqnarray@fleqn@fixed \fi \let\eqnarray@broken\relax \let\eqnarray@fleqn@fixed\relax \def\@startsection#1#2#3#4#5#6{% \@startsection@hook \if@noskipsec \leavevmode \fi \par \@tempskipa #4\relax \@afterindenttrue \ifdim \@tempskipa <\z@ \@tempskipa -\@tempskipa \@afterindentfalse \fi \if@nobreak \everypar{}% \else \addpenalty\@secpenalty\addvspace\@tempskipa \fi \@ifstar {\@ssect{#3}{#4}{#5}{#6}}% {\@dblarg{\@sect{#1}{#2}{#3}{#4}{#5}{#6}}}% }% \def\@startsection@hook{}% \def\@sect#1#2#3#4#5#6[#7]#8{% \ifnum #2>\c@secnumdepth \let\@svsec\@empty \else \refstepcounter{#1}\protected@edef\@svsec{\@seccntformat{#1}\relax} \fi \@tempskipa #5\relax \ifdim \@tempskipa>\z@ \begingroup \section@centering#6{% \@hangfrom{\hskip #3\relax\@svsec}\interlinepenalty \@M\sec@upcase{#8}\@@par}% \endgroup \csname #1mark\endcsname{#7}\addcontentsline {toc}{#1}{\ifnum #2>\c@secnumdepth \else \protect\numberline{\csname the#1\endcsname}\fi #7}\else \def\@svsechd{% #6{\hskip#3\relax\@svsec \sec@upcase{#8}}% \csname #1mark\endcsname {#7}\addcontentsline{toc}{#1}{% \ifnum #2>\c@secnumdepth \else \protect\numberline{\csname the#1\endcsname}% \fi #7}}\fi \@xsect{#5}% }% \def\@ssect#1#2#3#4#5{\@tempskipa #3\relax \ifdim \@tempskipa>\z@ \begingroup \section@centering #4{% \@hangfrom{\hskip #1}\interlinepenalty \@M \sec@upcase{#5}\@@par}\endgroup \else \def\@svsechd{#4{\hskip #1\relax \sec@upcase{#5}}}\fi \@xsect{#3}}% \def\@seccntformat#1{\csname the#1\endcsname.\quad} \def\section@centering{\centering}% \def\sec@upcase#1{\relax{#1}}% \def\@citex[#1]#2{% \let\@citea\@empty \@cite{% \@for\@citeb:=#2\do{% \@citea \def\@citea{,\penalty\@m\ }% \edef\@citeb{\expandafter\@firstofone\@citeb\@empty}% \if@filesw\immediate\write\@auxout{\string\citation{\@citeb}}\fi \@ifundefined{b@\@citeb}{% \G@refundefinedtrue \@latex@warning{% Citation `\@citeb' on page \thepage \space undefined% }% }{% \csname b@\@citeb\endcsname }% }% }{#1}% }% \def\revtex@ver{5.2}% \def\revtex@date{12 Dec 2003}% \def\revtex@org{AAS}% \def\revtex@jnl{AAS}% \def\revtex@genre{manuscript}% \def\class@typeout{% \typeout{% \revtex@org\space \revtex@genre\space substyle, v\revtex@ver\space <\revtex@date>.% }% }% \def\class@typeout@jnl{% \typeout{% \revtex@org\space \revtex@jnl\space \revtex@genre\space substyle, v\revtex@ver\space <\revtex@date>.% }% }% \AtBeginDocument{% \class@typeout }% \def\revtex@pageid{% \xdef\@thefnmark{\null}% \@footnotetext{% This \revtex@genre\space was prepared with the \revtex@org\space \LaTeX\ macros v\revtex@ver.% }% }% \def\ps@plaintop{% \let\@mkboth\@gobbletwo \def\@oddfoot{}% \def\@oddhead{\rmfamily\hfil--\space\thepage\space--\hfil}% \def\@evenfoot{}% \let\@evenhead\@oddhead }% \def\ps@msstitle{% mss ID on title page \let\@mkboth\@gobbletwo \def\@oddfoot{}% \def\@oddhead{\rmfamily\hfil\ms@id}% \def\@evenfoot{}% \let\@evenhead\@oddhead }% \setlength\textwidth{6.5in}% \setlength\textheight{8.4in}% \setlength\headheight{.15in}% \setlength\marginparsep {10\p@}% \setlength\marginparpush{5\p@}% \setlength\oddsidemargin {0in}% \setlength\evensidemargin {0in}% \setlength\marginparwidth {0in}% \setlength\topmargin{0in}% \setlength\lineskip{1\p@}% \setlength\normallineskip{1\p@}% \def\@doubleleading{1.6}% \def\@tightleading{1.1}% \renewcommand\baselinestretch{\@tightleading}% \newcommand\tighten{\def\baselinestretch{\@tightleading}}% \newcommand\tightenlines{\tighten}% \newcommand\singlespace{% \def\baselinestretch{\@tightleading}% \normalsize }% \newcommand\doublespace{% \def\baselinestretch{\@doubleleading}% \normalsize }% \def\singlespace@apj{% \def\baselinestretch{\@tightleading}% \def\arraystretch{\@tightleading}% \normalsize }% \def\doublespace@apj{% \def\baselinestretch@apj{\@doubleleading}% \def\arraystretch{\@doubleleading}% \normalsize }% \setlength\parskip{1.5ex}% \setlength\parindent{2em}% \setlength\smallskipamount{3\p@\@plus1\p@\@minus1\p@}% \setlength\medskipamount{6\p@\@plus2\p@\@minus2\p@}% \setlength\bigskipamount{12\p@\@plus4\p@\@minus4\p@}% \@lowpenalty 51 \@medpenalty 151 \@highpenalty 301 \newcommand\ptlandscape{% \setlength\textwidth{9in}% \setlength\textheight{6.5in}% \setlength\pt@width{\textwidth}% \setlength\hoffset{0.0in}% \setlength\voffset{-0.25in}% }% \def\eqsecnum{% \@addtoreset{equation}{section}% \def\theequation{% %\mbox{\normalsize\arabic{section}-\arabic{equation}}% Wrong! \arabic{section}-\arabic{equation}% }% }% \def\@journalname{The Astrophysical Journal}% \def\cpr@holder{American Astronomical Society}% \newcommand\received[1]{\gdef\@recvdate{#1}}% \newcommand\accepted[1]{\gdef\@accptdate{#1}}% \newcommand\revised[1]{\gdef\@revisedate{#1}}% \newcommand\journalid[2]{\gdef\@jourvol{#1}\gdef\@jourdate{#2}}% \newcommand\articleid[2]{\gdef\@startpage{#1}\gdef\@finishpage{#2}}% \newcommand\paperid[1]{\gdef\@paperid{#1}}% \newcommand\ccc[1]{\gdef\CCC@code{#1}}% \AtEndOfClass{% \@provide\@recvdate{}% \@provide\@accptdate{}% \@provide\@revisedate{}% \@provide\@jourvol{}% \@provide\@jourdate{}% \@provide\@startpage{}% \@provide\@finishpage{}% \@provide\@paperid{MS-0001-SAMP}% \@provide\CCC@code{000-00\$75.95-CDB}% }% \newcommand\cpright[2]{% \global\expandafter\let\expandafter\cpr@type\csname cpr@#1\endcsname \gdef\cpr@year{#2}% \typeout{`#1' copyright \cpr@year.}% }% \def\cpr@AAS{Copyright \cpr@year\space by the \cpr@holder.}% \def\cpr@PD{This article is in the public domain.}% \def\cpr@Crown{Crown copyright \cpr@year\space by the \cpr@holder.}% \def\cpr@none{No copyright is claimed for this article.}% \def\cpr@ASP{Copyright \cpr@year\space by the ASP.}% \def\cpr@year{\number\year}% \def\@slug{% \par \noindent\cpr@type\par \noindent Manuscript number \@paperid.\par \noindent\CCC@code\par }% \newcommand\lefthead{\substitute@command\lefthead\shorttitle}% \newcommand\righthead{\substitute@command\righthead\shortauthors}% \newcommand\shorttitle[1]{\gdef\@versohead{#1}}% \newcommand\shortauthors[1]{\gdef\@rectohead{#1}}% \shorttitle{\relax}% \shortauthors{\relax}% \def\@runheads{% \@tempcnta\c@page \@whilenum\@tempcnta>\z@\do{% \vskip 3ex \hbox\@to30pc{% \small \expandafter\uppercase\expandafter{\@versohead}: \expandafter\uppercase\expandafter{\@rectohead}\hfil }% \advance\@tempcnta\m@ne }% }% \newcommand\msid[1]{\gdef\ms@id{#1}}% mss ID \def\ms@id{}% \newcommand\slugcomment[1]{\gdef\slug@comment{#1}}% \slugcomment{}% \newdimen\@slugcmmntwidth \long\def\@makeslugcmmnt@mss{% \@ifx@empty\slug@comment{\relax}{% \vskip 5ex \sbox\@tempboxa{\slug@comment}% \@ifdim{\wd\@tempboxa >\@slugcmmntwidth}{% \hbox\@to\textwidth{% \hss \parbox\@slugcmmntwidth\slug@comment }% }{% \hbox\@to\textwidth{\hfil\box\@tempboxa\hfil}% }% }% }% \long\def\@makeslugcmmnt@ppt{% \@ifx@empty\slug@comment{\relax}{% \sbox\@tempboxa{\slug@comment}% \@ifdim{\wd\@tempboxa >\@slugcmmntwidth}{% \hbox\@to\textwidth{% \hss \parbox\@slugcmmntwidth\slug@comment }% }{% \hbox\@to\textwidth{\hfil\box\@tempboxa}% }% \vskip 2ex }% }% \def\@rcvaccrule{\vrule\@width1.75in\@height0.5pt\@depth\z@}% \def\@dates{\ifx\@title\@empty\else {Received}\space% \ifx\@empty\@recvdate\@rcvaccrule\else\@recvdate\fi;% \hspace{1.5em}{accepted}\space% \ifx\@empty\@accptdate\@rcvaccrule\else\@accptdate\fi% \fi}% % \def\@dates@pptt{% \@ifx@empty\@recvdate{}{% \@ifx@empty\@accptdate{}{% {\center \@ifnum{\col@number=\tw@}{\small}{\normalsize}% {\itshape Received}\space \@recvdate \@ifnum{\col@number=\tw@}{\\[.5ex]}{\hspace{1.5em}}% {\itshape accepted}\space \@accptdate \endcenter }% }% }% }% \def\sluginfo@mss{% {% \addpenalty{\@M}% \addvspace{6\p@}% \centering \@dates \@makeslugcmmnt \par \addvspace{6\p@}% }% }% \newcommand\sluginfo{% {% \addpenalty{\@M}% \addvspace{6\p@}% \centering \@dates \par \addvspace{6\p@}% }% }% \let\dates=\sluginfo \renewenvironment{abstract}{% \iflong@abstract% Abstract in one-column mode \onecolumn \fi \global\setbox\abstract@box\vtop\bgroup \columnwidth\textwidth\hsize\columnwidth\linewidth\hsize \normalsize \color@begingroup \@parboxrestore \@setminipage \quotation }{% \par \endquotation \removelastskip \vskip-\prevdepth \color@endgroup \egroup }% \newbox\abstract@box \def\abstractname{ABSTRACT}% \def\@abstract@mss{% \sluginfo \clearpage \@ifvoid\abstract@box{}{% \begin{center}\bfseries\abstractname\end{center}% \contribute@box\abstract@box }% }% \def\contribute@box#1{% \dimen@\ht#1% \leavevmode\hbox{\vrule\@height\ht#1\@width\z@}\par \nointerlineskip\nobreak\kern-\ht#1\unvbox#1\prevdepth\z@ }% \def\@abstract@ppt{% \@ifvoid\abstract@box{}{% \begin{center}\bfseries\abstractname\end{center}% \contribute@box\abstract@box }% }% \def\@abstract@pptt{% \@ifvoid\abstract@box{}{% \@ifnum{\col@number=\tw@}{% \section*{Abstract}% }{% \vspace{3em}% \begin{center}% \large \bfseries\abstractname\vspace{-.5em}\vspace{\z@}% \end{center}% }% \contribute@box\abstract@box }% }% \def\title#1{\appdef\@title{\make@title{#1}}}% \def\author#1{\appdef\@author{\make@author{#1}}}% %%% \def\authoraddr{\substitute@command\authoraddr\affil}% \def\email#1{\appdef\@author{\make@authoremail{#1}}}% \def\affil#1{\appdef\@author{\make@affil{#1}}}% \def\altaffilmark#1{\appdef\@author{\make@altaffilmark{#1}}}% \def\altaffiltext#1#2{\appdef\@author{\make@altaffiltext{#1}{#2}}}% \def\and{\appdef\@author{\make@and}}% \let\authoraddr\@gobble \let\@title\@empty \let\@author\@empty \let\@date\@empty \def\@maketitle{% \newpage \begingroup \let\footnote\thanks \let\email\make@authoremail \let\affil\make@affil \let\altaffilmark\make@altaffilmark \let\altaffiltext\make@altaffiltext \let\and\make@and \@title \@author \@date \par \@abstract \@ifxundefined\keyword@list{}{% \expandafter\@keywords \expandafter{\keyword@list}% }% \endgroup }% \def\make@title@mss#1{% {% \def\baselinestretch{\@tightleading}% \center\large\bfseries{#1}\endcenter %% }% \thispagestyle{msstitle}% mss ID }% \def\make@title@ppt#1{% \@makeslugcmmnt {\center\large\bfseries{#1}\endcenter}% \thispagestyle{empty}% }% \def\make@title@pptt#1{% {% \center \@ifnum{\col@number=\tw@}{\large}{\Large}% \bfseries #1% \endcenter }% }% \def\make@author#1{% {\topsep\z@\center\normalsize#1\endcenter}% }% \def\make@author@pptt#1{% {\topsep\z@ \center \@ifnum{\col@number=\tw@}{\normalsize}{\vspace{4ex}\large}% #1% \endcenter }% }% \let\make@authoraddr=\@gobble \def\make@authoremail#1{% {\topsep\z@\center\normalsize\tt#1\endcenter}% }% \newcommand\make@affil[1]{% \vspace*{-2.5ex}% {\topsep\z@\center#1\endcenter}% }% \def\make@affil@ppt#1{% \vspace*{-0.8ex}% {% \topsep\z@ \center \@ifnum{\col@number=\tw@}{\small}{\normalsize}% \itshape #1% \endcenter }% }% \def\make@affil@pptt#1{% \vspace*{-0.8ex}% {% \topsep\z@ \center \@ifnum{\col@number=\tw@}{\small}{\normalsize}% \itshape #1% \endcenter }% }% \def\thefootnote{\@arabic\c@footnote}% initial style \newcommand\make@altaffilmark[1]{$^{#1}$}% \newcommand\make@altaffiltext[2]{% \iflong@abstract% \footnotetext@ass[#1]{#2} \else \footnotetext@ass[#1]{\hsize\columnwidth #2} \fi }% %% \def\thanks#1{\footnotemark \protected@xdef\@thanks{\@thanks \iflong@abstract% \protect\footnotetext[\the\c@footnote]{\hsize18pc #1} \else \protect\footnotetext[\the\c@footnote]{#1} \fi }% } %% \def\footnotetext@ass{% \@ifnextchar [\@xfootnotenext@ass {%\protected@xdef\@thefnmark{\thempfn}% \@footnotetext}} \def\@xfootnotenext@ass[#1]{% \begingroup %\csname c@\@mpfn\endcsname #1\relax \unrestored@protected@xdef\@thefnmark{#1}% \endgroup \@footnotetext} \def\make@and{\vspace*{-0.5ex}{\topsep\z@\center and\endcenter}}% \newcommand\keywords{\appdef\keyword@list}% \let\keyword@list\undefined \def\@keywords#1{% \vspace*{-.7ex}% \@ifnum{\col@number=\tw@}{% \noindent {{\itshape\@keywordtext:\/}\space\@kwds{#1}}% }{% {% \quote {\itshape\@keywordtext:\/}\space \@kwds{#1}% \endquote }% }% }% \def\@keywords@pptt#1{% \vspace*{-.7ex}% \@ifnum{\col@number=\tw@}{% \noindent {% \small {\itshape\@keywordtext:\/}\space \@kwds{#1}% }% }{% {% \quote \small {\itshape\@keywordtext:\/}\space \@kwds{#1}% \endquote }% }% }% \def\@keywords@mss#1{%%% \vspace*{-.7ex}% \@ifnum{\col@number=\tw@}{% \noindent {% \small {\itshape\@keywordtext:\/}\space \@kwds{#1}% }% }{% {% \quote \small {\itshape\@keywordtext:\/}\space \@kwds{#1}% \endquote% \clearpage }% }% }% \let\subjectheadings=\keywords \def\@keywordtext{Subject headings}% \def\@keyworddelim{---}% \def\@kwds@jnl#1{% \def\@kwddlm{}% \@for\@kwd:=#1\do{% \@kwddlm \def\@kwddlm{\space\@keyworddelim\penalty\@m\space}% {\@kwd}% }% }% \def\@kwds#1{#1\relax}% \AtBeginDocument{% \everypar{% \everypar@hook }% }% \def\everypar@hook{% \setbox\z@\lastbox\par\removelastskip \everypar{}% \maketitle@trigger \leavevmode }% \def\@startsection@hook{\maketitle@trigger}% \prepdef\tableofcontents{\listof@hook}% \prepdef\listoffigures{\listof@hook}% \prepdef\listoftables{\listof@hook}% \def\listof@hook{\maketitle@trigger}% \def\maketitle@disarm{% \global\let\maketitle@trigger\relax \global\let\@startsection@hook\@empty \global\let\listof@hook\@empty \global\let\everypar@hook\@empty }% \def\maketitle@trigger{% \maketitle }% \setlength{\skip\footins}{4ex\@plus1ex\@minus.5ex}% \setlength\footnotesep{3ex}% \long\def\@makefntext@pptt#1{% \noindent \hbox\@to\z@{\hss$^{\@thefnmark}$}% #1% }% \newcounter{editornote}% \def\theeditornote{{\rmfamily E}\arabic{editornote}}% \newcommand\notetoeditor[1]{% \stepcounter{editornote}% \begingroup \def\protect{\noexpand\protect\noexpand}% \xdef\@thefnmark{\theeditornote}% \endgroup \@footnotemark\@footnotetext{NOTE TO EDITOR: #1}% }% \renewcommand\section{% \@startsection{section}{1}% {\z@}{5ex\@plus.5ex}{1ex\@plus.2ex}{\normalsize\bfseries}% }% \def\thesection{\@arabic{\c@section}}% \def\clear@section@page{}% \renewcommand\subsection{% \@startsection{subsection}{2}% {\z@}{5ex\@plus.5ex}{1ex\@plus.2ex}{\normalsize\bfseries}% }% \def\thesubsection{\thesection.\@arabic{\c@subsection}}% \renewcommand\subsubsection{% \@startsection{subsubsection}{3}% {\z@}{5ex\@plus.5ex}{1ex\@plus.2ex}{\normalsize\itshape}% }% \def\thesubsubsection{\thesubsection.\@arabic{\c@subsubsection}}% \newcommand\subsubsubsection{% \@startsection{subsubsection}{4}% {\z@}{-15\p@\@plus-5\p@\@minus-2\p@}{5\p@}{\normalfont\normalsize\itshape}% }% \def\thesubsubsubsection{\thesubsubsection.\@arabic{\c@subsubsubsection}}% \def\theparagraph{\thesubsubsection.\@arabic{\c@paragraph}}% \newcommand\acknowledgments{\vskip 3ex\@plus.8ex\@minus.4ex}% \let\acknowledgements=\acknowledgments \renewcommand\appendix{% \par \if@twocolumn\@restonecoltrue\onecolumn\fi \setcounter{section}{\z@}% \setcounter{subsection}{\z@}% \setcounter{equation}{\z@}% \def\thesection{\Alph{section}}% \def\theequation{% %\hbox{\normalsize\Alph{section}\arabic{equation}}% \thesection\arabic{equation}% }% \@addtoreset{equation}{section}% \appendix@figtab@defs \def\section{% \@startsection {section}{1}{\z@}% {5ex\@plus.5ex}{1ex\@plus.2ex}{\normalsize\bfseries}% }% }% \let\appendix@figtab@defs\@empty \def\appendix@figtab@defs@pptt{}% \newcounter{cureqno}% \newenvironment{mathletters}{% \refstepcounter{equation}% \setcounter{cureqno}{\value{equation}}% \let\@curtheeqn\theequation \edef\@tempa{\theequation}% \expandafter\def \expandafter\theequation \expandafter{\@tempa\alph{equation}}% \setcounter{equation}{0}% }{% \let\theequation\@curtheeqn \setcounter{equation}{\value{cureqno}}% }% \newcommand\eqnum[1]{% \def\theequation{#1}% \let\@currentlabel\theequation \addtocounter{equation}{\m@ne}% }% \renewenvironment{thebibliography}[1]{% \clear@thebibliography@page \subsection*{REFERENCES}% \thebib@list \def\refpar{\relax}% \def\newblock{\hskip .11em\@plus.33em\@minus.07em}% \sloppy \clubpenalty4000 \widowpenalty4000 \sfcode`\.=1000\relax }{% \endlist \revtex@pageid }% \def\clear@thebibliography@page{}% \def\thebib@list{% \list{\null}{% \leftmargin 3em\labelwidth\z@\labelsep\z@\itemindent-\leftmargin \usecounter{enumi}% }% }% \def\thebib@list@pptt{% \list{\null}{% \leftmargin 1.2em\labelwidth\z@\labelsep\z@\itemindent-\leftmargin \usecounter{enumi}% }% }% \newenvironment{references}{% \clear@thebibliography@page \subsection*{REFERENCES}% \bgroup \setlength\parindent\z@ \setlength\parskip\itemsep \let\refpar\references@refpar }{% \refpar \egroup \revtex@pageid }% \def\references@refpar@mss{% \par\setlength\hangindent{3em}\hangafter\@ne }% \def\references@refpar@pptt{% \par\setlength\hangindent{1.2em}\hangafter\@ne }% \let\references@refpar\references@refpar@mss \newcommand\reference{% \@ifnextchar\bgroup{\@reference}{% \@latexerr{Missing key on reference command}{% Each reference command should have a key corresponding to a \protect\markcite\space somewhere in the text }% }% }% \def\@reference#1{\relax\refpar}% \newcommand\markcite[1]{\remove@command\markcite}% \def\@biblabel#1{\relax}% \def\@cite#1#2{#1\if@tempswa , #2\fi}% \setcounter{topnumber}{7}% \newskip\tnotemarkskip \tnotemarkskip7pt \newdimen\@abovenoteskip% \newcommand\tablenotemark[1]{% \rlap{$^{\mathrm #1}$}\hskip\tnotemarkskip\ignorespaces% Fixed: the space after notemark }% \def\@tablenotetext#1#2{% \vspace{.5ex}% {\noindent\llap{$^{#1}$}#2\par}% }% \def\@tablenotes#1{% \par \vspace{4.5ex}\footnoterule\vspace{.5ex}% {\footnotesize#1}% }% \def\@tablenotes@pptt#1{% \par \vspace{3.2ex}\footnoterule\vspace{.4ex}% {\footnotesize#1}% }% \AtBeginDocument{% \let\tblnote@list\@empty }% \newcommand\tablenotetext[2]{\ifdim\@abovenoteskip=0pt\global\@abovenoteskip=20pt\fi% \appgdef\tblnote@list{\hsize\pt@width\leftskip\z@\rightskip\z@% \@tablenotetext{#1}{\parfillskip\z@ plus1fil#2\endgraf}}% }% \def\spew@tblnotes{% \@ifx@empty\tblnote@list{}{% \@tablenotes{\tblnote@list}% \global\let\tblnote@list\@empty }% }% \prepdef\endtable{\spew@tblnotes}% \expandafter\prepdef\csname endtable*\endcsname{\spew@tblnotes}% \let\tableline=\hline \long\def\@makecaption#1#2{\vskip 2ex\noindent#1\ #2\par}% \newcommand\tablenum[1]{% \def\thetable{#1}% \let\@currentlabel\thetable \addtocounter{table}{\m@ne}% }% \newcommand\figurenum[1]{% \def\thefigure{#1}% \let\@currentlabel\thefigure \addtocounter{figure}{\m@ne}% }% \newcommand\placetable{\@place@float{TABLE}}% \newcommand\placefigure{\@place@float{FIGURE}}% \newcommand\placeplate{\@place@float{PLATE}}% \def\@place@float#1#2{% \vspace{0.5ex}% \begin{center}EDITOR: PLACE #1 \ref{#2} HERE.\end{center}% \vspace{0.5ex}% }% \newcommand\figcaption{\@testopt{\@xfigcaption}{}}% \def\@xfigcaption[#1]#2{{\def\@captype{figure}\caption{#2}}}% \newcommand\dummytable{\refstepcounter{table}}% \newbox\pt@box \newdimen\pt@width \newcount\pt@line \newcount\pt@column \newcount\pt@nlines \newcount\pt@ncol \newcount\pt@page \newcommand\colhead[1]{\multicolumn{1}{c}{#1}\pt@addcol}% \gdef\pt@footnotesize{\string\footnotesize} \gdef\pt@scriptsize{\string\scriptsize} \newcommand\tabletypesize[1]{\def\pt@typesize{#1}\gdef\@typesize{\string#1} \ifx\@typesize\pt@footnotesize \def\pt@headfrac{\pt@headfrac@ass@footnotesize} \else \ifx\@typesize\pt@scriptsize \def\pt@headfrac{\pt@headfrac@ass@scriptsize} \else \def\pt@headfrac{\pt@headfrac@ass@normalsize}% \fi \fi }% Access to different type sizes in deluxetable \def\pt@typesize{}% \newcommand\tablecolumns[1]{% \pt@column=#1\relax% \pt@ncol=#1\relax% \global\let\pt@addcol\@empty% }% \newcommand\tablecaption[1]{\gdef\pt@caption{\tnotemarkskip8pt#1}}%Fixed: space after mark \newcommand\tablehead[1]{% \gdef\pt@head{% \hline\hline \relax\\[-1.7ex]% #1\hskip\tabcolsep \\[.7ex]% \hline \relax\\[-1.5ex]% }% }% \def\tablehead@aj#1{% \gdef\pt@head{% #1\hskip\tabcolsep \\[.7ex]% \hline \relax\\[-1.5ex]% }% }% \newif\if@pt@rot \newcommand\rotate{\@pt@rottrue}% \newcommand\tabletail[1]{\gdef\pt@tail{#1}}% \newcommand\tablewidth[1]{\pt@width=#1\relax}% \newcommand\tableheadfrac[1]{\gdef\pt@headfrac{#1}}% \AtBeginDocument{% \let\pt@caption\@empty% \let\pt@head\@empty% \let\pt@tail\@empty% \pt@width\textwidth% %\def\pt@headfrac{.1}% \def\pt@headfrac{\pt@headfrac@ass@normalsize}% initialize typesize to consider }% % while calculating rows \newdimen\tabbaseskip% \def\pt@calcnlines{% \begingroup% \if@pt@rot\textheight\textwidth\fi% rotate tables \pt@typesize% Type sizes in deluxetable \@tempdima\pt@headfrac\textheight \@tempdimb\textheight\advance\@tempdimb by -\@tempdima \@tempdima\arraystretch\baselineskip \global\tabbaseskip\baselineskip \divide\@tempdimb by\@tempdima \global\pt@nlines\@tempdimb \endgroup }% \def\pt@tabacol{% \edef\@preamble{\@preamble\hskip\tabcolsep\tabskip\fill}% }% \newdimen\pt@tmpcapwidth \long\def\@makecaption@plano#1#2{% \@ifdim{\pt@width>\z@}{% \pt@tmpcapwidth\pt@width }{% \pt@tmpcapwidth\hsize }% \parbox{\pt@tmpcapwidth}{% \@make@caption@text{#1}{#2}% }% \endcenter }% \def\fnum@ptable{Table \thetable}% \def\fnum@ptablecont{Table \thetable---{\rmfamily Continued}}% \long\def\@make@caption@text#1#2{% \center\rmfamily#1.\quad#2\endcenter }% \long\def\@makecaption@plano@cont#1#2{% \center\rmfamily#1\endcenter \vskip 2.5ex }% \def\fnum@ptablecont@pptt{Table \thetable---{\itshape Continued}}% \long\def\@make@caption@text@pptt#1#2{% \center\sc#1\\[.5ex]#2\endcenter }% \long\def\@makecaption@plano@cont@pptt#1#2{% \center\sc#1\endcenter \vskip 1.5ex }% \def\fnum@ptable@apj{TABLE \thetable}% \def\fnum@ptablecont@apj{TABLE \thetable---{\itshape Continued}}% \long\def\@make@caption@text@apj#1#2{% \center\Large\sc#1\\[.5ex]#2\endcenter }% \long\def\@makecaption@plano@cont@apj#1#2{% \center\Large\sc#1\endcenter \vskip 1.5ex }% \def\fnum@ptable@aj{Table \thetable.}% \def\fnum@ptablecont@aj{Table \thetable.\space{\rmfamily (continued)}}% \long\def\@make@caption@text@aj#1#2{% \center\large{\sc#1}\space#2\endcenter }% \long\def\@makecaption@plano@cont@aj#1#2{% \center\large{\sc#1}\endcenter \vskip 1.5ex }% \newbox\spew@tblnotesbox% \newbox\restof@tblnotesbox% \global\newdimen\noteheight% \global\newdimen\pt@tabnoteminht% \global\pt@tabnoteminht=0pt% \newenvironment{deluxetable}[1]{% \maketitle \def\pt@format{\string#1}% \let\@acol\pt@tabacol% \let\@tabularcr\@ptabularcr% \let\@tablenotetext\@ptablenotetext% \let\@tablenotes\@ptablenotes% \global\pt@ncol\z@% \global\pt@column\z@% \global\pt@page\@ne% \gdef\pt@addcol{\global\advance\pt@ncol\@ne}% \if@pt@rot\leavevmode\fi% }{% \ifx\@typesize\pt@footnotesize%%% considering the table typesize in calculation \global\pt@tabnoteminht=\pt@notemin@footnote\baselineskip \else \ifx\@typesize\pt@scriptsize \global\pt@tabnoteminht=\pt@notemin@script\baselineskip \else \global\pt@tabnoteminht=\pt@notemin@normal\baselineskip \fi \fi \global\advance\pt@tabnoteminht-\@abovenoteskip \global\@abovenoteskip=0pt \setbox\spew@tblnotesbox\vbox{\spew@tblnotes}% %% %% Finding the available space for tablenotes in current page \if@pt@rot\global\noteheight\textwidth\else\global\noteheight\textheight\fi% \global\advance\noteheight-\ht\captionbox% \global\advance\noteheight-\pt@line\tabbaseskip \if@twocolumn %% tables in preprint2 style \ifx\@typesize\pt@scriptsize \global\advance\noteheight-6\baselineskip% \else \global\advance\noteheight-3\baselineskip% \fi \else \global\advance\noteheight-2\baselineskip% \fi %% %% Print the maximum lines of notes below table within current page \ifdim\noteheight<\pt@tabnoteminht% if not possible to keep the minimum two lines \global\noteheight=0pt% % the whole notes move to next page. \global\setbox\restof@tblnotesbox\vbox{\unvbox\spew@tblnotesbox}% \else %% %% if possible two lines, check the length of notes \ifdim\ht\spew@tblnotesbox>\noteheight% % Print maximum notes in available space and store the remaining part \hbox\@to\hsize{\hfil\vsplit\spew@tblnotesbox to \noteheight\hfil}% \global\setbox\restof@tblnotesbox\vbox{\unvbox\spew@tblnotesbox}% \else% % Print the whole notes in current page. \vbox{\hbox\@to\hsize{\hfil\box\spew@tblnotesbox\hfil}}% \fi \fi \typeout@deluxetable% \endcenter% \end@plano@float% %% %% Print the remaining tablenotes into new page(s). %% print each page until the remaining box empty. \loop\ifvoid\restof@tblnotesbox\else% \clearpage %% %% check whether the remaining box is a full/partial page \ifdim\ht\restof@tblnotesbox<\if@pt@rot\hsize\else\vsize\fi% \vbox to \textheight{\if@pt@rot\vfill\fi\hbox to \textwidth{\if@pt@rot\else\hfil\fi \if@pt@rot\rotatebox{90}{\box\restof@tblnotesbox} \else{\box\restof@tblnotesbox}\fi\hfil}\vfill}% \else% \vbox to \textheight{\vfill\hbox to \textwidth{\hfil% \if@pt@rot\rotatebox{90}{\vsplit\restof@tblnotesbox to \textwidth} \else{\vsplit\restof@tblnotesbox to \textheight}\fi\hfil}\vfill}% \fi% \clearpage \repeat% \addtocounter{table}{\m@ne}% \tabletypesize{\normalsize}% }% \let@environment{planotable}{deluxetable}% \def\@plano@float{% Invoked by \startdata \begingroup% \if@pt@rot\columnwidth\textheight\fi% Deluxetable table \rotate \@plano@float@{table}% }% \def\end@plano@float{% S/B invoked by \enddata; instead by \enddeluxetable \end@plano@float@\endgroup}% \def\@plano@float@{\@float}% Extra layer of abstraction for float processing \def\end@plano@float@{% \end@float}% \newdimen\firsttabskip \firsttabskip-\hsize \appdef\@endfloatbox{% \if@pt@rot \global\setbox\@currbox\vbox{\hskip\firsttabskip\global\firsttabskip\z@% \rotatebox{90}{\box\@currbox}}\else\global\firsttabskip\z@\fi% }% \def\typeout@deluxetable@mss{% \typeout{% Table \thetable\space has been set to width \the\pt@width }% }% \def\typeout@deluxetable@ppt{% \typeout{% Page \the\pt@page \space of table \thetable\space has been set to width \the\pt@width\space with \the\pt@nlines\space lines per page }% }% \let\typeout@deluxetable\typeout@deluxetable@mss \newcommand\startdata{% \pt@calcnlines \@ifdim{\pt@width>\z@}{% \def\@halignto{\@to\pt@width}% }{% \def\@halignto{}% }% \let\fnum@table=\fnum@ptable \let\@makecaption\@makecaption@plano \global\pt@line\z@ \start@pt@tabular \after@startdata }% \global\newbox\captionbox \def\start@pt@tabular{\par% \@plano@float \center \expandafter\caption\expandafter{\pt@caption}% \global\setbox\captionbox\vbox{\expandafter\caption\expandafter{\pt@caption}} \pt@typesize% Type sizes in deluxetable \expandafter\@tabular\expandafter{\pt@format}% }% \def\set@pt@box#1{\setbox\pt@box}% \def\after@startdata{\pt@head}% \def\after@startdata@aj{\hline\hline\relax\\[-1.7ex]\pt@head}% \def\enddata{% \crcr \noalign{\vskip .7ex}% \before@enddata% \endtabular% \setbox\pt@box\lastbox% \pt@width\wd\pt@box \hbox \@to \hsize{\hfil\box\pt@box\hfil}% \ignorespaces}% \def\before@enddata{\hline}% \def\before@enddata@aj{\hline\hline}% \def\nl{\substitute@command\nl\\}% \def\nextline{\substitute@command\nextline\\}% \def\@ptabularcr{% {\ifnum0=`}\fi% A klootch just in case the next token is & or \cr \@ifstar{% \@testopt{\@argptabularcr\@empty}\z@skip% }{% \@testopt{\@argptabularcr\ptable@@split}\z@skip% }% }% \newdimen\pt@reduceline \newdimen\extra@vspace \extra@vspace\z@ \def\@xargptarraycr#1{\@tempdima #1% \global\advance\extra@vspace\@tempdima% % adding the optional spaces \advance\@tempdima\dp \@arstrutbox% \vrule \@height\z@ \@depth\@tempdima \@width\z@% \global\pt@reduceline\arraystretch\tabbaseskip% total lines to be reduced \@whilenum\pt@reduceline<\extra@vspace% % reducing the excess lines% \do{% \global\advance\extra@vspace-\pt@reduceline% \global\advance\pt@line1 }% \cr}% \def\@argptabularcr#1[#2]{% \ifnum0=`{\fi}% To undo the effect of the klootch. \@ifdim{#2>\z@}{% \unskip\@xargptarraycr{#2}% }{% \@yargarraycr{#2}% }\ptable@split#1% }% \def\ptable@split#1{% \noalign{% \global\advance\pt@line\@ne% \@ifnum{\pt@line<\pt@nlines}{}{% \aftergroup#1% }% }% }% \def\ptable@@split{% \before@suspendpt% \endtabular% \setbox\pt@box\lastbox% \pt@width\wd\pt@box\box\pt@box% \typeout@pt@nl% \global\advance\pt@page\@ne% \endcenter% \end@plano@float% \clearpage \global\extra@vspace\z@ \addtocounter{table}{-2}% \let\fnum@table=\fnum@ptablecont% \let\@makecaption\@makecaption@plano@cont% \global\pt@ncol=\pt@column% Either 0 or value of \tablecolumns \global\pt@line\z@% \start@pt@tabular% \before@resumept% \pt@head% }% \def\before@suspendpt{}% \def\before@resumept{}% \def\before@suspendpt@aj{\@tabularcr\noalign{\vskip .7ex}\hline}% \def\before@resumept@aj{\hline\relax\@tabularcr[-1.7ex]}% \def\typeout@pt@nl@ppt{% \typeout{% Page \the\pt@page\space of table \thetable\space has been set to width \the\pt@width }% }% \def\typeout@pt@nl@mss{% \typeout{% Page \the\pt@page\space of table \thetable\space has been set to width \the\pt@width\space with \the\pt@nlines\space lines per page }% }% \def\typeout@pt@nl@aj{% \typeout{% Table \thetable\space has been set to width \the\pt@width\space with \the\pt@nlines\space lines per page }% }% \let\typeout@pt@nl\typeout@pt@nl@mss \newcommand\tablevspace[1]{\substitute@command\tablevspace\\[#1]}% \newcommand\tablebreak{\cr\ptable@@split}%\\{\cr\ptable@@split}% \newcommand\cutinhead[1]{% \noalign{\vskip 1.5ex}% \hline \@ptabularcr \noalign{\vskip -4ex}% \multicolumn{\pt@ncol}{c}{#1}% \@ptabularcr \noalign{\vskip .8ex}% \hline \@ptabularcr \noalign{\vskip -2ex}% }% \def\cutinhead@ppt#1{% \noalign{\vskip 1.5ex}% \hline \@ptabularcr \noalign{\vskip -2ex}% Style Note: in apj, it is -1.5ex \multicolumn{\pt@ncol}{c}{#1}% \@ptabularcr \noalign{\vskip .8ex}% \hline \@ptabularcr \noalign{\vskip -2ex}% }% \newcommand\sidehead[1]{% \noalign{\vskip 1.5ex}% \multicolumn{\pt@ncol}{@{\hskip\z@}l}{#1}% \@ptabularcr \noalign{\vskip .5ex}% }% \def\@ptablenotetext#1#2{% \vspace{0ex}% Style Note: in ppt, it is gone {%\parbox{\pt@width}% {\hskip1em$^{\mathrm#1}$#2}\par}% }% \def\@ptablenotes#1{% \par \vspace{2ex}% {\setlength\parskip{1.5ex}#1}% }% \def\@ptablenotes@apj#1{% \par \vspace{2ex}% {#1}% }% \newcommand\tablerefs[1]{\ifdim\@abovenoteskip=0pt\global\@abovenoteskip=10pt\fi \appgdef\tblnote@list{\hsize\pt@width\leftskip\z@\rightskip\z@% \@tableref{\parfillskip\z@ plus1fil#1\endgraf}}}% \def\@tableref#1{% \par \vspace*{3ex}% {%\parbox{\pt@width} %%%% {\hskip1em\rmfamily References. --- #1}\par}% }% \newcommand\tablecomments[1]{\ifdim\@abovenoteskip=0pt\global\@abovenoteskip=10pt\fi \appgdef\tblnote@list{\hsize\pt@width\leftskip\z@\rightskip\z@% \@tablecom{\parfillskip\z@ plus1fil#1\endgraf}}}% \def\@tablecom#1{% \par \vspace*{3ex}% {%\parbox{\pt@width} %%% {\hskip1em\rmfamily Note. --- #1}\par}% }% \def\@tableref@pptt#1{% \par \vspace*{3ex}% {%\parbox{\pt@width} %%% {\hskip1em{\sc References.---}#1}\par}% }% \def\@tablecom@pptt#1{% \vspace*{3ex}{% %\parbox{\pt@width} %%% {\hskip1em{\sc Note.---}#1}\par}% }% \newcounter{plate}% \def\ftype@plate{4}% \def\ext@plate{lof}% \newenvironment{plate}{\@float{plate}}{\end@float}% \newenvironment{plate*}{\@dblfloat{plate}}{\end@dblfloat}% \let\platewidth=\tablewidth \newcommand\platenum[1]{% \def\theplate{#1}% \let\@currentlabel\theplate \addtocounter{plate}{\m@ne}% }% \def\thefigure{\@arabic\c@figure}% \def\thetable{\@arabic\c@table}% \def\theplate{\@arabic\c@plate}% \def\fnum@figure{{\rmfamily Fig.\space\thefigure.---}}% \def\fnum@table{{\rmfamily Table \thetable:}}% \def\fnum@plate{{\bfseries Plate \theplate.}}% \def\fps@figure{bp}% \def\fps@table{bp}% \def\fps@plate{bp}% \def\eps@scaling{1.0}% \newcommand\epsscale[1]{\gdef\eps@scaling{#1}}% \newcommand\plotone[1]{% \typeout{Plotone included the file #1} \centering \leavevmode \includegraphics[width={\eps@scaling\columnwidth}]{#1}% }% \newcommand\plottwo[2]{{% \typeout{Plottwo included the files #1 #2} \centering \leavevmode \columnwidth=.45\columnwidth \includegraphics[width={\eps@scaling\columnwidth}]{#1}% \hfil \includegraphics[width={\eps@scaling\columnwidth}]{#2}% }}% \def\plotfiddle#1#2#3#4#5#6#7{{ \typeout{Plotfiddle included the file #1} \centering\leavevmode%% Re-implement from v4.0 \vbox to #2{\rule{0pt}{#2}} \hspace*{#6pt}\includegraphics[width=#4pt, height=#5pt, angle=#3, origin=c]{#1}}% } \let\jnl@style=\rmfamily \def\ref@jnl#1{{\jnl@style#1}}% \newcommand\aj{\ref@jnl{AJ}}% % Astronomical Journal \newcommand\actaa{\ref@jnl{Acta Astron.}}% % Acta Astronomica \newcommand\araa{\ref@jnl{ARA\&A}}% % Annual Review of Astron and Astrophys \newcommand\apj{\ref@jnl{ApJ}}% % Astrophysical Journal \newcommand\apjl{\ref@jnl{ApJ}}% % Astrophysical Journal, Letters \newcommand\apjs{\ref@jnl{ApJS}}% % Astrophysical Journal, Supplement \newcommand\ao{\ref@jnl{Appl.~Opt.}}% % Applied Optics \newcommand\apss{\ref@jnl{Ap\&SS}}% % Astrophysics and Space Science \newcommand\aap{\ref@jnl{A\&A}}% % Astronomy and Astrophysics \newcommand\aapr{\ref@jnl{A\&A~Rev.}}% % Astronomy and Astrophysics Reviews \newcommand\aaps{\ref@jnl{A\&AS}}% % Astronomy and Astrophysics, Supplement \newcommand\azh{\ref@jnl{AZh}}% % Astronomicheskii Zhurnal \newcommand\baas{\ref@jnl{BAAS}}% % Bulletin of the AAS \newcommand\caa{\ref@jnl{Chinese Astron. Astrophys.}}% % Chinese Astronomy and Astrophysics \newcommand\cjaa{\ref@jnl{Chinese J. Astron. Astrophys.}}% % Chinese Journal of Astronomy and Astrophysics \newcommand\icarus{\ref@jnl{Icarus}}% % Icarus \newcommand\jcap{\ref@jnl{J. Cosmology Astropart. Phys.}}% % Journal of Cosmology and Astroparticle Physics \newcommand\jrasc{\ref@jnl{JRASC}}% % Journal of the RAS of Canada \newcommand\memras{\ref@jnl{MmRAS}}% % Memoirs of the RAS \newcommand\mnras{\ref@jnl{MNRAS}}% % Monthly Notices of the RAS \newcommand\na{\ref@jnl{New A}}% % New Astronomy \newcommand\nar{\ref@jnl{New A Rev.}}% % New Astronomy Review \newcommand\pra{\ref@jnl{Phys.~Rev.~A}}% % Physical Review A: General Physics \newcommand\prb{\ref@jnl{Phys.~Rev.~B}}% % Physical Review B: Solid State \newcommand\prc{\ref@jnl{Phys.~Rev.~C}}% % Physical Review C \newcommand\prd{\ref@jnl{Phys.~Rev.~D}}% % Physical Review D \newcommand\pre{\ref@jnl{Phys.~Rev.~E}}% % Physical Review E \newcommand\prl{\ref@jnl{Phys.~Rev.~Lett.}}% % Physical Review Letters \newcommand\pasa{\ref@jnl{PASA}}% % Publications of the Astron. Soc. of Australia \newcommand\pasp{\ref@jnl{PASP}}% % Publications of the ASP \newcommand\pasj{\ref@jnl{PASJ}}% % Publications of the ASJ \newcommand\qjras{\ref@jnl{QJRAS}}% % Quarterly Journal of the RAS \newcommand\rmxaa{\ref@jnl{Rev. Mexicana Astron. Astrofis.}}% % Revista Mexicana de Astronomia y Astrofisica \newcommand\skytel{\ref@jnl{S\&T}}% % Sky and Telescope \newcommand\solphys{\ref@jnl{Sol.~Phys.}}% % Solar Physics \newcommand\sovast{\ref@jnl{Soviet~Ast.}}% % Soviet Astronomy \newcommand\ssr{\ref@jnl{Space~Sci.~Rev.}}% % Space Science Reviews \newcommand\zap{\ref@jnl{ZAp}}% % Zeitschrift fuer Astrophysik \newcommand\nat{\ref@jnl{Nature}}% % Nature \newcommand\iaucirc{\ref@jnl{IAU~Circ.}}% % IAU Cirulars \newcommand\aplett{\ref@jnl{Astrophys.~Lett.}}% % Astrophysics Letters and Communications \newcommand\apspr{\ref@jnl{Astrophys.~Space~Phys.~Res.}}% % Astrophysics Space Physics Research \newcommand\bain{\ref@jnl{Bull.~Astron.~Inst.~Netherlands}}% % Bulletin Astronomical Institute of the Netherlands \newcommand\fcp{\ref@jnl{Fund.~Cosmic~Phys.}}% % Fundamental Cosmic Physics \newcommand\gca{\ref@jnl{Geochim.~Cosmochim.~Acta}}% % Geochimica Cosmochimica Acta \newcommand\grl{\ref@jnl{Geophys.~Res.~Lett.}}% % Geophysics Research Letters \newcommand\jcp{\ref@jnl{J.~Chem.~Phys.}}% % Journal of Chemical Physics \newcommand\jgr{\ref@jnl{J.~Geophys.~Res.}}% % Journal of Geophysical Research \newcommand\jqsrt{\ref@jnl{J.~Quant.~Spec.~Radiat.~Transf.}}% % Journal of Quantitiative Spectroscopy and Radiative Trasfer \newcommand\memsai{\ref@jnl{Mem.~Soc.~Astron.~Italiana}}% % Mem. Societa Astronomica Italiana \newcommand\nphysa{\ref@jnl{Nucl.~Phys.~A}}% % Nuclear Physics A \newcommand\physrep{\ref@jnl{Phys.~Rep.}}% % Physics Reports \newcommand\physscr{\ref@jnl{Phys.~Scr}}% % Physica Scripta \newcommand\planss{\ref@jnl{Planet.~Space~Sci.}}% % Planetary Space Science \newcommand\procspie{\ref@jnl{Proc.~SPIE}}% % Proceedings of the SPIE \let\astap=\aap \let\apjlett=\apjl \let\apjsupp=\apjs \let\applopt=\ao \newcommand\phn{\phantom{0}}% \newcommand\phd{\phantom{.}}% \newcommand\phs{\phantom{$-$}}% \newcommand\phm[1]{\phantom{#1}}% \let\la=\lesssim % For Springer A&A compliance... \let\ga=\gtrsim \newcommand\sq{\mbox{\rlap{$\sqcap$}$\sqcup$}}% \newcommand\arcdeg{\mbox{$^\circ$}}% \newcommand\arcmin{\mbox{$^\prime$}}% \newcommand\arcsec{\mbox{$^{\prime\prime}$}}% \newcommand\fd{\mbox{$.\!\!^{\mathrm d}$}}% \newcommand\fh{\mbox{$.\!\!^{\mathrm h}$}}% \newcommand\fm{\mbox{$.\!\!^{\mathrm m}$}}% \newcommand\fs{\mbox{$.\!\!^{\mathrm s}$}}% \newcommand\fdg{\mbox{$.\!\!^\circ$}}% \newcommand\farcm@mss{\mbox{$.\mkern-4mu^\prime$}}% \let\farcm\farcm@mss \newcommand\farcs@mss{\mbox{$.\!\!^{\prime\prime}$}}% \let\farcs\farcs@mss \newcommand\fp{\mbox{$.\!\!^{\scriptscriptstyle\mathrm p}$}}% \newcommand\micron{\mbox{$\mu$m}}% \def\farcm@apj{% \mbox{.\kern -0.7ex\raisebox{.9ex}{\scriptsize$\prime$}}% }% \def\farcs@apj{% \mbox{% \kern 0.13ex.% \kern -0.95ex\raisebox{.9ex}{\scriptsize$\prime\prime$}% \kern -0.1ex% }% }% \newcommand\case[2]{\mbox{$\frac{#1}{#2}$}}% \newcommand\slantfrac{\case}% \newcommand\onehalf{\slantfrac{1}{2}}% \newcommand\onethird{\slantfrac{1}{3}}% \newcommand\twothirds{\slantfrac{2}{3}}% \newcommand\onequarter{\slantfrac{1}{4}}% \newcommand\threequarters{\slantfrac{3}{4}}% \newcommand\ubvr{\mbox{$U\!BV\!R$}}%% UBVR system \newcommand\ub{\mbox{$U\!-\!B$}}% % U-B \newcommand\bv{\mbox{$B\!-\!V$}}% % B-V \newcommand\vr{\mbox{$V\!-\!R$}}% % V-R \newcommand\ur{\mbox{$U\!-\!R$}}% % U-R \newcommand\ion[2]{#1$\;${\small\rmfamily\@Roman{#2}}\relax}% \newcommand\nodata{ ~$\cdots$~ }% \newcommand\diameter{\ooalign{\hfil/\hfil\crcr\mathhexbox20D}}% \newcommand\degr{\arcdeg}% \newcommand\Sun{\sun}% Sun symbol, "S" \newcommand\Sol{\sun}% \newcommand\sun{\odot}% \newcommand\Mercury{\astro{\char1}}% Mercury symbol, "1" \newcommand\Venus{\astro{\char2}}% Venus symbol, "2" \newcommand\Earth{\earth}% Earth symbol, "3" \newcommand\Terra{\earth}% \newcommand\earth{\oplus}% \newcommand\Mars{\astro{\char4}}% Mars symbol, "4" \newcommand\Jupiter{\astro{\char5}}% Jupiter symbol, "5" \newcommand\Saturn{\astro{\char6}}% Saturn symbol, "6" \newcommand\Uranus{\astro{\char7}}% Uranus symbol, "7" \newcommand\Neptune{\astro{\char8}}% Neptune symbol, "8" \newcommand\Pluto{\astro{\char9}}% Pluo symbol, "9" \newcommand\Moon{\astro{\char10}}% Moon symbol, "M" \newcommand\Luna{\Moon}% \newcommand\Aries{\astro{\char11}}% \newcommand\VEq{\Aries}% vernal equinox (Aries) \newcommand\Taurus{\astro{\char12}}% \newcommand\Gemini{\astro{\char13}}% \newcommand\Cancer{\astro{\char14}}% \newcommand\Leo{\astro{\char15}}% \newcommand\Virgo{\astro{\char16}}% \newcommand\Libra{\astro{\char17}}% \newcommand\AEq{\Libra}% autumnal equinox (Libra) \newcommand\Scorpius{\astro{\char18}}% \newcommand\Sagittarius{\astro{\char19}}% \newcommand\Capricornus{\astro{\char20}}% \newcommand\Aquarius{\astro{\char21}}% \newcommand\Pisces{\astro{\char22}}% \def\load@astro{% \dimen@=1\aas@ptsize\p@ \font\astro@font=Astrosym at\dimen@ }% \def\astro#1{\leavevmode\hbox{\astro@font#1}}% \def\astro@font{% \ClassWarning{aastex}{% Please use class option `astro', since you are using the astro font.% }% }% \newcommand\sbond{\chem@bnd{\@sbnd}}% \newcommand\dbond{\chem@bnd{\@dbnd}}% \newcommand\tbond{\chem@bnd{\@tbnd}}% \def\chem@bnd#1{% {% \kern.1em\relax \setbox\z@\hbox{M}% \dimen@ii.8em\relax \p@=.1em\relax \dimen@.5\ht\z@\dimen@i-\dimen@ \advance\dimen@1.5\p@\advance\dimen@i-1.0\p@ #1% \kern.1em\relax }% }% \def\@sbnd{% \advance\dimen@-1.5\p@\advance\dimen@i1.5\p@ \vrule\@height\dimen@\@depth\dimen@i\@width\dimen@ii\nobreak }% \def\@dbnd{% \advance\dimen@-0.5\p@\advance\dimen@i0.5\p@ \vrule\@height\dimen@\@depth\dimen@i\@width\dimen@ii\nobreak \advance\dimen@-1.5\p@\advance\dimen@i1.5\p@ \hskip-\dimen@ii \vrule\@height\dimen@\@depth\dimen@i\@width\dimen@ii\nobreak }% \def\@tbnd{% \vrule\@height\dimen@\@depth\dimen@i\@width\dimen@ii\nobreak \advance\dimen@-1.5\p@\advance\dimen@i1.5\p@ \hskip-\dimen@ii \vrule\@height\dimen@\@depth\dimen@i\@width\dimen@ii\nobreak \advance\dimen@-1.5\p@\advance\dimen@i1.5\p@ \hskip-\dimen@ii \vrule\@height\dimen@\@depth\dimen@i\@width\dimen@ii\nobreak }% \renewcommand\LaTeX{% \leavevmode L% \raise.42ex\hbox{% \count@=\the\fam $\fam\count@\scriptstyle\kern-.3em A$% }% \kern-.15em\TeX }% \newcommand\anchor[2]{#2}% \newcommand\url{\@dblarg\@url}% \def\@url[#1]{\anchor{#1}}% \def\@text@email#1{#1}% \def\authoremail{\substitute@command\authoremail\email}% \newcommand\objectname{\@testopt\@objectname{[}} \def\@objectname[#1]#2{#2}% \newcommand\object{\@testopt\@object{[}}% \def\@object[#1]#2{#2}% %% macro for facility \newcommand\facility{\@testopt\@facility{[}}% \def\@facility[#1]#2{#2}% %% macro for supportfrom \newcommand\supportfrom{\@testopt\@supportfrom{[}}% \def\@supportfrom[#1]#2{#2}% %% macro for dataset \newcommand\dataset{\@testopt\@dataset{[}}% \def\@dataset[#1]#2{#2}% \newcommand\sizrpt{% (\fontname\the\font): em=\the\fontdimen6\font, ex=\the\fontdimen5\font \typeout{% (\fontname\the\font): em=\the\fontdimen6\font, ex=\the\fontdimen5\font }% }% \def\aas@preprint{% \def\revtex@genre{preprint}% \let\ptlandscape\@empty \setlength\@slugcmmntwidth{.67\textwidth}% \let\@makeslugcmmnt\@makeslugcmmnt@ppt \let\@abstract\@abstract@ppt \let\make@title\make@title@ppt \let\make@affil\make@affil@ppt \let\notetoeditor\@gobble \let\clear@section@page\@empty \let\placetable\@gobble \let\placefigure\@gobble \let\placeplate\@gobble \let\typeout@deluxetable\typeout@deluxetable@ppt \let\typeout@pt@nl\typeout@pt@nl@mss \ps@plaintop \let\references@refpar\references@refpar@mss \let\cutinhead\cutinhead@ppt \def\pt@headfrac@ass@normalsize{.1} \def\pt@headfrac@ass@footnotesize{.12} \def\pt@headfrac@ass@scriptsize{.15} \def\pt@notemin@normal{4.5} \def\pt@notemin@footnote{4.5} \def\pt@notemin@script{5} }% \@namedef{aas@preprint2}{% \aas@preprint \def\revtex@genre{2-column preprint}% \ps@plain \@twocolumntrue \@rightskip=\z@\@plus4em \rightskip\@rightskip \opt@just \just@just % -SZ restored preprint2 to full justification \setlength\parindent{1.2em}% \setlength\parskip{0.5ex}% \setlength\columnsep{0.5in}% \setlength\hoffset{-0.2in}% \tolerance=600 \setlength\emergencystretch{6\p@}% \def\baselinestretch{1.0}% \def\@tightleading{1.0}% \let\singlespace\@empty \let\doublespace\@empty \let\@dates\@dates@pptt \let\@abstract\@abstract@pptt \let\make@title\make@title@pptt \let\make@author\make@author@pptt \let\make@affil\make@affil@pptt \let\@keywords\@keywords@pptt \setlength{\skip\footins}{3ex\@plus1ex\@minus.5ex}% \setlength\footnotesep{2ex}% \let\@makefntext\@makefntext@pptt \let\section\section@pptt \let\subsection\subsection@pptt \let\subsubsection\subsubsection@pptt \let\section@centering\@empty \let\appendix@figtab@defs\appendix@figtab@defs@pptt \def\clear@thebibliography@page{% \if@restonecol\if@twocolumn\else\twocolumn\fi\fi }% \let\references@refpar\references@refpar@pptt \let\thebib@list\thebib@list@pptt \let\@tablenotes\@tablenotes@pptt \let\fnum@ptablecont\fnum@ptablecont@pptt \let\@make@caption@text\@make@caption@text@pptt \let\@makecaption@plano@cont\@makecaption@plano@cont@pptt \let\cutinhead\cutinhead@ppt \def\@plano@float@{\@dblfloat}% Extra layer of abstraction for float processing \def\end@plano@float@{\end@dblfloat}% %\let\@tableref\@tableref@pptt \let\@tablecom\@tablecom@pptt \def\pt@headfrac@ass@normalsize{.12} \def\pt@headfrac@ass@footnotesize{.15} \def\pt@headfrac@ass@scriptsize{.18} \def\pt@notemin@normal{5} \def\pt@notemin@footnote{5} \def\pt@notemin@script{5} }% \def\section@pptt{% \@startsection{section}{1}% {\z@}{2.3ex\@plus1ex\@minus.2ex}% {1.5ex\@plus.2ex}{\normalsize\bfseries}% }% \def\subsection@pptt{% \@startsection{subsection}{2}% {\z@}{2ex\@plus1ex\@minus.2ex}{1ex\@plus.2ex}{\normalsize\bfseries}% }% \def\subsubsection@pptt{% \@startsection{subsubsection}{3}% {\z@}{2ex\@plus1ex\@minus.2ex}{1ex\@plus.2ex}{\normalsize\itshape}% }% \def\aas@manuscript{% \def\revtex@genre{manuscript}% \let\ptlandscape\@empty \def\baselinestretch{\@doubleleading}% \let\footnote@size\@empty \def\tighten{\def\baselinestretch{\@doubleleading}}% \def\singlespace{}% \def\doublespace{}% \opt@tighten \setlength\@slugcmmntwidth{\textwidth}% \let\@makeslugcmmnt\@makeslugcmmnt@mss \@rightskip=\z@\@plus4em \rightskip\@rightskip \opt@just \let\sluginfo\sluginfo@mss \let\@abstract\@abstract@mss \let\@keywords\@keywords@mss % pagebreak after keywords \let\make@title\make@title@mss \def\clear@section@page{\clearpage}% \def\clear@thebibliography@page{\clearpage}% \let\typeout@deluxetable\typeout@deluxetable@mss \let\typeout@pt@nl\typeout@pt@nl@mss \ps@plaintop \let\references@refpar\references@refpar@mss \def\pt@headfrac@ass@normalsize{.08} \def\pt@headfrac@ass@footnotesize{.1} \def\pt@headfrac@ass@scriptsize{.12} \def\pt@notemin@normal{3} \def\pt@notemin@footnote{3} \def\pt@notemin@script{4} }% \def\journal{\@gobble}% \def\volume{\@gobble}% \def\issue{\@gobble}% \def\SGMLbi#1{#1}% \def\SGMLbsc#1{#1}% \def\SGMLclc#1{#1}% \def\SGMLentity#1{\}% \def\SGML{\@gobble}% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% %% Modify the |\@makecol| macro for one-column abstract. \newif\if@printfoot% \global\@printfoottrue% \global\newbox\my@footins \gdef \@makecol@pptt {% \ifvoid\footins \setbox\@outputbox \box\@cclv \else \if@printfoot \else \global\setbox\my@footins\vbox{\box\footins} %\global\advance\c@colht by -\ht\my@footins \fi \setbox\@outputbox \vbox{% \global\setbox\footins\vbox{\unvbox\my@footins\unvbox\footins} \boxmaxdepth \@maxdepth \unvbox\@cclv \if@printfoot \vskip\skip\footins \color@begingroup \normalcolor \footnoterule \unvbox \footins \color@endgroup \else \global\@printfoottrue \fi }% \fi \xdef\@freelist{\@freelist\@midlist}% \global \let \@midlist \@empty \@combinefloats \ifvbox\@kludgeins \@makespecialcolbox \else \setbox\@outputbox \vbox to \@colht{% \@texttop \dimen@ \dp\@outputbox \unvbox \@outputbox \ifbotragg% \vskip -\dimen@ \@textbottom \fi }% \fi \global \maxdepth \@maxdepth } %% %% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% macro to switch from one-column long abstract to two-column normal text \iflong@abstract \newtoks\juo@sar \juo@sar={} \def\@ca#1#2#3#4{} \@ifundefined{stripsep}{\newskip\stripsep\stripsep 15pt}{} \newskip\m@addvipersep \m@addvipersep\z@ \newskip\c@addvipersep \c@addvipersep\z@ \newdimen\ht@strip \newdimen\right@cor \newdimen\cor@height \cor@height=0pt \newdimen\juo@pr \newdimen\juo@ht \newbox\@viper \newcount\juo@sk \newdimen\c@colht \newbox\my@outputbox %% macro for adding strip \def\add@strip#1#2#3#4{\begingroup% \xdef\ex@{\global\noexpand\juo@sar{\the\juo@sar\noexpand\@ca{#1}{#2}{#3}{#4}}}\ex@% \endgroup} %% macro for remove strip \def\remove@strip#1{\ifx#1\@empty\global\juo@sk=0\else \global\advance\juo@sk by-1\expandafter\next@item\the #1\@@#1\fi} \def\next@item \@ca#1#2#3#4#5\@@#6{\global #6={#5}\global\juo@pr=#1\global\juo@ht=#2% \global\cor@height=#3\global\m@addvipersep=#4} %% macro for strip command \def\strip{\@ifnextchar[{\@strip}{\@strip[0pt/0pt]}} \def\@strip[#1/#2]{\global\@tempdima=#1\global\@tempdimb=#2% \global \setbox\@viper\vbox\bgroup% \hsize\textwidth \@parboxrestore \col@number \@ne \vrule height\topskip width\z@ depth\z@} \def\endstrip{% \egroup \if@firstcolumn \ifdim\pagetotal>\z@ \global\ht@strip\pagegoal \global\advance\ht@strip by-\pagetotal \global\advance\ht@strip by-\stripsep \global\advance\ht@strip by-\ht\@viper \global\advance\ht@strip by-\stripsep \global\juo@ht=\ht\@viper \else \global\ht@strip\z@ \fi \ifdim\ht@strip>\z@ \add@strip{\the\pagetotal}{\the\juo@ht}{\the\@tempdima}{\the\@tempdimb}% \global\advance\juo@sk by1 \fi \fi } \newif\ifbotragg\botraggfalse \def\@outputdblcol@pptt{% \if@firstcolumn \global\@firstcolumnfalse \global\setbox\@leftcolumn\box\@outputbox \global\c@colht\@colht\global\c@addvipersep\z@ \ifnum\juo@sk>0 \remove@strip\juo@sar \global\@colht\the\juo@pr \global\@printfootfalse \ifdim\right@cor>\z@ \global\advance\@colht by\right@cor \fi \global\advance\@colht by\cor@height \global\cor@height=0pt \fi \else \ifdim\c@colht>\@colht% \@tempdima\@colht% \ifdim\@colht>\z@%% \ifvoid\footins% \else% \vskip-\skip\footins% \fi% \splittopskip0pt% \setbox\my@outputbox\vbox{% \vspace*{\@colht}%% \global\botraggfalse% \vskip.7\baselineskip% \vsplit\@outputbox to \baselineskip% \unvbox\@outputbox}% \unvbox\my@outputbox% \ifvoid\my@outputbox% \global\botraggtrue \fi% \global \@printfoottrue \global\c@addvipersep\m@addvipersep% \else% \fi% \ifnum\juo@sk>0% \else% \global\@colht\c@colht% \fi% \else% \global \@firstcolumntrue% \global\setbox\@outputbox\vbox to \ht\@leftcolumn{\unvbox\@outputbox}% \setbox\@outputbox \vbox{\hb@xt@\textwidth {% \hb@xt@\columnwidth {\box\@leftcolumn \hss}% \hfil \vrule \@width\columnseprule \hfil \hb@xt@\columnwidth{\box\@outputbox \hss}}% \vss}% \@combinedblfloats \@outputpage \begingroup \@dblfloatplacement \@startdblcolumn \@whilesw\if@fcolmade \fi {\@outputpage\@startdblcolumn}% \endgroup \global\juo@sk=0\global\juo@sar={}% \global\cor@height\z@\global\c@addvipersep\z@ \fi \fi } \fi \endinput %% %% End of file `aastex.cls'. emulateapj.cls0100644000000000000000000012367010376206774012434 0ustar rootroot%% This is emulateapj.cls, version Sept 8, 2003 %% For the latest version check http://hea-www.harvard.edu/~alexey/emulateapj %% %% 2/9/03: MAJOR CHANGE: This is a complete rewrite of emulateapj. It adds %% the use of single-column floats (figures, tables and footnotes) in the %% two-column mode. All standard LaTeX/AASTeX environments such as %% {figure}, {table}, {figure*}, {table*} and {deluxetable} (and %% {deluxetable*} added here) should work as expected. Enjoy. %% %% %% `emulateapj' is a LaTeX2e class to emulate the Astrophysical Journal %% (ApJ) page layout. The page length of the resulting document is very %% close to that in ApJ when Times fonts are used instead of the LaTeX %% default CM fonts (see below). %% %% If a manuscript is prepared for ApJ submission using the standard AAS %% (American Astronomical Society) LaTeX macros and the `aastex' style (see %% instructions for authors on the ApJ web site), the only thing required %% from the user should be to replace \documentclass{aastex} with %% \documentclass{emulateapj}, and perhaps resize figures as desired and %% replace {deluxetable} with {deluxetable*} %% (possible minor problems are described below). %% %% emulateapj requires revtex4.cls. If you don't have it already, it can be %% downloaded from http://publish.aps.org/revtex4/ (it's a small package). %% Other extrnal packages used are latexsym, graphicx, amssymb, longtable, %% epsf. They should already be present in the modern TeX distributions; if %% not, download them from www.ctan.org. %% %% To switch to the Times font, use the accompanying file apjfonts.sty (see %% the site above): %% \usepackage{apjfonts}. Alternatively, e.g., use the standard %% \usepackage{mathptmx}, the only difference is in math and Greek symbols. %% %% Alexey Vikhlinin %% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% Release notes (02/09/03): %% %% 1) This is a complete rewrite of emulateapj. The package is now %% based on revtex instead of aastex + multicol. Some inconsistencies with %% aastex may have been missed, so please don't hesitate to report them. %% %% 2) The {deluxetable} environment is re-implemented (the problem with the %% the aastex's deluxetable is it does not float). There is also a new %% environment {deluxetable*} (absent in aastex) to set a floating table %% two-column wide. These were not thoroughly tested, so please report any %% problems. Known problems: %% (a) \rotate doesn't work (too difficult to implement). Place the table %% at the end of the paper after references, inside {turnpage} environment %% (\begin{turnpage}\begin{deluxetable} ... \end{deluxetable}\end{turnpage}) %% %% 3) Multi-page tables cannot be set properly inside the main text; you %% need to move the table to the end of the paper (after the references) and %% issue the command \LongTables before it. %% %% 4) By default, deluxetables are typeset with \footnotesize. If you want %% to use a different size, use, e.g., \tabletypesize{\normalsize} _outside_ %% the deluxetable environment. If you need to increase interline spacing %% in the tables, use \def\arraystretch{1.XXX} also _outside_ deluxetables. %% %% 5) Option `onecolumn' (as in \documentclass[onecolumn]{emulateapj}) %% sets the whole paper (except the reference section) in one column %% as done by the ApJ for papers with long equations. %% %% 6) Options `apj' and `apjl' (\documentclass[apj]{emulateapj}) change the %% spacing of the references (the default is ApJL wide spacing). %% %% 7) By default, appendix subsections are not numbered: %% APPENDIX %% Derivation of Equations %% If you want them numbered (`A. Derivation of Equations'), use the option %% \documentclass[numberedappendix]{emulateapj} %% %% 8) By default, the comment in the upper-left corner of the title page and %% under the abstract will say "Draft version \today". There are additional %% commands \journalinfo{} and \submitted{} (the latter is equivalent to the %% aastex \slugcomment{} which also works) to change those comments. Used %% alone, \submitted{} will act on both those places. %% %% 9) The \title command sets the entire title, including math, in upper %% case. If this is undesirable, use \lowercase{} macro, e.g., %% \title{UPPER CASE OK HERE \lowercase{$a+b=c$}}. %% %% 10) On the last page where the references start, there may be problems %% with placement of footnotes. There is a command \lastpagefootnotes which %% can be issued somewhere before those footnotes. It will result in the %% remaining footnotes set together at the end of the text, properly %% adjusted. %% %% 11) There may be problems with single-column figure placements on the %% last page; try moving the figure around or explicitly specifying [t] %% placement. There may also be minor column misalignments on %% complicated pages with footnotes, sections, etc.; these are too difficult %% to fix. %% %% 12) Any footnotes in the paper title should be set as %% \title{Title\footnotemark[1]} \footnotetext[1]{text} (with foootnotetext %% outside the title), rather that simply a \footnote{}. %% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% changes since 2/9/3: %% %% 2/14/3: fixed several bugs in deluxetable and footnotes inside the title. %% %% 3/3/3: Table caption is made in two lines. works only in {table} or %% {table*}, but not in {deluxetable} %% %% 3/3/3: Redefine p@subsection etc. for ApJ-style cross-references. %% %% 3/16/3: Define \tablerefs %% %% 3/25/3: Fix two-column references in the onecolumn mode (see %% \set@column@hsize{2}) %% %% 4/9/3: Change the definition of \tablenotemark. It is less general but %% works in the table caption. Also, put the body of deluxetable* %% inside a minipage to fix table footnotes. %% %% 5/14/3: Change section title font sizes. They are now different for 'apj' %% and 'apjl' options %% %% 7/8/3: redefine NAT@sort@cites after loding revtex4 to prevent citations %% from being sorted %% %% 7/15/3: Fix \and in the author list %% %% 7/17/3: Make \colhead to center column titles by default %% %% 7/27/3: Redefile \@biblabel to remove the numbered list from thebibliography %% %% 9/08/3: Further fixes to cutinhead: define @ptabularcr and use LT@cols %% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% Copyright 2000-2003 Alexey Vikhlinin %% %% The first version of this package was written by Maxim Markevitch. %% Pieces of AASTeX style are used. %% %% This program can be redistributed and/or modified under the terms %% of the LaTeX Project Public License available from CTAN archives in %% directory macros/latex/base/lppl.txt. This means you are free to use and %% distribute this package; however, if you modify anything, please change the %% file name and remove the authors email address. %% %% Alexey Vikhlinin %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \def\emulapj@ver{9/08/03} \ProvidesClass{emulateapj} \newif\if@two@col \DeclareOption{twocolumn}{\@two@coltrue} \DeclareOption{onecolumn}{\@two@colfalse} \newlength{\bibbaselineskip}\setlength{\bibbaselineskip}{3.075mm} \DeclareOption{numberedappendix}{ \def\AppendixApjSectionMarkInTitle#1{#1.\ } } \DeclareOption{apj}{ \setlength{\bibbaselineskip}{2.7mm} \def\apjsecfont{\small} \def\secnum@size{\small} \def\subsecnum@size{\normalsize} } \DeclareOption{apjl}{ \setlength{\bibbaselineskip}{3.075mm} \def\apjsecfont{\footnotesize} \def\secnum@size{\small} \def\subsecnum@size{\small} } \def\AppendixApjSectionMarkInTitle#1{\relax} \DeclareOption{numberedappendix}{ \def\AppendixApjSectionMarkInTitle#1{#1.\ } } \def\center@table@notes{% \def\@spew@tblnotes{% \centerline{\begin{minipage}{\pt@width}\spew@tblnotes\end{minipage}}% }% } \def\left@just@table@notes{% \def\@spew@tblnotes{\spew@tblnotes}% } \left@just@table@notes \ExecuteOptions{apjl,twocolumn} \ProcessOptions \let\@startsection@from@latex=\@startsection \if@two@col \LoadClass[twocolumn,nofootinbib,showkeys,twoside,floatfix]{revtex4} \else \LoadClass[nofootinbib,showkeys,twoside,floatfix]{revtex4} \fi % Restore natbib package without sorting. \def\NAT@sort{0} \def\NAT@sort@cites#1{\edef\NAT@cite@list{#1}} \RequirePackage{latexsym}% \RequirePackage{graphicx}% \RequirePackage{amssymb}% \RequirePackage{longtable}% \newcommand{\bibstyle@aas}{\bibpunct{(}{)}{;}{a}{}{,}}% \@citestyle{aas}% \let\@startsection=\@startsection@from@latex \def\baselinestretch{1.02} \AtBeginDocument{\def\arraystretch{1.0}} \RequirePackage{epsf,graphicx} %%%%%%%% The following code is taken from size10.clo; it fixes %%%%%%%% aastex's definition of type sizes \renewcommand\normalsize{% \@setfontsize\normalsize\@xpt{10.56} \abovedisplayskip 2.2mm \@plus2\p@ \@minus5\p@ \abovedisplayshortskip \z@ \@plus3\p@ \belowdisplayshortskip 6\p@ \@plus3\p@ \@minus3\p@ \belowdisplayskip \abovedisplayskip \let\@listi\@listI} \normalsize \renewcommand\small{% \@setfontsize\small\@ixpt{9.68}% \abovedisplayskip 8.5\p@ \@plus3\p@ \@minus4\p@ \abovedisplayshortskip \z@ \@plus2\p@ \belowdisplayshortskip 4\p@ \@plus2\p@ \@minus2\p@ \def\@listi{\leftmargin\leftmargini \topsep 4\p@ \@plus2\p@ \@minus2\p@ \parsep 2\p@ \@plus\p@ \@minus\p@ \itemsep \parsep}% \belowdisplayskip \abovedisplayskip } \renewcommand\footnotesize{% \@setfontsize\footnotesize\@viiipt{8.36}% \abovedisplayskip 6\p@ \@plus2\p@ \@minus4\p@ \abovedisplayshortskip \z@ \@plus\p@ \belowdisplayshortskip 3\p@ \@plus\p@ \@minus2\p@ \def\@listi{\leftmargin\leftmargini \topsep 3\p@ \@plus\p@ \@minus\p@ \parsep 2\p@ \@plus\p@ \@minus\p@ \itemsep \parsep}% \belowdisplayskip \abovedisplayskip } \renewcommand\scriptsize{\@setfontsize\scriptsize\@viipt\@viiipt} \renewcommand\tiny{\@setfontsize\tiny\@vpt\@vipt} \renewcommand\large{\@setfontsize\large\@xiipt{14}} \renewcommand\Large{\@setfontsize\Large\@xivpt{18}} \renewcommand\LARGE{\@setfontsize\LARGE\@xviipt{22}} \renewcommand\huge{\@setfontsize\huge\@xxpt{25}} \renewcommand\Huge{\@setfontsize\Huge\@xxvpt{30}} \setlength\smallskipamount{3\p@ \@plus 1\p@ \@minus 1\p@} \setlength\medskipamount{6\p@ \@plus 2\p@ \@minus 2\p@} \setlength\bigskipamount{12\p@ \@plus 4\p@ \@minus 4\p@} \setlength\headheight{12\p@} \def\@listi{\leftmargin\leftmargini \parsep 4\p@ \@plus2\p@ \@minus\p@ \topsep 8\p@ \@plus2\p@ \@minus4\p@ \itemsep4\p@ \@plus2\p@ \@minus\p@} \let\@listI\@listi \@listi \def\@listii {\leftmargin\leftmarginii \labelwidth\leftmarginii \advance\labelwidth-\labelsep \topsep 4\p@ \@plus2\p@ \@minus\p@ \parsep 2\p@ \@plus\p@ \@minus\p@ \itemsep \parsep} \def\@listiii{\leftmargin\leftmarginiii \labelwidth\leftmarginiii \advance\labelwidth-\labelsep \topsep 2\p@ \@plus\p@\@minus\p@ \parsep \z@ \partopsep \p@ \@plus\z@ \@minus\p@ \itemsep \topsep} \def\@listiv {\leftmargin\leftmarginiv \labelwidth\leftmarginiv \advance\labelwidth-\labelsep} \def\@listv {\leftmargin\leftmarginv \labelwidth\leftmarginv \advance\labelwidth-\labelsep} \def\@listvi {\leftmargin\leftmarginvi \labelwidth\leftmarginvi \advance\labelwidth-\labelsep} % **************************************************** % * TWO AND SINGLE ONE COLUMN STYLES: AV * % **************************************************** % %%%%% include atbeginend.sty by AV: % Copy \begin and \end to \BeginEnvironment and \EndEnvironment \let\BeginEnvironment=\begin \let\EndEnvironment=\end %% \ifundefined from TeXbook \def\IfUnDef#1{\expandafter\ifx\csname#1\endcsname\relax} % Null command needed to eat its argument \def\NullCom#1{} \def\begin#1{% % if defined \BeforeBeg for this environment, execute it \IfUnDef{BeforeBeg#1}\else\csname BeforeBeg#1\endcsname\fi% \IfUnDef{AfterBeg#1}% This is done to skip the command for environments % which can take arguments, like multicols; YOU MUST NOT % USE \AfterBegin{...}{...} for such environments! \let\SaveBegEnd=\BeginEnvironment% \else % Start this environment \BeginEnvironment{#1}% % and execute code after \begin{environment} \csname AfterBeg#1\endcsname \let\SaveBegEnd=\NullCom \fi \SaveBegEnd{#1} } \def\end#1{% % execute code before \end{environment} \IfUnDef{BeforeEnd#1}\else\csname BeforeEnd#1\endcsname\fi% % close this environment \EndEnvironment{#1} % and execute code after \begin{environment} \IfUnDef{AfterEnd#1}\else\csname AfterEnd#1\endcsname\fi% } \long\def\BeforeBegin#1#2{\expandafter\gdef\csname BeforeBeg#1\endcsname {#2}} \long\def\BeforeEnd #1#2{\expandafter\gdef\csname BeforeEnd#1\endcsname {#2}} \long\def\AfterBegin #1#2{\expandafter\gdef\csname AfterBeg#1\endcsname {#2}} \long\def\AfterEnd #1#2{\expandafter\gdef\csname AfterEnd#1\endcsname{#2}} %%%% end of atbeginend.sty % **************************************** % * PAGE LAYOUT * % **************************************** % Page size, spacing parameters, etc. \textwidth=7.1in \columnsep=0.3125in \parindent=0.125in \voffset=-20mm \hoffset=-7.5mm \topmargin=0in \headheight=.15in \headsep=0.5in \oddsidemargin=0in \evensidemargin=0in \parskip=0cm %\tolerance=600 % 3x "normal" value; cuts down on overfull complaints %% AV,MM, to have 64 lines per column, with textheight 25cm: \textheight=64\baselineskip %\textheight=\baselinestretch\textheight \ifdim\textheight>25.2cm\textheight=25.0cm\fi \let\tighten=\relax \let\tightenlines=\tighten \let\singlespace=\relax \let\doublespace=\relax \def\eqsecnum{ \@newctr{equation}[section] \def\theequation{\hbox{\normalsize\arabic{section}-\arabic{equation}}}} %% running heads: \def\lefthead#1{\gdef\@versohead{#1}} \lefthead{\relax} \def\righthead#1{\gdef\@rectohead{#1}} \righthead{\relax} \let\shorttitle=\lefthead % New AASTEX commands \let\shortauthors\righthead % New AASTEX commands %% MM Create "apjheads" page style: \def\ps@apjheads{\let\@mkboth\markboth \def\@evenfoot{} \def\@evenhead{\lower9mm\hbox to\textwidth{ \rm\thepage\hfil \rm\@rectohead \hfil}}} \def\@oddfoot{} \def\@oddhead{\lower9mm\hbox to\textwidth{ \hfil\rm\@versohead\hfil \rm\thepage}} \@twosidetrue \ps@apjheads %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % TITLE PAGE % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \long\def\frontmatter@title@above{ \vspace*{-\headsep}\vspace*{\headheight} \footnotesize {\footnotesize\textsc{\@journalinfo}}\par {\scriptsize Preprint typeset using \LaTeX\ style emulateapj v.\ \emulapj@ver}\par\vspace*{-\baselineskip}\vspace*{0.625in} }% \def\frontmatter@title@produce{% \begingroup \frontmatter@title@above \frontmatter@title@format \@title \@ifx{\@title@aux\@title@aux@cleared}{}{% \expandafter\frontmatter@footnote\expandafter{\@title@aux}% }% \par %% \class@warn{Unused short title ignored}% \frontmatter@title@below \endgroup }% \renewcommand\title[2][]{% \def\@title{\uppercase{#2}}% \def\@shorttitle{#1}% \let\@AF@join\@title@join }% \def\frontmatter@title@format{\normalsize\centering} \def\frontmatter@title@below{\vspace*{-2.63\baselineskip\vspace*{0.25in}}}% \def\frontmatter@above@affilgroup{\vspace*{0.25in}}% \def\frontmatter@authorformat{\small\scshape\centering}% \def\frontmatter@affiliationfont{\normalfont\footnotesize}% \def\frontmatter@finalspace{\vspace*{-\baselineskip}\vspace*{0.375in}} \def\@separator{\\}% \def\frontmatter@footnote#1{% \begingroup \@booleanfalse\temp@sw \def\@tempa{#1}% \let\@tempb\@empty \def\@TBN@opr{\y@match\@tempa}% \@FMN@list \temp@sw{% \expandafter\frontmatter@footnotemark \expandafter{\@tempb}% }{% \def\@thefnmark{\relax} \frontmatter@footnotetext{#1} }% \endgroup }% \newcounter{front@matter@foot@note}\setcounter{front@matter@foot@note}{0} \def\frontmatter@above@affiliation{\vspace*{0.5mm}}% \renewcommand\affiliation[1]{% \move@AU\move@AF% \begingroup% \@affiliation{\hspace*{2mm}#1}% }% \let\affil=\affiliation \def\altaffilmark#1{\textsuperscript{#1}} \def\altaffiltext#1#2{\altaffiliation{\hspace*{3mm}\textsuperscript{#1}~#2}\stepcounter{front@matter@foot@note}} \let\old@foot@note@mark=\footnotemark \let\old@foot@note@text=\footnotetext \def\footnotemark[#1]{\altaffilmark{#1}} \def\footnotetext[#1]#2{\altaffiltext{#1}{#2}} % ABSTRACT \def\frontmatter@abstractfont{\normalsize}% \def\frontmatter@abstractwidth{6in} \def\frontmatter@preabstractspace{0.0\baselineskip} \def\frontmatter@postabstractspace{0.0\baselineskip} \def\abstractname{ABSTRACT} \long\def\frontmatter@abstractheading{% \vspace*{-\baselineskip}\vspace*{1.5pt} \centerline{\itshape\footnotesize\@submitted} \vspace*{0.13189in} \begingroup \centering \abstractname \vskip 1mm \par \endgroup \everypar{\rightskip=0.5in\leftskip=\rightskip}\par }% % Redefine the LaTeX \and command for this style. \def\and{\author{\vspace*{-0.2in}and\vspace*{-0.558cm}}\noaffiliation} \def\@listand{\@ifnum{\@tempcnta=\tw@}{\andname\space}{}}% % **************************************** % * KEYWORDS * % **************************************** \def\@keys@name{\textit{Subject headings:}\/~\mbox{}}% \newlength{\keys@width} \def\frontmatter@keys@format{\vspace*{0.5mm}% \settowidth{\keys@width}{\normalsize\@keys@name}% \rightskip=0.5in\leftskip=\rightskip\parindent=0pt% \hangindent=\keys@width\hangafter=1\normalsize}% \def\@keywords@produce#1{% \showKEYS@sw{% \begingroup% \frontmatter@keys@format% \@keys@name#1\par \endgroup }{% \@if@empty{#1}{}{% \class@warn{If you want your keywords to appear in your output, use document class option showkeys}% }% }% }% \let\subjectheadings=\keywords % **************************************** % * FOOTNOTES * % **************************************** % Modify code from revtex: \def\@xfootnotemark@ltx[#1]{% \begingroup % \csname c@\@mpfn\endcsname #1\relax \unrestored@protected@xdef\@thefnmark{#1}% \endgroup \H@@footnotemark }% % Modify code from LaTeX to fix footnotes: \def\@xfootnotenext[#1]{% \begingroup % \csname c@\@mpfn\endcsname #1\relax \unrestored@protected@xdef\@thefnmark{#1}% \endgroup \@footnotetext} % Footnotes on the last page: user issues \lastpagefootnotes. It catches all % footnotes and issues them before \begin{refernces} or % \begin{\thebibliography} at the end of right column. \newcounter{lastfootnote} \setcounter{lastfootnote}{0} \long\gdef\lastfootnote{\mbox{}} \let\orig@footnote=\footnote \long\def\lastpagefootnotes{ \long\def\footnote##1{\refstepcounter{lastfootnote}\footnotemark\g@addto@macro\lastfootnote{\\[\footnotesep]\refstepcounter{footnote}\mbox{}\hspace*{3mm}\textsuperscript{\thefootnote}~##1}} \BeforeBegin{references}{\addtocounter{footnote}{-\c@lastfootnote}\vspace*{-\baselineskip}\vspace*{\skip\footins}\bgroup\footnotesize\lastfootnote\par\egroup} \BeforeBegin{thebibliography}{\addtocounter{footnote}{-\c@lastfootnote}\vspace*{-\baselineskip}\vspace*{\skip\footins}\bgroup\footnotesize\lastfootnote\par\egroup} \AfterEnd{references}{\let\footnote=\orig@footnote} \AfterEnd{thebibliography}{\let\footnote=\orig@footnote} } \let\lastpagefootnote=\lastpagefootnotes % this command is copied from the original revtex, but adds space above % footnote (if any) above the references. \@namedef{balance@2}{% \expandafter\balance@two\csname col@1\endcsname\@outputbox % Avoid a bug by preventing a restore when leaving this group \global\setbox\csname col@1\endcsname\box\csname col@1\endcsname \@ifvoid\footbox{}{% \global\setbox\footbox\vbox{% \setbox\z@\box\@tempboxa \let\recover@footins\relax \balance@two\footbox\@tempboxa \vskip\skip\footins \hb@xt@\textwidth{\box\footbox\hfil\box\@tempboxa}% }% }% }% \skip\footins 4.5mm plus 1mm minus 1mm \footnotesep 0pt \let\footnoterule\relax \def\@makefntext#1{\mbox{}\hspace*{3mm}\@makefnmark~#1} \def\notetoeditor#1{}% % We do not need notes to editor in the preprint \def\placetable#1{}% % We do not need notes to editor in the preprint \def\placefigure#1{}% % We do not need notes to editor in the preprint % **************************************** % * SECTIONS * % **************************************** \newif\if@firstsection \@firstsectiontrue \def\section{% \if@firstsection\@firstsectionfalse \maketitle\setcounter{footnote}{\thefront@matter@foot@note} \let\footnotetext=\old@foot@note@text \let\footnotemark=\old@foot@note@mark \fi \@startsection{section}{1}{\z@}{9pt plus 2pt minus 1pt}{4pt}{\apjsecfont\center}} \def\subsection{\@startsection{subsection}{2}{\z@}{9pt plus 1pt minus 1pt}{4pt}% {\normalsize\itshape \center}} \def\subsubsection{\@startsection{subsubsection}{3}{\z@}% {2ex plus 1ex minus .2ex}{1ex plus .2ex}{\normalsize\it \center}} \def\thesection{\@arabic{\c@section}} \def\thesubsection{\thesection.\@arabic{\c@subsection}} \def\thesubsubsection{\thesubsection.\@arabic{\c@subsubsection}} \def\theparagraph{\thesubsubsection.\@arabic{\c@paragraph}} \def\p@section {} \def\p@subsection {} \def\p@subsubsection {} \def\p@paragraph {} \def\p@subparagraph {} \def\sec@upcase#1{\uppercase{#1}} \def\subsec@upcase#1{\relax{#1}} % % How the section number will appear in the section title - AV \def\ApjSectionMarkInTitle#1{#1.\ } \def\ApjSectionpenalty{0} \def\@sect#1#2#3#4#5#6[#7]#8% {\@tempskipa #5\relax \ifdim \@tempskipa >\z@ \begingroup #6\relax \ifnum #2>\c@secnumdepth \def \@svsec {}\else \refstepcounter{#1} \edef \@svsec {\ApjSectionMarkInTitle {\csname the#1\endcsname}}\fi \@hangfrom {\hskip #3\relax \ifnum #2=1\secnum@size {\rm\@svsec~}% \else \subsecnum@size {\rm\@svsec~}\fi }% {\interlinepenalty \@M \ifnum #2=1\sec@upcase{#8}% \else \subsec@upcase{#8}\fi\par}\endgroup \csname #1mark\endcsname {#7}\addcontentsline{toc}{#1}% {\ifnum #2>\c@secnumdepth \else \protect \numberline {\csname the#1\endcsname }\fi #7}% \else \ifnum #2>\c@secnumdepth \def \@svsec {}\else \refstepcounter{#1} \edef \@svsec {\ApjSectionMarkInTitle {\csname the#1\endcsname}}\fi \def \@svsechd {#6\hskip #3% \ifnum #2=1\secnum@size{\rm\@svsec~}\else\subsecnum@size{\rm\@svsec~}\fi% \ifnum #2=1\sec@upcase{#8}\else\subsec@upcase{#8}\fi% \csname #1mark\endcsname {#7}\addcontentsline{toc}{#1}% {\ifnum #2>\c@secnumdepth \else \protect \numberline {\csname the#1\endcsname }\fi #7}}\fi \@xsect {#5} \penalty \ApjSectionpenalty %-refstepcounter is now within a group. So \@currentlabel, which is normally %-set by \refstepcounter is hidden within a group. Need to set it manually. \protected@edef\@currentlabel{\csname p@#1\endcsname\csname the#1\endcsname} } \def\@ssect#1#2#3#4#5{\@tempskipa #3\relax \ifdim \@tempskipa>\z@ \begingroup #4\@hangfrom{\hskip #1}{\interlinepenalty \@M \sec@upcase{#5}\par}\endgroup \else \def\@svsechd{#4\hskip #1\relax \sec@upcase{#5}}\fi \@xsect{#3} % MM: \penalty \ApjSectionpenalty} \def\acknowledgments{\vskip 5.8mm plus 1mm minus 1mm} \let\acknowledgements=\acknowledgments % second spelling % **************************************** % * APPENDIX * % **************************************** \renewenvironment{appendix}[0]{ \onecolumngrid \vskip 10pt plus 2pt minus 1pt \noindent\mbox{}\hfill{\small APPENDIX}\hfill\mbox{}\par \nopagebreak\medskip\@nobreaktrue\def\ApjSectionpenalty{\@M} \@firstsectionfalse \setcounter{section}{0} \setcounter{subsection}{0} \setcounter{equation}{0} % \setcounter{figure}{0} % \setcounter{table}{0} % \def\fnum@figure{Figure \Alph{section}\thefigure:} % \def\fnum@table{Table \Alph{section}\thetable:} \def\thesection{\Alph{section}} \def\theequation{\hbox{\Alph{section}\arabic{equation}}} \def\thefigure{\thesection\@arabic\c@figure} \def\thetable{\thesection\@arabic\c@table} % % Do not use appendix numbers in the titles \def\ApjSectionMarkInTitle{\AppendixApjSectionMarkInTitle} \def\section{\setcounter{equation}{0}\@startsection {section}{1}{\z@} {10pt}{5pt}{\centering\scshape}} % % }{} % **************************************** % * BIBLIOGRAPHY * % **************************************** \renewenvironment{references}[0]{ \onecolumngrid \par \vspace*{10pt plus 3pt} \noindent \makebox[\textwidth][c]{\footnotesize REFERENCES} \par \vspace*{4pt plus 3pt} \set@column@hsize{2}\twocolumngrid \parindent=0cm \parskip=0cm \def\baselinestretch{1.0} \footnotesize \baselineskip=\baselinestretch\bibbaselineskip plus 1pt minus 1pt \interlinepenalty \@M \hyphenpenalty=10000 \frenchspacing % AV - to get right spacing after ``et al.'' \def\refpar{\par\hangindent=1.2em\hangafter=1}} { \onecolumngrid } % redefine thebibliography % redefine thebibliography % remove numbers from the reference list \def\@biblabel#1{\relax} \newdimen\bibindent \renewenvironment{thebibliography}[1]{ \onecolumngrid \par \vspace*{10pt plus 3pt} \noindent \makebox[\textwidth][c]{\footnotesize REFERENCES} \par \vspace*{4pt plus 3pt} \set@column@hsize{2}\twocolumngrid \list{}% { \parindent=0pt \parskip=0pt \parsep=0pt % AV \bibindent=0pt % \def\baselinestretch{1.0} \footnotesize \baselineskip=\bibbaselineskip \interlinepenalty \@M % AV \frenchspacing % AV - to get right spacing after ``et al.'' \hyphenpenalty=10000 \itemindent=-1.0em % \itemsep=0pt % \listparindent=0pt % \settowidth\labelwidth{0pt} % \labelsep=0pt % \leftmargin=1.0em \advance\leftmargin\labelsep %%% \usecounter{enumiv}% \let\p@enumiv\@empty \renewcommand\theenumiv{\relax}}% \sloppy\clubpenalty4000\widowpenalty4000% \sfcode`\.\@m} {\def\@noitemerr {\@latex@warning{Empty `thebibliography' environment}}% \endlist \onecolumngrid } % %% AV: \def\reference{\@ifnextchar\bgroup {\@reference} {\@latexerr{Missing key on reference command} {Each reference command should have a key corresponding to a markcite somewhere in the text}}} \def\@reference#1{\refpar} %% subtitle header and journal info: \def\submitted#1{\gdef\@submitted{#1}} \def\journalinfo#1{\gdef\@journalinfo{#1}} \def\subtitle{ \vspace*{-12mm} \noindent {\scriptsize {\sc \@journalinfo} \\ Preprint typeset using \LaTeX\ style emulateapj v.\ \emulapj@ver} } \let\slugcomment\submitted % slugcomment == submitted \submitted{Draft version \today} \journalinfo{\@submitted} %% AV: allow figures to take the whole page \renewcommand{\topfraction}{1.0} \renewcommand{\bottomfraction}{1.0} \renewcommand{\textfraction}{0.0} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % Equations % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % EQNARRAY with reduced spacing around tab characters - AV \def\eqnarray{% \stepcounter{equation}% \def\@currentlabel{\p@equation\theequation}% \global\@eqnswtrue \setlength{\arraycolsep}{0.25\arraycolsep} \m@th \global\@eqcnt\z@ \tabskip\@centering \let\\\@eqncr $$\everycr{}\halign to\displaywidth\bgroup \hskip\@centering$\displaystyle\tabskip\z@skip{##}$\@eqnsel &\global\@eqcnt\@ne\hskip \tw@\arraycolsep \hfil${##}$\hfil &\global\@eqcnt\tw@ \hskip \tw@\arraycolsep $\displaystyle{##}$\hfil\tabskip\@centering &\global\@eqcnt\thr@@ \hb@xt@\z@\bgroup\hss##\egroup \tabskip\z@skip \cr } % **************************************** % * TABLES AND FIGURES * % **************************************** \def\@arstrut@hline@clnc{0.5\p@}% % Klootch: magic number \setcounter{topnumber}{7} \setlength{\belowcaptionskip}{0pt} \setlength{\abovecaptionskip}{5pt} \setlength{\textfloatsep}{-\baselineskip} \addtolength{\textfloatsep}{12mm plus 10mm minus 10mm} \setlength{\dbltextfloatsep}{-\baselineskip} \addtolength{\dbltextfloatsep}{12mm plus 10mm minus 10mm} \renewcommand{\topfraction}{1.0} \renewcommand{\bottomfraction}{1.0} \renewcommand{\textfraction}{0.0} \renewcommand{\dbltopfraction}{1.0} % Copyed from revtex4.cls; without it, captions are centered \def\@xfloat@prep{% \let\footnote\footnote@latex \def\@mpfn{mpfootnote}% \def\thempfn{\thempfootnote}% \c@mpfootnote\z@ \let\@footnotetext\@mpfootnotetext \let\H@@footnotetext\@mpfootnotetext \let\@makefntext\@mpmakefntext }% \long\def\@makecaption#1#2{% \noindent\begin{minipage}{0.9999\linewidth} %% \noindent is needed because %% otherwise minipage + parindent does not fit into the line and spurious %% vertical skip appear after caption \if\csname ftype@\@captype\endcsname 2 \vskip 2ex\noindent \centering\small\scshape #1\par #2\par\medskip \else \vskip \abovecaptionskip\footnotesize\noindent #1 #2\par\vskip \belowcaptionskip \fi \end{minipage} } %%%%%%%%%%%% FIX \cutinhead \def\@ptabularcr{\\} \newcommand\cutinhead[1]{% \noalign{\vskip 1.5ex}% \hline \@ptabularcr \noalign{\vskip -1.5ex}% \multicolumn{\LT@cols}{c}{#1}% \@ptabularcr \noalign{\vskip .8ex}% \hline \@ptabularcr \noalign{\vskip -2ex}% }% \newcommand\figcaption{\@testopt{\@xfigcaption}{}}% %% suggested by Joern Wilms wilms@astro.uni-tuebingen.de %% wilms@rocinante.colorado.edu \def\@figcaption#1{{\def\@captype{figure}\caption{\footnotesize #1}}} \def\@xfigcaption[#1]#2{{\def\@captype{figure}\caption{\footnotesize #2}}} \def\thefigure{\@arabic\c@figure} \def\fnum@figure{{\footnotesize\scshape ~~Fig.\space\thefigure.---}} \def\thetable{\@arabic\c@table} %%% Table captions without making a floating table \def\tabcaption{\@ifnextchar[{\@xtabcaption}{\@tabcaption}} \def\@tabcaption#1{{\def\@captype{table}\caption{#1}}} \def\@xtabcaption[#1]#2{{\def\@captype{table}\caption{#2}}} \def\fnum@table{\scshape Table~\thetable} % \let\fnum@ptable=\fnum@table % \def\fnum@ptablecont{{\centering{\scshape Table~\thetable}---{\itshape % Continued}}}% \def\tabletypesize#1{\def\table@hook{#1}\gdef\@table@type@size{#1}} \tabletypesize{\footnotesize} \let\tablefontsize=\tabletypesize % for compatibility with old documents % \long\def\@make@caption@text#1#2{% % {\small\centering#1{\scshape #2}\par\vskip1.4ex} % }% \long\def\@makecaption@plano@cont#1#2{% {\small \centering#1\par}\vskip1.4ex\relax }% %% Commands from aastex.cls: \newcommand\objectname{\@testopt\@objectname{[]}}% \def\@objectname[#1]#2{#2}% \newlength{\plot@width} \def\eps@scaling{1.0}% \newcommand\epsscale[1]{\def\eps@scaling{#1}}% \newcommand\plotone[1]{% \centering \leavevmode \setlength{\plot@width}{0.85\linewidth} \includegraphics[width={\eps@scaling\plot@width}]{#1}% }% \newcommand\plottwo[2]{% \centering \leavevmode \setlength{\plot@width}{0.425\linewidth} \includegraphics[width={\eps@scaling\plot@width}]{#1}% \hfil \includegraphics[width={\eps@scaling\plot@width}]{#2}% }% \newcommand\plotfiddle[7]{% \centering \leavevmode \vbox\@to#2{\rule{\z@}{#2}}% \includegraphics[% scale=#4, angle=#3, origin=c ]{#1}% }% \newcommand\figurenum[1]{% \def\thefigure{#1}% \let\@currentlabel\thefigure \addtocounter{figure}{\m@ne}% }% \newcommand\phn{\phantom{0}}% \newcommand\phd{\phantom{.}}% \newcommand\phs{\phantom{$-$}}% \newcommand\phm[1]{\phantom{#1}}% \let\la=\lesssim % For Springer A&A compliance... \let\ga=\gtrsim \newcommand\sq{\mbox{\rlap{$\sqcap$}$\sqcup$}}% \newcommand\arcdeg{\mbox{$^\circ$}}% \newcommand\arcmin{\mbox{$^\prime$}}% \newcommand\arcsec{\mbox{$^{\prime\prime}$}}% \newcommand\fd{\mbox{$.\!\!^{\mathrm d}$}}% \newcommand\fh{\mbox{$.\!\!^{\mathrm h}$}}% \newcommand\fm{\mbox{$.\!\!^{\mathrm m}$}}% \newcommand\fs{\mbox{$.\!\!^{\mathrm s}$}}% \newcommand\fdg{\mbox{$.\!\!^\circ$}}% \newcommand\farcm@mss{\mbox{$.\mkern-4mu^\prime$}}% \let\farcm\farcm@mss \newcommand\farcs@mss{\mbox{$.\!\!^{\prime\prime}$}}% \let\farcs\farcs@mss \newcommand\fp{\mbox{$.\!\!^{\scriptscriptstyle\mathrm p}$}}% \newcommand\micron{\mbox{$\mu$m}}% \def\farcm@apj{% \mbox{.\kern -0.7ex\raisebox{.9ex}{\scriptsize$\prime$}}% }% \def\farcs@apj{% \mbox{% \kern 0.13ex.% \kern -0.95ex\raisebox{.9ex}{\scriptsize$\prime\prime$}% \kern -0.1ex% }% }% \renewcommand\case[2]{\mbox{$\frac{#1}{#2}$}}% \renewcommand\slantfrac{\case}% \newcommand\onehalf{\slantfrac{1}{2}}% \newcommand\onethird{\slantfrac{1}{3}}% \newcommand\twothirds{\slantfrac{2}{3}}% \newcommand\onequarter{\slantfrac{1}{4}}% \newcommand\threequarters{\slantfrac{3}{4}}% \newcommand\ubvr{\mbox{$U\!BV\!R$}}%% UBVR system \newcommand\ub{\mbox{$U\!-\!B$}}% % U-B \newcommand\bv{\mbox{$B\!-\!V$}}% % B-V \renewcommand\vr{\mbox{$V\!-\!R$}}% % V-R \newcommand\ur{\mbox{$U\!-\!R$}}% % U-R \newcommand\ion[2]{#1$\;${\small\rmfamily\@Roman{#2}}\relax}% \newcommand\nodata{ ~$\cdots$~ }% \newcommand\diameter{\ooalign{\hfil/\hfil\crcr\mathhexbox20D}}% \newcommand\degr{\arcdeg}% \newcommand\Sun{\sun}% \newcommand\Sol{\sun}% \newcommand\sun{\odot}% \newcommand\Mercury{\astro{\char1}}% Mercury symbol, "1" \newcommand\Venus{\astro{\char2}}% Venus symbol, "2" \newcommand\Earth{\earth}% \newcommand\Terra{\earth}% \newcommand\earth{\oplus}% \newcommand\Mars{\astro{\char4}}% Mars symbol, "4" \newcommand\Jupiter{\astro{\char5}}% Jupiter symbol, "5" \newcommand\Saturn{\astro{\char6}}% Saturn symbol, "6" \newcommand\Uranus{\astro{\char7}}% Uranus symbol, "7" \newcommand\Neptune{\astro{\char8}}% Neptune symbol, "8" \newcommand\Pluto{\astro{\char9}}% Pluo symbol, "9" \newcommand\Moon{\astro{\char10}}% Moon symbol, "M" \newcommand\Luna{\Moon}% \newcommand\Aries{\astro{\char11}}% \newcommand\VEq{\Aries}% vernal equinox (Aries) \newcommand\Taurus{\astro{\char12}}% \newcommand\Gemini{\astro{\char13}}% \newcommand\Cancer{\astro{\char14}}% \newcommand\Leo{\astro{\char15}}% \newcommand\Virgo{\astro{\char16}}% \newcommand\Libra{\astro{\char17}}% \newcommand\AEq{\Libra}% autumnal equinox (Libra) \newcommand\Scorpius{\astro{\char18}}% \newcommand\Sagittarius{\astro{\char19}}% \newcommand\Capricornus{\astro{\char20}}% \newcommand\Aquarius{\astro{\char21}}% \newcommand\Pisces{\astro{\char22}}% \let\jnl@style=\rmfamily \def\ref@jnl#1{{\jnl@style#1}}% \newcommand\aj{\ref@jnl{AJ}}% % Astronomical Journal \newcommand\araa{\ref@jnl{ARA\&A}}% % Annual Review of Astron and Astrophys \renewcommand\apj{\ref@jnl{ApJ}}% % Astrophysical Journal \newcommand\apjl{\ref@jnl{ApJ}}% % Astrophysical Journal, Letters \newcommand\apjs{\ref@jnl{ApJS}}% % Astrophysical Journal, Supplement \renewcommand\ao{\ref@jnl{Appl.~Opt.}}% % Applied Optics \newcommand\apss{\ref@jnl{Ap\&SS}}% % Astrophysics and Space Science \newcommand\aap{\ref@jnl{A\&A}}% % Astronomy and Astrophysics \newcommand\aapr{\ref@jnl{A\&A~Rev.}}% % Astronomy and Astrophysics Reviews \newcommand\aaps{\ref@jnl{A\&AS}}% % Astronomy and Astrophysics, Supplement \newcommand\azh{\ref@jnl{AZh}}% % Astronomicheskii Zhurnal \newcommand\baas{\ref@jnl{BAAS}}% % Bulletin of the AAS \newcommand\jrasc{\ref@jnl{JRASC}}% % Journal of the RAS of Canada \newcommand\memras{\ref@jnl{MmRAS}}% % Memoirs of the RAS \newcommand\mnras{\ref@jnl{MNRAS}}% % Monthly Notices of the RAS \renewcommand\pra{\ref@jnl{Phys.~Rev.~A}}% % Physical Review A: General Physics \renewcommand\prb{\ref@jnl{Phys.~Rev.~B}}% % Physical Review B: Solid State \renewcommand\prc{\ref@jnl{Phys.~Rev.~C}}% % Physical Review C \renewcommand\prd{\ref@jnl{Phys.~Rev.~D}}% % Physical Review D \renewcommand\pre{\ref@jnl{Phys.~Rev.~E}}% % Physical Review E \renewcommand\prl{\ref@jnl{Phys.~Rev.~Lett.}}% % Physical Review Letters \newcommand\pasp{\ref@jnl{PASP}}% % Publications of the ASP \newcommand\pasj{\ref@jnl{PASJ}}% % Publications of the ASJ \newcommand\qjras{\ref@jnl{QJRAS}}% % Quarterly Journal of the RAS \newcommand\skytel{\ref@jnl{S\&T}}% % Sky and Telescope \newcommand\solphys{\ref@jnl{Sol.~Phys.}}% % Solar Physics \newcommand\sovast{\ref@jnl{Soviet~Ast.}}% % Soviet Astronomy \newcommand\ssr{\ref@jnl{Space~Sci.~Rev.}}% % Space Science Reviews \newcommand\zap{\ref@jnl{ZAp}}% % Zeitschrift fuer Astrophysik \renewcommand\nat{\ref@jnl{Nature}}% % Nature \newcommand\iaucirc{\ref@jnl{IAU~Circ.}}% % IAU Cirulars \newcommand\aplett{\ref@jnl{Astrophys.~Lett.}}% % Astrophysics Letters \newcommand\apspr{\ref@jnl{Astrophys.~Space~Phys.~Res.}}% % Astrophysics Space Physics Research \newcommand\bain{\ref@jnl{Bull.~Astron.~Inst.~Netherlands}}% % Bulletin Astronomical Institute of the Netherlands \newcommand\fcp{\ref@jnl{Fund.~Cosmic~Phys.}}% % Fundamental Cosmic Physics \newcommand\gca{\ref@jnl{Geochim.~Cosmochim.~Acta}}% % Geochimica Cosmochimica Acta \newcommand\grl{\ref@jnl{Geophys.~Res.~Lett.}}% % Geophysics Research Letters \renewcommand\jcp{\ref@jnl{J.~Chem.~Phys.}}% % Journal of Chemical Physics \newcommand\jgr{\ref@jnl{J.~Geophys.~Res.}}% % Journal of Geophysics Research \newcommand\jqsrt{\ref@jnl{J.~Quant.~Spec.~Radiat.~Transf.}}% % Journal of Quantitiative Spectroscopy and Radiative Trasfer \newcommand\memsai{\ref@jnl{Mem.~Soc.~Astron.~Italiana}}% % Mem. Societa Astronomica Italiana \newcommand\nphysa{\ref@jnl{Nucl.~Phys.~A}}% % Nuclear Physics A \newcommand\physrep{\ref@jnl{Phys.~Rep.}}% % Physics Reports \newcommand\physscr{\ref@jnl{Phys.~Scr}}% % Physica Scripta \newcommand\planss{\ref@jnl{Planet.~Space~Sci.}}% % Planetary Space Science \newcommand\procspie{\ref@jnl{Proc.~SPIE}}% % Proceedings of the SPIE \let\astap=\aap \let\apjlett=\apjl \let\apjsupp=\apjs \let\applopt=\ao \renewcommand\nodata{ ~$\cdots$~ }% \newcommand\ulap[1]{\vbox\@to\z@{{\vss#1}}}% \newcommand\dlap[1]{\vbox\@to\z@{{#1\vss}}}% \gdef\@tablecaption{} \def\tablecaption#1{\gdef\@tablecaption{#1}} % \newcommand\tablehead[1]{% % \gdef\pt@head{% % \hline\hline % \relax\\[-1.7ex]% % #1\hskip\tabcolsep % \\[.7ex]% % \hline % \relax\\[-1.5ex]% % }% % }% \def\LT@endpbox{% \@finalstrut\@arstrutbox \egroup \the\LT@p@ftn \global\LT@p@ftn{}% \hfil} \def\LT@makecaption#1#2#3{% \LT@mcol\LT@cols c{\hbox to\z@{\hss\parbox[t]\LTcapwidth{% \sbox\@tempboxa{#2.~~#3}% \ifdim\wd\@tempboxa>\hsize #2.~~#3% \else \hbox to\hsize{\hfil\box\@tempboxa\hfil}% \fi \endgraf\vskip\baselineskip}% \hss}}} \global\let\tablenotemark\relax \global\def\tablenotemark#1{\textsuperscript{\normalfont #1}} %\global\def\tablenotemark#1{\footnotemark[#1]} \global\let\tablenotetext\relax \global\def\tablenotetext#1#2{\footnotetext[#1]{#2}} \def\startdata{} \def\tablehead#1{ \kill \caption{\@tablecaption}\\ \hline \hline\\[-1.7ex] #1\hskip\tabcolsep\\[.7ex] \hline\\[-1.5ex] \endfirsthead \caption[]{\@tablecaption --- \emph{Continued}}\\ \hline \hline\\[-1.7ex] #1\hskip\tabcolsep\\[.7ex] \hline\\[-1.5ex] \endhead \hline \endfoot } \def\colhead#1{\multicolumn{1}{c}{#1}} \newenvironment{deluxetable}[1]{ \begin{table} \def\nl{\\} \def\tabcolsep{5pt} \let\caption=\LT@caption \begin{longtable}{#1} }{\gdef\pt@width{\LTcapwidth}\end{longtable}\@spew@tblnotes\end{table}} \newenvironment{deluxetable*}[1]{ \begin{table*} \def\nl{\\} \def\tabcolsep{5pt} \let\caption=\LT@caption \begin{minipage}{0.999\linewidth} \begin{longtable*}{#1} }{\gdef\pt@width{\LTcapwidth}\end{longtable*}\@spew@tblnotes% \end{minipage}% \end{table*}} \def\LongTables{ \renewenvironment{deluxetable}[1]{ % \def\table@hook{\@table@type@size} \def\nl{\\} \def\tabcolsep{5pt} \let\caption=\LT@caption \begin{longtable}{##1} }{\gdef\pt@width{\LTcapwidth}\end{longtable}\@spew@tblnotes} \renewenvironment{deluxetable*}[1]{ % \def\table@hook{\@table@type@size} \def\nl{\\} \def\tabcolsep{5pt} \let\caption=\LT@caption \begin{longtable*}{##1} }{\gdef\pt@width{\LTcapwidth}\end{longtable*}\@spew@tblnotes} } \def\tableheadfrac#1{} \def\tablewidth#1{} \newcount\pt@column \newcount\pt@ncol \newcommand\tablecolumns[1]{% \pt@column=#1\relax \pt@ncol=#1\relax \global\let\pt@addcol\@empty }% \def\cutinhead@ppt#1{% \noalign{\vskip 1.5ex}% \hline \@ptabularcr \noalign{\vskip -2ex}% Style Note: in apj, it is -1.5ex \multicolumn{\pt@ncol}{c}{#1}% \\ \noalign{\vskip .8ex}% \hline \\ \noalign{\vskip -2ex}% }% \newcommand\sidehead[1]{% \noalign{\vskip 1.5ex}% \multicolumn{\pt@ncol}{@{\hskip\z@}l}{#1}% \\ \noalign{\vskip .5ex}% }% %\def\startdata{\relax} \def\enddata{\relax} \gdef\tblnote@list{} \gdef\tblref@list{} \newcommand\tablecomments[1]{\gdef\tblnote@list{\@tablecom{#1}}}% \newcommand\tablerefs[1]{\gdef\tblref@list{\@tableref{#1}}}% \def\@tablecom#1{% \vspace*{\abovecaptionskip} \par {\parbox{\linewidth}{\hskip1em\rmfamily {\scshape Note}. --- #1}\par}% }% \def\@tableref#1{% \vspace*{\abovecaptionskip} \par {\parbox{\linewidth}{\hskip1em\rmfamily {\scshape References}. --- #1}\par}% }% \def\spew@tblnotes{% \@ifx@empty\tblref@list{}{% \@tablenotes{\tblref@list}% \global\let\tblref@list\@empty }% \@ifx@empty\tblnote@list{}{% \@tablenotes{\tblnote@list}% \global\let\tblnote@list\@empty } }% \def\@tablenotes#1{% \par \footnoterule% {\@table@type@size#1}% }% emulateapj.sty0100644000000000000000000011637010376206774012471 0ustar rootroot%% This is emulateapj.sty, version 8 Jan 1999 %% if this date looks old please check for a newer version at the site below. %% %% `emulateapj' is a LaTeX (2.09 or 2e) style to approximate the Astrophysical %% Journal (ApJ) page look. The length of the resulting document is close to %% that in ApJ if postscript Times fonts are used instead of the standard CM %% fonts (see below). `emulateapj' requires `multicol' package available %% from CTAN archives (www.ctan.org). %% %% The file emulateapj.sty is a modification of the AAS (American Astronomical %% Society) preprint style aaspp4.sty, including pieces of the TeX %% apjformat* by someone BLW. If a manuscript is prepared using the standard %% AAS macros used for the electronic manuscript submission, the only thing %% the user needs to do is to replace the style `aaspp4' with `emulateapj' in %% the first line of the document. We tried not to touch any of the nonobvious %% aaspp4 functionality to save trouble for users, so large parts of the code %% are probably useless, about which we did not care. %% %% The latest version of emulateapj.sty is available from %% http://hea-www.harvard.edu/~alexey/emulateapj/ %% To use Times postscript fonts, also use the accompanying file apjfonts.sty %% (at the site above, you can also pick up a package of font files). %% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% %% Solutions for some common problems: %% %% 1) Because `multicol' package cannot deal with floats of the width of the %% single column, footnotes, figures, tables etc. can only be set across two %% columns (that is, use `figure*' environment instead of `figure'.) %% Alternatively, insert figures as non-floats in the exact place of the text %% by hand. %% %% 2) There is a command \submitted{your text} to replace the default text %% in the upper left corner of the front page ("Draft version \today") with %% `your text'. Use it before the title commands. %% %% 3) There is a package option `onecolumn' (available only with LaTeX2e), %% \usepackage[onecolumn]{emulateapj}, which sets the whole paper in one %% column mode (as is done by the ApJ for papers with long equations). Even %% if the document is `onecolumn', `thebibliography' or `references' are %% typeset in two columns. %% %% 4) For users of `deluxetable': in LaTeX2e, the table font size cannot be %% reduced by simply putting a fontsize command inside the 'deluxetable' %% environment. To change the font size, \tablefontsize command is defined. %% To use, put e.g., \tablefontsize{\footnotesize} after \begin{deluxetable}. %% %% 5) The \title command makes the entire title text, even math, in upper %% case. If you wish to preserve the lower case in some portion of the %% title, use the \lowercase macro, e.g. \title{Upper case text %% \lowercase{$lower case$}} If you wish to suppress uppercasing in the %% entire title, redefine the \uppercase macro locally: %% {\let\uppercase\relax \title{The Title} } %% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% Copyright 1996-1999 Alexey Vikhlinin and Maxim Markevitch. %% For parts of the code, Copyright 1994 American Astronomical Society. %% %% This program can be redistributed and/or modified under the terms %% of the LaTeX Project Public License available from CTAN archives in %% directory macros/latex/base/lppl.txt. This means you are free to use and %% distribute this package; however, if you modify anything, please change the %% file name and remove the author's email addresses. %% %% Alexey Vikhlinin %% Maxim Markevitch %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% Changes: %% %% circa 96 (MM) original version %% 6.11.96 (AV) support for thebibliography added; also fix `tabular' %% 12.12.96 (AV) add command \submitted %% 10.01.97 (MM) raised title by 8mm, changed section spacing %% 24.01.97 (AV) fixed Appendix %% 24.02.97 (AV) fixed appendix interference with thebibliography %% 7.03.97 (AV) fixed small bug in appendix %% 16.03.97 (AV) changed definition of {references} and {thebibliography} %% to prohibit the page break between the reference section %% title and body and the split of a reference item across %% columns or pages. %% 25.06.97 (AV) put \end{multicols} before \end{document} if they were not %% closed by bibliography or appendix. %% 25.06.97 (AV) ``onecolumn'' option: \usepackage[onecolumn]{emulateapj} %% 15.09.97 (AV) \tablefontsize for plano table to change the font size %% throughout the table %% 15.09.97 (AV) (suggested by Joern Wilms wilms@astro.uni-tuebingen.de) %% redefine \figcapion to type the caption text in \footnotesize %% and change fnum@figure to type Fig.XXX in \sc %% 15.09.97 (AV) define \tabcation which makes it possible to typeset %% non-floating tables. %% 21.10.97 (AV) fix \keywords for long keyword lists. %% 24.10.97 (AV) make title width = abstract %% 10.12.97 (AV) prohibit hyphenation in the references %% 10.12.97 (AV) make author list width = 0.9abstract %% 28.02.98 (AV) define textheight equal to the whole number of lines. %% 06.03.98 (AV) fix @firstsection in definition of \section %% 11.05.98 (AV) A sectioning command definition was changed for Apr 4, 98 %% version, which introduced a bug in labeling mechanism. It %% is fixed now. %% 19.05.98 (AV) \frenchspacing inside references and thebibliography %% 24.11.98 (AV) \caption{...} produces the right output for both tables and %% and figures without the need of font changes and explicit %% alignments. %% 22.12.98 (AV) Captions are put inside minipage so that in non-floating %% mode, they will not split across pages or columns. %% 9.01.99 (AV) Fixed spurious spacing after \makecaption. %% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \@ifundefined{documentclass}{ % non-latex2e: \input{multicol.sty}\let\scshape=\sc% \@ifundefined{epsfbox}{\@input{epsf.sty}}{\relax}} {\RequirePackage{multicol,epsf,graphicx}\ProvidesPackage{emulateapj}} % **************************************************** % * TWO AND SINGLE COLUMN STYLES: AV * % **************************************************** % % I define `slocitlum' which is \relax if onecolumn option is chosen or % plain multicols if twocolumn (default option); `slocitlum' is used % everywhere except for `thebibliography' and `references' which should be % always set in two columns. % \newenvironment{slocitlum}[1]{\relax}{\relax} \@ifundefined{documentclass}{ % non-latex2e: \renewenvironment{slocitlum}[1]{\begin{multicols}{#1}}{\end{multicols}} } { % LaTeX2e; use package option mechanism \DeclareOption{twocolumn}{ \renewenvironment{slocitlum}[1]{\begin{multicols}{#1}}{\end{multicols}} } \DeclareOption{onecolumn}{ \renewenvironment{slocitlum}[1]{\relax}{\relax} } \ExecuteOptions{twocolumn} \ProcessOptions } %%%%% include atbeginend.sty by AV: % Copy \begin and \end to \BeginEnvironment and \EndEnvironment \let\BeginEnvironment=\begin \let\EndEnvironment=\end %% \ifundefined from TeXbook \def\IfUnDef#1{\expandafter\ifx\csname#1\endcsname\relax} % Null command needed to eat its argument \def\NullCom#1{} \def\begin#1{% % if defined \BeforeBeg for this environment, execute it \IfUnDef{BeforeBeg#1}\else\csname BeforeBeg#1\endcsname\fi% \IfUnDef{AfterBeg#1}% This is done to skip the command for environments % which can take arguments, like multicols; YOU MUST NOT % USE \AfterBegin{...}{...} for such environments! \let\SaveBegEnd=\BeginEnvironment% \else % Start this environment \BeginEnvironment{#1}% % and execute code after \begin{environment} \csname AfterBeg#1\endcsname \let\SaveBegEnd=\NullCom \fi \SaveBegEnd{#1} } \def\end#1{% % execute code before \end{environment} \IfUnDef{BeforeEnd#1}\else\csname BeforeEnd#1\endcsname\fi% % close this environment \EndEnvironment{#1} % and execute code after \begin{environment} \IfUnDef{AfterEnd#1}\else\csname AfterEnd#1\endcsname\fi% } \def\BeforeBegin#1#2{\expandafter\gdef\csname BeforeBeg#1\endcsname {#2}} \def\BeforeEnd #1#2{\expandafter\gdef\csname BeforeEnd#1\endcsname {#2}} \def\AfterBegin #1#2{\expandafter\gdef\csname AfterBeg#1\endcsname {#2}} \def\AfterEnd #1#2{\expandafter\gdef\csname AfterEnd#1\endcsname{#2}} %%%% end of atbeginend.sty \def\revtex@ver{4.0} % Version number of this file. \def\revtex@date{25 Apr 95} % Revision date. \def\revtex@org{AAS} % Sponsoring organization. \def\revtex@jnl{AAS} % Applicable journal, if specific. \def\revtex@genre{emulateapj} % Document "type". %aas % Display identifying message on screen and in logfile. %aas \typeout{\revtex@org\space \revtex@genre\space substyle, %aas v\revtex@ver\space <\revtex@date>.} % **************************************** % * PAGE LAYOUT * % **************************************** % Page size, spacing parameters, etc. %% (MM) for ApJ approx, using Times-Roman 10pt font: \textwidth=18.55cm \columnsep=8.5mm \parindent=3.5mm \voffset=-20mm \hoffset=-9mm \newlength{\abstrwidth} \abstrwidth=15.9cm \topmargin=0in \headheight=.15in \headsep=0.5in \oddsidemargin=0in \evensidemargin=0in \parskip=0cm \tolerance=600 % 3x "normal" value; cuts down on overfull complaints \def\@tightleading{1.1} \def\@doubleleading{1.6} %% AV,MM, to have 63 lines per column, with textheight 25cm: \def\baselinestretch{0.92} \textheight=24.4cm \textheight=63\baselineskip \textheight=\baselinestretch\textheight \ifdim\textheight>24.6cm\textheight=24.4cm\fi \let\tighten=\relax \let\tightenlines=\tighten \let\singlespace=\relax \let\doublespace=\relax \def\eqsecnum{ \@newctr{equation}[section] \def\theequation{\hbox{\normalsize\arabic{section}-\arabic{equation}}}} \def\@journalname{The Astrophysical Journal} \def\cpr@holder{American Astronomical Society} \def\received#1{\gdef\@recvdate{#1}} \received{} \def\accepted#1{\gdef\@accptdate{#1}} \accepted{} \def\revised#1{\gdef\@revisedate{#1}} \revised{} \def\journalid#1#2{\gdef\@jourvol{#1}\gdef\@jourdate{#2}} \def\articleid#1#2{\gdef\@startpage{#1}\gdef\@finishpage{#2}} \def\paperid#1{\gdef\@paperid{#1}} \paperid{MS-0001-SAMP} \def\ccc#1{\gdef\CCC@code{#1}} \ccc{000-00\$75.95-CDB} \def\cpright#1#2{\@nameuse{cpr@#1} \gdef\cpr@year{#2} \typeout{`#1' copyright \cpr@year.}} \newcount\@cprtype \@cprtype=\@ne % Default copyright type. \def\cpr@AAS{\@cprtype=1} \def\cpr@PD{\@cprtype=2} \def\cpr@Crown{\@cprtype=3} \def\cpr@none{\@cprtype=4} \def\cpr@ASP{\@cprtype=5} \def\cpr@year{\number\year} % Default copyright year. \def\@slug{\par\noindent \ifcase\@cprtype \relax \or Copyright \cpr@year\space by the \cpr@holder. \or This article is in the public domain. \or Crown copyright \cpr@year\space by the \cpr@holder. \or No copyright is claimed for this article. \or Copyright \cpr@year\space by the ASP. \fi \par\noindent Manuscript number \@paperid.\par\noindent \CCC@code } %% running heads: \def\lefthead#1{\gdef\@versohead{#1}} \lefthead{\relax} \def\righthead#1{\gdef\@rectohead{#1}} \righthead{\relax} %% MM Create "apjheads" page style: \def\ps@apjheads{\let\@mkboth\markboth \def\@evenfoot{} \def\@evenhead{\lower9mm\hbox to\textwidth{ \rm\thepage\hfil \rm\@rectohead \hfil}}} \def\@oddfoot{} \def\@oddhead{\lower9mm\hbox to\textwidth{ \hfil\rm\@versohead\hfil \rm\thepage}} \@twosidetrue \ps@apjheads % \@runheads determines formatting of running head information. \def\@runheads{\@tempcnta\c@page \@whilenum \@tempcnta >0\do{ \vskip 3ex \hbox to30pc{\small\expandafter\uppercase\expandafter{\@versohead}: \expandafter\uppercase\expandafter{\@rectohead}\hfil} \advance\@tempcnta by\m@ne} } \def\slugcomment#1{\gdef\slug@comment{#1}} \slugcomment{} \newdimen\@slugcmmntwidth \@slugcmmntwidth .67\textwidth \long\def\@makeslugcmmnt{\ifx\slug@comment\@empty\relax\else \setbox\@tempboxa\hbox{\slug@comment} \ifdim \wd\@tempboxa >\@slugcmmntwidth \hbox to\textwidth{\hss \parbox\@slugcmmntwidth\slug@comment} \else \hbox to\textwidth{\hfil\box\@tempboxa} \fi \vskip 2ex \fi} \def\@rcvaccrule{\vrule\@width1.75in\@height0.5pt\@depth\z@} \def\@dates{{\center\if@twocolumn\small\else\normalsize\fi% {\it Received}\space% \ifx\@empty\@recvdate\@rcvaccrule\else\@recvdate\fi;% \if@twocolumn\\[.5ex]\else\hspace{1.5em}\fi% {\it accepted}\space% \ifx\@empty\@accptdate\@rcvaccrule\else\@accptdate\fi% \endcenter} } \def\sluginfo{{\center \@dates %\@slug %\@runheads \endcenter}} \let\dates=\sluginfo % Backwards compatibility % **************************************** % * FRONT MATTER * % **************************************** %% AV renewed \@ifundefined{documentclass}{ % non-latex2e: \let\abstract\relax \let\endabstract\relax \def\abstract{\bgroup\center\minipage{\abstrwidth} \vspace{2pt}\centerline{ABSTRACT} \vspace{3pt} \parindent=3.5mm} \def\endabstract{\endminipage \endcenter \egroup} } {% LaTeX 2e definition \renewenvironment{abstract}[0]{\center \begin{minipage}{\abstrwidth} \vspace{2pt} \centerline{ABSTRACT} \vspace{3pt} \parindent=3.5mm} {\end{minipage}\endcenter} } \BeforeBegin{abstract}{\centerline{\small\it{\@submitted}}} %% MM %% "apjbot" for the title page: \def\ps@apjbot{ \def\@oddfoot{\raise7mm\hbox to\textwidth{\hfil\rm\thepage\hfil}} \def\@oddhead{}} \def\title#1{{\thispagestyle{apjbot} \subtitle \vspace{12mm} \center \begin{minipage}{\abstrwidth} \center\uppercase{#1}\endcenter \end{minipage}\endcenter}} \def\author#1{ \vspace*{-1.5ex}% {\topsep 3pt \center \begin{minipage}{0.9\abstrwidth}\center\small\scshape#1\endcenter\end{minipage} \endcenter } \vspace*{-1pt}} \let\authoraddr=\@gobble \let\authoremail=\@gobble \def\affil#1{\vspace*{-0.8ex}{\topsep 0pt\center \begin{minipage}{0.9\abstrwidth}\center\footnotesize% \def\baselinestretch{1.0}% #1\endcenter\end{minipage} \endcenter}} \def\altaffilmark#1{$^{#1}$} \def\altaffiltext#1#2{\footnotetext[#1]{#2}\stepcounter{footnote}} % Redefine the LaTeX \and command for this style. %% MM \def\and{\vspace{0pt}{\topsep\z@\center {\sc and}\endcenter}\vspace{3pt}} % **************************************** % * KEYWORDS * % **************************************** \def\@keywordtext{Subject headings} \def\@keyworddelim{---} %% MM,AV \newlength{\kwdtextwidth} \settowidth{\kwdtextwidth}{{\it\@keywordtext:\/}} \def\keywords#1{\begin{center} \begin{minipage}{\abstrwidth} \vspace*{-6pt}\raggedright \par\hangindent=\kwdtextwidth\hangafter=1 \noindent {\it\@keywordtext:\/}\space #1 \end{minipage} \end{center}} \let\subjectheadings=\keywords \def\@kwds#1{#1\relax} % **************************************** % * FOOTNOTES * % **************************************** %% MM \skip\footins 2mm \footnotesep 2ex \let\footnoterule\relax \def\notetoeditor#1{}% % **************************************** % * SECTIONS * % **************************************** \newif\if@firstsection \@firstsectiontrue %% MM: section vertical indents by eye: \def\section{% \if@firstsection\@firstsectionfalse\begin{slocitlum}{2}\fi% \@startsection{section}{1}{\z@}{10pt plus 2pt minus 1pt}{5pt}{\footnotesize \center}} \def\subsection{\@startsection{subsection}{2}{\z@}{5pt plus 1pt minus 1pt}{5pt}% {\normalsize\it \center}} \def\subsubsection{\@startsection{subsubsection}{3}{\z@}% {2ex plus 1ex minus .2ex}{1ex plus .2ex}{\normalsize\it \center}} \def\thesection{\@arabic{\c@section}} \def\thesubsection{\thesection.\@arabic{\c@subsection}} \def\thesubsubsection{\thesubsection.\@arabic{\c@subsubsection}} \def\theparagraph{\thesubsubsection.\@arabic{\c@paragraph}} \def\sec@upcase#1{\uppercase{#1}} \def\subsec@upcase#1{\relax{#1}} \def\secnum@size{\small} \def\subsecnum@size{\normalsize} % % How the section number will appear in the section title - AV \def\ApjSectionMarkInTitle#1{#1.\ } \def\@sect#1#2#3#4#5#6[#7]#8% {\@tempskipa #5\relax \ifdim \@tempskipa >\z@ \begingroup #6\relax \ifnum #2>\c@secnumdepth \def \@svsec {}\else \refstepcounter{#1} \edef \@svsec {\ApjSectionMarkInTitle {\csname the#1\endcsname}}\fi \@hangfrom {\hskip #3\relax \ifnum #2=1\secnum@size {\rm\@svsec~}% \else \subsecnum@size {\rm\@svsec~}\fi }% {\interlinepenalty \@M \ifnum #2=1\sec@upcase{#8}% \else \subsec@upcase{#8}\fi\par}\endgroup \csname #1mark\endcsname {#7}\addcontentsline{toc}{#1}% {\ifnum #2>\c@secnumdepth \else \protect \numberline {\csname the#1\endcsname }\fi #7}% \else \ifnum #2>\c@secnumdepth \def \@svsec {}\else \refstepcounter{#1} \edef \@svsec {\ApjSectionMarkInTitle {\csname the#1\endcsname}}\fi \def \@svsechd {#6\hskip #3% \ifnum #2=1\secnum@size{\rm\@svsec~}\else\subsecnum@size{\rm\@svsec~}\fi% \ifnum #2=1\sec@upcase{#8}\else\subsec@upcase{#8}\fi% \csname #1mark\endcsname {#7}\addcontentsline{toc}{#1}% {\ifnum #2>\c@secnumdepth \else \protect \numberline {\csname the#1\endcsname }\fi #7}}\fi \@xsect {#5} \penalty 0 %-refstepcounter is now within a group. So \@currentlabel, which is normally %-set by \refstepcounter is hidden within a group. Need to set it manually. \protected@edef\@currentlabel{\csname p@#1\endcsname\csname the#1\endcsname} } % \def\@sect#1#2#3#4#5#6[#7]#8{% % \ifnum #2>\c@secnumdepth % \def\@svsec{}\else % % \refstepcounter{#1}\edef\@svsec{\csname the#1\endcsname.\ }\fi % \refstepcounter{#1}\edef\@svsec{\ApjSectionMarkInTitle{\csname the#1\endcsname}}\fi % \@tempskipa #5\relax % \ifdim \@tempskipa>\z@ % \begingroup #6\relax % \@hangfrom{\hskip #3\relax% % \ifnum#2=1\secnum@size{\rm\@svsec} % \else\subsecnum@size{\rm\@svsec~}\fi% % }{\interlinepenalty \@M % \ifnum#2=1\sec@upcase{#8}\else\subsec@upcase{#8}\fi\par}% % \endgroup % \csname #1mark\endcsname{#7}\addcontentsline % {toc}{#1}{\ifnum #2>\c@secnumdepth \else % \protect\numberline{\csname the#1\endcsname}\fi % #7}\else % \def\@svsechd{#6\hskip #3\@svsec \sec@upcase{#8}\csname #1mark\endcsname % {#7}\addcontentsline % {toc}{#1}{\ifnum #2>\c@secnumdepth \else % \protect\numberline{\csname the#1\endcsname}\fi % #7}}\fi % \@xsect{#5} % % MM: % \penalty 0} \def\@ssect#1#2#3#4#5{\@tempskipa #3\relax \ifdim \@tempskipa>\z@ \begingroup #4\@hangfrom{\hskip #1}{\interlinepenalty \@M \sec@upcase{#5}\par}\endgroup \else \def\@svsechd{#4\hskip #1\relax \sec@upcase{#5}}\fi \@xsect{#3} % MM: \penalty 0} \def\acknowledgments{\vskip 3ex plus .8ex minus .4ex} \let\acknowledgements=\acknowledgments % second spelling % **************************************** % * APPENDIX * % **************************************** \def\NoApjSectionMarkInTitle#1{\relax} \renewenvironment{appendix}[0]{ \if\inmulticols\inmulticolstest\end{slocitlum}\fi \vskip 10pt plus 2pt minus 1pt \centerline{\small APPENDIX} \@firstsectionfalse \setcounter{section}{0} \setcounter{subsection}{0} \setcounter{equation}{0} % \setcounter{figure}{0} % \setcounter{table}{0} % \def\fnum@figure{Figure \Alph{section}\thefigure:} % \def\fnum@table{Table \Alph{section}\thetable:} \def\thesection{\Alph{section}} % \def\theequation{\hbox{\normalsize\Alph{section}\arabic{equation}}} % % The following command causes LaTeX 2e to overflow its parameter stack. If % TeX is rebuilt with a larger parameter stack, this can be corrected: remove % the three lines below and uncomment the line above. % \@ifundefined{documentclass} {\def\theequation{\normalsize\hbox{\Alph{section}\arabic{equation}}}} {\def\theequation{\hbox{\Alph{section}\arabic{equation}}}} \def\thefigure{\thesection\@arabic\c@figure} \def\thetable{\thesection\@arabic\c@table} % % Do not use appendix numbers in the titles \def\ApjSectionMarkInTitle{\NoApjSectionMarkInTitle} \def\section{\setcounter{equation}{0}\@startsection {section}{1}{\z@} {10pt}{5pt}{\centering\small}} }{} \BeforeBegin{appendix}{\if\inmulticols\inmulticolstest\end{slocitlum}} % **************************************** % * EQUATION NUMBERING * % **************************************** \newcounter{cureqno} \newenvironment{mathletters}{\refstepcounter{equation}% \setcounter{cureqno}{\value{equation}}% \let\@curtheeqn\theequation% \edef\cur@eqn{\theequation}% \def\theequation{\cur@eqn\alph{equation}}% \setcounter{equation}{0}}% {\let\theequation\@curtheeqn% \setcounter{equation}{\value{cureqno}}} \def\eqnum#1{\def\theequation{#1}\let\@currentlabel\theequation \addtocounter{equation}{\m@ne}} % **************************************** % * BIBLIOGRAPHY * % **************************************** \newenvironment{references}[0]{ \vspace{3pt plus 3pt} % \hbox to \textwidth{\centerline{\footnotesize REFERENCES}} % \vspace{-5pt} \begin{multicols}{2}[\hbox to \textwidth{\centerline{\footnotesize REFERENCES}} \vspace{-5pt}] \parindent=0cm \parskip=0cm \footnotesize \baselineskip=8pt \interlinepenalty \@M \hyphenpenalty=10000 \frenchspacing % AV - to get right spacing after ``et al.'' \def\refpar{\par\hangindent=1.2em\hangafter=1}} {\end{multicols}} % redefine thebibliography \renewenvironment{thebibliography}[1]{ \vspace{3pt plus 3 pt} % AV \begin{multicols}{2}[\hbox % AV to \textwidth{\centerline{\footnotesize % AV REFERENCES}} \vspace{-5pt}] % AV \list{ \@biblabel{\@arabic\c@enumiv}}% { \@openbib@code \parindent=0pt \parskip=0pt \parsep=0pt % AV \bibindent=0pt % \footnotesize \baselineskip=8pt \interlinepenalty \@M % AV \frenchspacing % AV - to get right spacing after ``et al.'' \hyphenpenalty=10000 \itemindent=-1.0em % \itemsep=0pt % \listparindent=0pt % \settowidth\labelwidth{\@biblabel{#1}} % \labelsep=0pt % \leftmargin=1.0em \advance\leftmargin\labelsep \usecounter{enumiv}% \let\p@enumiv\@empty \renewcommand\theenumiv{\@arabic\c@enumiv}}% \sloppy\clubpenalty4000\widowpenalty4000% \sfcode`\.\@m} {\def\@noitemerr {\@latex@warning{Empty `thebibliography' environment}}% \endlist\if\inmulticols\inmulticolstest\end{multicols}\fi} % %% AV: \def\inmulticols{0} \def\inmulticolstest{1} \BeforeBegin{multicols}{\def\inmulticols{1}} \AfterEnd{multicols}{\def\inmulticols{0}} \BeforeBegin{slocitlum}{\def\inmulticols{1}} \AfterEnd{slocitlum}{\def\inmulticols{0}} \BeforeBegin{references}{\if\inmulticols\inmulticolstest\end{slocitlum}% \else\vspace{10pt}\fi} \BeforeBegin{thebibliography}{\if\inmulticols\inmulticolstest\end{slocitlum}% \else\vspace{10pt}\fi} \BeforeEnd{document}{\if\inmulticols\inmulticolstest\end{slocitlum}\fi} %aas \subsection*{\small REFERENCES} %aas \list{\null}{\leftmargin 1.2em\labelwidth\z@\labelsep\z@\itemindent -1.2em %aas \usecounter{enumi}} %aas \def\refpar{\relax} %aas \def\newblock{\hskip .11em plus .33em minus .07em} %aas \sloppy\clubpenalty4000\widowpenalty4000 %aas \sfcode`\.=1000\relax} %aas \def\endthebibliography{\endlist\revtex@pageid} \def\@biblabel#1{\relax} %\def\@cite#1#2{({#1\if@tempswa , #2\fi})} \def\@cite#1#2{#1\if@tempswa , #2\fi} \def\reference{\@ifnextchar\bgroup {\@reference} {\@latexerr{Missing key on reference command} {Each reference command should have a key corresponding to a markcite somewhere in the text}}} \def\@reference#1{\relax\refpar} \def\markcite{\@ifnextchar\bgroup{\@markcite} {\@latexerr{Missing key on markcite command} {Each markcite command should have a key corresponding to a reference somewhere in the references section}}} \def\@markcite#1{\relax} \def\@citex[#1]#2{\if@filesw\immediate\write\@auxout{\string\citation{#2}}\fi \def\@citea{}\@cite{\@for\@citeb:=#2\do {\@citea\def\@citea{,\penalty\@m\ }\@ifundefined {b@\@citeb}{\@warning {Citation `\@citeb' on page \thepage \space undefined}}% {\csname b@\@citeb\endcsname}}}{#1}} %% subtitle header: \def\submitted#1{\gdef\@submitted{#1}} \def\subtitle{ \vspace*{-12mm} \noindent {\scriptsize {\sc \@submitted} \\ Preprint typeset using \LaTeX\ style emulateapj} } \let\slugcomment\submitted % slugcomment == submitted \submitted{Draft version \today} %% AV: allow figures to take the whole page \renewcommand{\topfraction}{1.0} \renewcommand{\bottomfraction}{1.0} \renewcommand{\textfraction}{0.0} % **************************************** % * TABLES AND FIGURES * % **************************************** \setcounter{topnumber}{7} \def\tablenotemark#1{\rlap{$^{\rm #1}$}} \newtoks\@temptokenb \def\tblnote@list{} \def\tablenotetext#1#2{ \@temptokena={\vspace{.5ex}{\noindent\llap{$^{#1}$}#2}\par} \@temptokenb=\expandafter{\tblnote@list} \xdef\tblnote@list{\the\@temptokenb\the\@temptokena}} \def\spew@tblnotes{ \ifx\tblnote@list\@empty\relax \else \vspace{3.2ex} \footnoterule \vspace{.4ex} {\footnotesize\tblnote@list} \gdef\tblnote@list{} \fi} \def\endtable{\spew@tblnotes\end@float} \@namedef{endtable*}{\spew@tblnotes\end@dblfloat} \let\tableline=\hline %\long\def\@makecaption#1#2{\vskip 2ex\noindent #1 #2\par} \setlength{\belowcaptionskip}{0pt} \setlength{\abovecaptionskip}{5pt} \long\def\@makecaption#1#2{% \noindent\begin{minipage}{0.99\linewidth} %% \noindent is needed because %% otherwise minipage + parindent does not fit into the line and spurious %% vertical skip appear after caption \if\csname ftype@\@captype\endcsname 2 \vskip 2ex\noindent \centering\small\sc #1 #2\par\medskip \else \vskip \abovecaptionskip\footnotesize\noindent #1 #2\par\vskip \belowcaptionskip \fi \end{minipage} } \def\tablenum#1{\def\thetable{#1}\let\@currentlabel\thetable \addtocounter{table}{\m@ne}} \def\figurenum#1{\def\thefigure{#1}\let\@currentlabel\thefigure \addtocounter{figure}{\m@ne}} \let\placetable=\@gobble \let\placefigure=\@gobble \let\placeplate=\@gobble \def\figcaption{\@ifnextchar[{\@xfigcaption}{\@figcaption}} % \def\@figcaption#1{{\def\@captype{figure}\caption{#1}}} % \def\@xfigcaption[#1]#2{{\def\@captype{figure}\caption{#2}}} %% suggested by Joern Wilms wilms@astro.uni-tuebingen.de %% wilms@rocinante.colorado.edu \def\@figcaption#1{{\def\@captype{figure}\caption{\footnotesize #1}}} \def\@xfigcaption[#1]#2{{\def\@captype{figure}\caption{\footnotesize #2}}} \def\dummytable{\refstepcounter{table}} %%%% %%%% the code below is unchanged from aaspp4.sty: %%%% % **************************************** % * PLANO TABLES * % **************************************** \newbox\pt@box \newdimen\pt@width \newcount\pt@line \newcount\pt@column \newcount\pt@nlines \newcount\pt@ncol \newcount\pt@page \def\colhead#1{\multicolumn{1}{c}{#1}\pt@addcol} \def\tablecolumns#1{\pt@column=#1\pt@ncol=#1\gdef\pt@addcol{\relax}} \def\tablecaption#1{\gdef\pt@caption{#1}} \def\pt@caption{\relax} \def\tablehead#1{\gdef\pt@head{\hline\hline\relax\\[-1.7ex] #1\hskip\tabcolsep\\[.7ex]\hline\relax\\[-1.5ex]}} \def\pt@head{\relax} \def\tabletail#1{\gdef\pt@tail{#1}} \def\pt@tail{\relax} \def\tablewidth#1{\pt@width=#1} \pt@width\textwidth \def\tableheadfrac#1{\gdef\pt@headfrac{#1}} \def\pt@headfrac{.1} \def\tablefontsize#1{\gdef\pt@fontsize{#1}} \def\pt@fontsize{\relax} \def\pt@calcnlines{\@tempdima\pt@headfrac\textheight \@tempdimb\textheight\advance\@tempdimb by-\@tempdima \@tempdima\arraystretch\baselineskip \divide\@tempdimb by\@tempdima \global\pt@nlines\@tempdimb} \def\pt@tabular{\hbox \bgroup \pt@fontsize $\let\@acol\@ptabacol \let\@classz\@tabclassz \let\@classiv\@tabclassiv \let\\\@tabularcr\@tabarray} \def\@ptabacol{\edef\@preamble{\@preamble \hskip \tabcolsep\tabskip\fill}} \def\fnum@ptable{Table \thetable} \def\fnum@ptablecont{Table \thetable---{\it Continued}} \newdimen\pt@tmpcapwidth \def\set@mkcaption{\long\def\@makecaption##1##2{\ifdim\pt@width>\z@% \pt@tmpcapwidth\pt@width\else\pt@tmpcapwidth\textwidth\fi% \center\parbox{\pt@tmpcapwidth}{\center\sc##1\\[.5ex]##2\endcenter}% \endcenter}} %\def\set@mkcaption{\long\def\@makecaption##1##2{ % \center\sc##1\\[.5ex]##2\endcenter\vskip 1.5ex}} \def\set@mkcaptioncont{\long\def\@makecaption##1##2{ \center\sc##1\endcenter\vskip 1.5ex}} \newenvironment{deluxetable}[1]{\def\pt@format{\string#1}% \set@tblnotetext\global\pt@ncol=0\global\pt@column=0\global\pt@page=1% \def\pt@addcol{\global\advance\pt@ncol by\@ne}}% {%\crcr\noalign{\vskip .7ex}\hline\endtabular% \pt@width\wd\pt@box\box\pt@box\spew@ptblnotes% \typeout{Page \the\pt@page\space of table \thetable\space has been set to width \the\pt@width\space with \the\pt@nlines\space lines per page}% \endcenter\end@dblfloat} \let\planotable=\deluxetable \let\endplanotable=\enddeluxetable \def\startdata{\pt@line=0\pt@calcnlines% \ifdim\pt@width>\z@\def\@halignto{to \pt@width}\else\def\@halignto{}\fi% \let\fnum@table=\fnum@ptable\set@mkcaption% \@dblfloat{table}\center\caption{\pt@caption}\leavevmode% \setbox\pt@box=\pt@tabular{\pt@format}\pt@head} \def\enddata{\crcr\noalign{\vskip .7ex}\hline\endtabular} \def\pt@nl{\global\advance\pt@line by\@ne% \ifnum\pt@line=\pt@nlines% \endtabular\pt@width\wd\pt@box\box\pt@box \typeout{Page \the\pt@page\space of table \thetable\space has been set to width \the\pt@width}% \global\advance\pt@page by\@ne% \endcenter\end@dblfloat\clearpage% \addtocounter{table}{\m@ne}% \let\fnum@table=\fnum@ptablecont\set@mkcaptioncont% \@dblfloat{table}\center\caption{\pt@caption}\leavevmode% \global\pt@ncol=\pt@column% Either 0 or value of \tablecolumns \global\pt@line=0% \setbox\pt@box=\pt@tabular{\pt@format}\pt@head% \else\\ \fi} \let\nl=\pt@nl \let\nextline=\pt@nl \def\tablevspace#1{\noalign{\vskip#1}} \def\tablebreak{\pt@line\pt@nlines\advance\pt@line by\m@ne\pt@nl} \def\cutinhead#1{\noalign{\vskip 1.5ex} \hline\pt@nl\noalign{\vskip -2.0ex} \multicolumn{\pt@ncol}{c}{#1}\pt@nl \noalign{\vskip .8ex} \hline\pt@nl\noalign{\vskip -2ex}} \def\sidehead#1{\noalign{\vskip 1.5ex} \multicolumn{\pt@ncol}{@{\hskip\z@}l}{#1}\pt@nl \noalign{\vskip .5ex}} \def\set@tblnotetext{\def\tablenotetext##1##2{{% \@temptokena={{\parbox{\pt@width}{\hskip1em$^{\rm ##1}$##2}}\par}% \@temptokenb=\expandafter{\tblnote@list} \xdef\tblnote@list{\the\@temptokenb\the\@temptokena}}}} \def\spew@ptblnotes{ \ifx\tblnote@list\@empty\relax \else \par \vspace{2ex} {\parskip=1.5ex% \tblnote@list} \gdef\tblnote@list{} \fi} \def\tablerefs#1{\@temptokena={\vspace*{3ex}{% \parbox{\pt@width}{\hskip1em{\sc References.---}#1}\par}}% \@temptokenb=\expandafter{\tblnote@list} \xdef\tblnote@list{\the\@temptokenb\the\@temptokena}} \def\tablecomments#1{\pt@fontsize\@temptokena={\vspace*{3ex}{% \parbox{\pt@width}{\hskip1em{\sc Note.---}#1}\par}}% \@temptokenb=\expandafter{\tblnote@list} \xdef\tblnote@list{\the\@temptokenb\the\@temptokena}} % **************************************** % * FIGURE, TABLE, PLATE PARAMETERS * % **************************************** \newcounter{plate} \def\theplate{\@arabic\c@plate} \def\fps@plate{bp} \def\ftype@plate{4} % Yes. This must a power of 2. \def\ext@plate{lof} % Put plates in LOF. \def\fnum@plate{{\bf Plate \theplate.}} \def\plate{\@float{plate}} \let\endplate\end@float \@namedef{plate*}{\@dblfloat{plate}} \@namedef{endplate*}{\end@dblfloat} \let\platewidth=\tablewidth \def\platenum#1{\def\theplate{#1}\let\@currentlabel\theplate \addtocounter{plate}{\m@ne}} \def\thefigure{\@arabic\c@figure} \def\fnum@figure{{\footnotesize\sc ~~Fig.\space\thefigure.---}} \def\thetable{\@arabic\c@table} %%% Table captions without making a floating table \def\tabcaption{\@ifnextchar[{\@xtabcaption}{\@tabcaption}} \def\@tabcaption#1{{\def\@captype{table}\caption{#1}}} \def\@xtabcaption[#1]#2{{\def\@captype{table}\caption{#2}}} \def\fnum@table{{\centering{\sc Table~\thetable}\vskip0.7ex}} \def\fps@figure{bp} \def\fps@table{bp} % **************************************** % * EPS INCLUSIONS * % **************************************** \def\eps@scaling{.95} \def\epsscale#1{\gdef\eps@scaling{#1}} \def\plotone#1{\centering \leavevmode \epsfxsize=\eps@scaling\columnwidth \epsfbox{#1}} \def\plottwo#1#2{\centering \leavevmode \epsfxsize=.45\columnwidth \epsfbox{#1} \hfil \epsfxsize=.45\columnwidth \epsfbox{#2}} \def\plotfiddle#1#2#3#4#5#6#7{\centering \leavevmode \vbox to#2{\rule{0pt}{#2}} \special{psfile=#1 voffset=#7 hoffset=#6 vscale=#5 hscale=#4 angle=#3}} % **************************************** % * ABBREVIATIONS * % **************************************** \let\jnl@style=\rm \def\ref@jnl#1{{\jnl@style#1}} \def\aj{\ref@jnl{AJ}} % Astronomical Journal \def\araa{\ref@jnl{ARA\&A}} % Annual Review of Astron and Astrophys \def\apj{\ref@jnl{ApJ}} % Astrophysical Journal \def\apjl{\ref@jnl{ApJ}} % Astrophysical Journal, Letters \def\apjs{\ref@jnl{ApJS}} % Astrophysical Journal, Supplement \def\ao{\ref@jnl{Appl.~Opt.}} % Applied Optics \def\apss{\ref@jnl{Ap\&SS}} % Astrophysics and Space Science \def\aap{\ref@jnl{A\&A}} % Astronomy and Astrophysics \def\aapr{\ref@jnl{A\&A~Rev.}} % Astronomy and Astrophysics Reviews \def\aaps{\ref@jnl{A\&AS}} % Astronomy and Astrophysics, Supplement \def\azh{\ref@jnl{AZh}} % Astronomicheskii Zhurnal \def\baas{\ref@jnl{BAAS}} % Bulletin of the AAS \def\jrasc{\ref@jnl{JRASC}} % Journal of the RAS of Canada \def\memras{\ref@jnl{MmRAS}} % Memoirs of the RAS \def\mnras{\ref@jnl{MNRAS}} % Monthly Notices of the RAS \def\pra{\ref@jnl{Phys.~Rev.~A}} % Physical Review A: General Physics \def\prb{\ref@jnl{Phys.~Rev.~B}} % Physical Review B: Solid State \def\prc{\ref@jnl{Phys.~Rev.~C}} % Physical Review C \def\prd{\ref@jnl{Phys.~Rev.~D}} % Physical Review D \def\pre{\ref@jnl{Phys.~Rev.~E}} % Physical Review E \def\prl{\ref@jnl{Phys.~Rev.~Lett.}} % Physical Review Letters \def\pasp{\ref@jnl{PASP}} % Publications of the ASP \def\pasj{\ref@jnl{PASJ}} % Publications of the ASJ \def\qjras{\ref@jnl{QJRAS}} % Quarterly Journal of the RAS \def\skytel{\ref@jnl{S\&T}} % Sky and Telescope \def\solphys{\ref@jnl{Sol.~Phys.}} % Solar Physics \def\sovast{\ref@jnl{Soviet~Ast.}} % Soviet Astronomy \def\ssr{\ref@jnl{Space~Sci.~Rev.}} % Space Science Reviews \def\zap{\ref@jnl{ZAp}} % Zeitschrift fuer Astrophysik \def\nat{\ref@jnl{Nature}} % Nature \def\iaucirc{\ref@jnl{IAU~Circ.}} % IAU Cirulars \def\aplett{\ref@jnl{Astrophys.~Lett.}} % Astrophysics Letters \def\apspr{\ref@jnl{Astrophys.~Space~Phys.~Res.}} % Astrophysics Space Physics Research \def\bain{\ref@jnl{Bull.~Astron.~Inst.~Netherlands}} % Bulletin Astronomical Institute of the Netherlands \def\fcp{\ref@jnl{Fund.~Cosmic~Phys.}} % Fundamental Cosmic Physics \def\gca{\ref@jnl{Geochim.~Cosmochim.~Acta}} % Geochimica Cosmochimica Acta \def\grl{\ref@jnl{Geophys.~Res.~Lett.}} % Geophysics Research Letters \def\jcp{\ref@jnl{J.~Chem.~Phys.}} % Journal of Chemical Physics \def\jgr{\ref@jnl{J.~Geophys.~Res.}} % Journal of Geophysics Research \def\jqsrt{\ref@jnl{J.~Quant.~Spec.~Radiat.~Transf.}} % Journal of Quantitiative Spectroscopy and Radiative Trasfer \def\memsai{\ref@jnl{Mem.~Soc.~Astron.~Italiana}} % Mem. Societa Astronomica Italiana \def\nphysa{\ref@jnl{Nucl.~Phys.~A}} % Nuclear Physics A \def\physrep{\ref@jnl{Phys.~Rep.}} % Physics Reports \def\physscr{\ref@jnl{Phys.~Scr}} % Physica Scripta \def\planss{\ref@jnl{Planet.~Space~Sci.}} % Planetary Space Science \def\procspie{\ref@jnl{Proc.~SPIE}} % Proceedings of the SPIE \let\astap=\aap \let\apjlett=\apjl \let\apjsupp=\apjs \let\applopt=\ao % **************************************** % * MISCELLANEOUS * % **************************************** \def\phn{\phantom{0}} % Phantom numeral for aligning columns in tables \def\phd{\phantom{.}} % Phantom decimal for aligning columns in tables \def\phs{\phantom{$-$}} % Phantom minus sign for aligning columns in tables \def\phm#1{\phantom{#1}} % Generic \phantom command \def\sun{\hbox{$\odot$}} \def\earth{\hbox{$\oplus$}} \def\lesssim{\mathrel{\hbox{\rlap{\hbox{\lower4pt\hbox{$\sim$}}}\hbox{$<$}}}} \def\gtrsim{\mathrel{\hbox{\rlap{\hbox{\lower4pt\hbox{$\sim$}}}\hbox{$>$}}}} \def\sq{\hbox{\rlap{$\sqcap$}$\sqcup$}} \def\arcdeg{\hbox{$^\circ$}} \def\arcmin{\hbox{$^\prime$}} \def\arcsec{\hbox{$^{\prime\prime}$}} \def\fd{\hbox{$.\!\!^{\rm d}$}} \def\fh{\hbox{$.\!\!^{\rm h}$}} \def\fm{\hbox{$.\!\!^{\rm m}$}} \def\fs{\hbox{$.\!\!^{\rm s}$}} \def\fdg{\hbox{$.\!\!^\circ$}} \def\farcm{\hbox{$.\mkern-4mu^\prime$}} \def\farcs{\hbox{$.\!\!^{\prime\prime}$}} \def\fp{\hbox{$.\!\!^{\scriptscriptstyle\rm p}$}} \def\micron{\hbox{$\mu$m}} \let\la=\lesssim % For Springer A&A compliance... \let\ga=\gtrsim \def\case#1#2{\hbox{$\frac{#1}{#2}$}} \def\slantfrac#1#2{\hbox{$\,^#1\!/_#2$}} \def\onehalf{\slantfrac{1}{2}} \def\onethird{\slantfrac{1}{3}} \def\twothirds{\slantfrac{2}{3}} \def\onequarter{\slantfrac{1}{4}} \def\threequarters{\slantfrac{3}{4}} \def\ubvr{\hbox{$U\!BV\!R$}} % UBVR system \def\ub{\hbox{$U\!-\!B$}} % U-B \def\bv{\hbox{$B\!-\!V$}} % B-V \def\vr{\hbox{$V\!-\!R$}} % V-R \def\ur{\hbox{$U\!-\!R$}} % U-R \def\ion#1#2{#1$\;${\small\rm\@Roman{#2}}\relax} %\def\cellipsis{\hfill$\cdots$\hfill} %\def\nodata{\multicolumn{1}{c}{$\cdots$}} \def\nodata{ ~$\cdots$~ } \newcount\lecurrentfam \def\LaTeX{\lecurrentfam=\the\fam \leavevmode L\raise.42ex \hbox{$\fam\lecurrentfam\scriptstyle\kern-.3em A$}\kern-.15em\TeX} % **************************************** % * DEBUGGING * % **************************************** \def\sizrpt{ (\fontname\the\font): em=\the\fontdimen6\font, ex=\the\fontdimen5\font \typeout{ (\fontname\the\font): em=\the\fontdimen6\font, ex=\the\fontdimen5\font }} emulateapj5.sty0100644000000000000000000006300710376206774012554 0ustar rootroot%% This is emulateapj5.sty, version Dec 11, 2001 %% if this version is old please obtain a new one at the site below %% %% %% `emulateapj5' is a LaTeX2e style to approximate the Astrophysical %% Journal (ApJ) page look. The page length of the document is close to that %% in ApJ if postscript Times fonts are used instead of the standard CM fonts %% (see below). %% %% The file emulateapj5.sty is a complementary package to the AAS (American %% Astronomical Society) document class aastex.cls. If a manuscript is %% prepared using the standard AAS macros used for electronic manuscript %% submission, the only thing required from the user is to add %% \usepackage{emulateapj5}. %% %% %% The latest version of emulateapj.sty is available from %% http://hea-www.harvard.edu/~alexey/emulateapj/ %% To use Times postscript fonts, you may use the accompanying file %% apjfonts.sty (at the site above, there is also a package of font files %% if necessary), but modern TeX distributions may provide better %% alternatives. %% %% %% Alexey Vikhlinin %% %%~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ %% Solutions for some common problems: %% %% 1) Because `multicol' package cannot deal with floats of the width of the %% single column, footnotes, figures, tables etc. can only be set across two %% columns (that is, use `figure*' environment instead of `figure'.) %% Alternatively, insert figures as non-floats in the exact place of the text %% by hand. %% %% 2) There is a command \submitted{your text} to replace the default text %% in the upper left corner of the front page ("Draft version \today") with %% `your text'. Use it before the title commands. You may also use the AASTeX %% command \slugcomment. %% %% 3) There is a package option `onecolumn' %% \usepackage[onecolumn]{emulateapj}, which sets the whole paper in one column %% mode as is done by the ApJ for papers with lengthy equations. Even if the %% document is `onecolumn', `thebibliography' or `references' are typeset in %% two columns. %% %% 4) The \title command makes the entire title text, even math, upper case. %% If you wish to preserve the lower case in some portion of the title, use %% the \lowercase macro, e.g. \title{Upper case text \lowercase{$lower case$}} %% If you wish to preserve the letter case in the entrire title, redefine %% the \uppercase macro locally: %% {\let\uppercase\relax \title{The Title} } %% %% 5) By default, sections within appendix are not numbered: %% APPENDIX %% Derivation of equation 1 %% %% If you want the numbered sections within appendix %% APPENDIX %% A. Derivation of equation 1 %% \usepackage[numberedappendix]{emulateapj} %% %% 6) The comment string in the top-left corner of the first page can be %% controlled by the \journalinfo command (unavailable in standard %% AASTeX), e.g. \journalinfo{astro-ph/xxxxxx}. Be sure to issue this %% command before \title. %% %% By default, the contents of the top-left comment string is identical %% to \slugcomment, which is printed before the abstract in italics. %% %%~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ %% Changes: %% 28 Jan 00 (AV): Original release, incorporating all of the important code %% from emulateapj, but with a substantial rewriting. %% 11 Apr 00 (AV): Change spacing between the affiliation and slugcomment, %% and also the font size for slugcomment. %% %% 20 Apr 00 (AV): change sizes in aastex \cutinhead. %% %% 22 Jun 00 (AV): make \altaffilmark use \textsuperscript to please the %% owners of expert fonts %% %% 14 Jul 00 (AV): put a space between the footnotemark and text. %% %% 15 Jul 00 (AV): instead of \UpperCase\footnotesize, the section titles %% are set in \scshape\lowercase %% %% 16 Jul 00 (AV): appendix sections can be optionally numbered with the %% [numberedappendix] package option. %% %% 21 Aug 00 (AV): add \mbox{} to definition of \@mkfntext to deal with the %% AAStex's poor definition of \@mkfnmark involving \rlap %% %% 26 Aug 00 (AV): prohibit page break between ``APPENDIX'' and the first %% appendix title. %% %% 14 Sep 00 (AV): a) add definition of \email (AASTeX's one did not work) %% b) per suggestion from Joel Parker, the comment on %% top-left can be controlled by \journalinfo independetly %% of the \slugcomment %% %% 19 Feb 01 (AV): set \@rightskip=\z@ to remove \raggedright from the %% lists. %% %% 25 Apr 01 (AV): use \centering in title and add explicit vertical %% space before \author (to allow multiple \author) commands %% %% 11 Dec 01 (AV): \altaffiltext uses arabic marks when inside \author{} %% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %% Copyright 2000-2001 Alexey Vikhlinin %% %% The original idea is due to Maxim Markevitch who wrote the first version %% of this package %% %% This program can be redistributed and/or modified under the terms %% of the LaTeX Project Public License available from CTAN archives in %% directory macros/latex/base/lppl.txt. This means you are free to use and %% distribute this package; however, if you modify anything, please change the %% file name and remove the authors email address. %% %% Alexey Vikhlinin %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \def\emulapj@ver{11/12/01} \RequirePackage{multicol,epsf,graphicx} \ProvidesPackage{emulateapj5} % **************************************************** % * Fix aastex pecularities * % **************************************************** \rightskip \z@ \@rightskip=\z@ \AtBeginDocument{% \everypar{} }% %%%%%%%% The following code is taken from size10.clo; it fixes %%%%%%%% aastex's definition of type sizes \renewcommand\normalsize{% \@setfontsize\normalsize\@xpt\@xiipt \abovedisplayskip 0.0625in \@plus2\p@ \@minus5\p@ \abovedisplayshortskip \z@ \@plus3\p@ \belowdisplayshortskip 6\p@ \@plus3\p@ \@minus3\p@ \belowdisplayskip \abovedisplayskip \let\@listi\@listI} \normalsize \renewcommand\small{% \@setfontsize\small\@ixpt{11}% \abovedisplayskip 8.5\p@ \@plus3\p@ \@minus4\p@ \abovedisplayshortskip \z@ \@plus2\p@ \belowdisplayshortskip 4\p@ \@plus2\p@ \@minus2\p@ \def\@listi{\leftmargin\leftmargini \topsep 4\p@ \@plus2\p@ \@minus2\p@ \parsep 2\p@ \@plus\p@ \@minus\p@ \itemsep \parsep}% \belowdisplayskip \abovedisplayskip } \renewcommand\footnotesize{% \@setfontsize\footnotesize\@viiipt{9.5}% \abovedisplayskip 6\p@ \@plus2\p@ \@minus4\p@ \abovedisplayshortskip \z@ \@plus\p@ \belowdisplayshortskip 3\p@ \@plus\p@ \@minus2\p@ \def\@listi{\leftmargin\leftmargini \topsep 3\p@ \@plus\p@ \@minus\p@ \parsep 2\p@ \@plus\p@ \@minus\p@ \itemsep \parsep}% \belowdisplayskip \abovedisplayskip } \renewcommand\scriptsize{\@setfontsize\scriptsize\@viipt\@viiipt} \renewcommand\tiny{\@setfontsize\tiny\@vpt\@vipt} \renewcommand\large{\@setfontsize\large\@xiipt{14}} \renewcommand\Large{\@setfontsize\Large\@xivpt{18}} \renewcommand\LARGE{\@setfontsize\LARGE\@xviipt{22}} \renewcommand\huge{\@setfontsize\huge\@xxpt{25}} \renewcommand\Huge{\@setfontsize\Huge\@xxvpt{30}} \setlength\smallskipamount{3\p@ \@plus 1\p@ \@minus 1\p@} \setlength\medskipamount{6\p@ \@plus 2\p@ \@minus 2\p@} \setlength\bigskipamount{12\p@ \@plus 4\p@ \@minus 4\p@} \setlength\headheight{12\p@} \def\@listi{\leftmargin\leftmargini \parsep 4\p@ \@plus2\p@ \@minus\p@ \topsep 8\p@ \@plus2\p@ \@minus4\p@ \itemsep4\p@ \@plus2\p@ \@minus\p@} \let\@listI\@listi \@listi \def\@listii {\leftmargin\leftmarginii \labelwidth\leftmarginii \advance\labelwidth-\labelsep \topsep 4\p@ \@plus2\p@ \@minus\p@ \parsep 2\p@ \@plus\p@ \@minus\p@ \itemsep \parsep} \def\@listiii{\leftmargin\leftmarginiii \labelwidth\leftmarginiii \advance\labelwidth-\labelsep \topsep 2\p@ \@plus\p@\@minus\p@ \parsep \z@ \partopsep \p@ \@plus\z@ \@minus\p@ \itemsep \topsep} \def\@listiv {\leftmargin\leftmarginiv \labelwidth\leftmarginiv \advance\labelwidth-\labelsep} \def\@listv {\leftmargin\leftmarginv \labelwidth\leftmarginv \advance\labelwidth-\labelsep} \def\@listvi {\leftmargin\leftmarginvi \labelwidth\leftmarginvi \advance\labelwidth-\labelsep} \def\open@footnotetext{% \insert\footins\bgroup % \egroup in \close@footnotetext \footnotesize% Added by AV \interlinepenalty\interfootnotelinepenalty \splittopskip\footnotesep \splitmaxdepth\dp\strutbox \floatingpenalty \@MM \reset@font\footnote@size \hsize\columnwidth \@parboxrestore }% % **************************************************** % * TWO AND SINGLE ONE COLUMN STYLES: AV * % **************************************************** % % I define `slocitlum' which is \relax if onecolumn option is chosen or % plain multicols if twocolumn (default option); `slocitlum' is used % everywhere except for `thebibliography' and `references' which should be % always set in two columns. % \newenvironment{slocitlum}[1]{\relax}{\relax} \DeclareOption{twocolumn}{ \renewenvironment{slocitlum}[1]{\begin{multicols}{#1}}{\end{multicols}} } \DeclareOption{onecolumn}{ \renewenvironment{slocitlum}[1]{\relax}{\relax} } \ExecuteOptions{twocolumn} %%%%% include atbeginend.sty by AV: % Copy \begin and \end to \BeginEnvironment and \EndEnvironment \let\BeginEnvironment=\begin \let\EndEnvironment=\end %% \ifundefined from TeXbook \def\IfUnDef#1{\expandafter\ifx\csname#1\endcsname\relax} % Null command needed to eat its argument \def\NullCom#1{} \def\begin#1{% % if defined \BeforeBeg for this environment, execute it \IfUnDef{BeforeBeg#1}\else\csname BeforeBeg#1\endcsname\fi% \IfUnDef{AfterBeg#1}% This is done to skip the command for environments % which can take arguments, like multicols; YOU MUST NOT % USE \AfterBegin{...}{...} for such environments! \let\SaveBegEnd=\BeginEnvironment% \else % Start this environment \BeginEnvironment{#1}% % and execute code after \begin{environment} \csname AfterBeg#1\endcsname \let\SaveBegEnd=\NullCom \fi \SaveBegEnd{#1} } \def\end#1{% % execute code before \end{environment} \IfUnDef{BeforeEnd#1}\else\csname BeforeEnd#1\endcsname\fi% % close this environment \EndEnvironment{#1} % and execute code after \begin{environment} \IfUnDef{AfterEnd#1}\else\csname AfterEnd#1\endcsname\fi% } \def\BeforeBegin#1#2{\expandafter\gdef\csname BeforeBeg#1\endcsname {#2}} \def\BeforeEnd #1#2{\expandafter\gdef\csname BeforeEnd#1\endcsname {#2}} \def\AfterBegin #1#2{\expandafter\gdef\csname AfterBeg#1\endcsname {#2}} \def\AfterEnd #1#2{\expandafter\gdef\csname AfterEnd#1\endcsname{#2}} %%%% end of atbeginend.sty % **************************************** % * PAGE LAYOUT * % **************************************** % Page size, spacing parameters, etc. %% (MM) for ApJ approx, using Times-Roman 10pt font: \textwidth=18.55cm \columnsep=8.5mm \parindent=3.5mm \voffset=-20mm \hoffset=-9mm \newlength{\abstrwidth} \abstrwidth=15.9cm \topmargin=0in \headheight=.15in \headsep=0.5in \oddsidemargin=0in \evensidemargin=0in \parskip=0cm %\tolerance=600 % 3x "normal" value; cuts down on overfull complaints \def\@tightleading{1.1} \def\@doubleleading{1.6} %% AV,MM, to have 63 lines per column, with textheight 25cm: \def\baselinestretch{0.92} \textheight=24.4cm \textheight=63\baselineskip \textheight=\baselinestretch\textheight \ifdim\textheight>24.6cm\textheight=24.4cm\fi \let\tighten=\relax \let\tightenlines=\tighten \let\singlespace=\relax \let\doublespace=\relax \def\eqsecnum{ \@newctr{equation}[section] \def\theequation{\hbox{\normalsize\arabic{section}-\arabic{equation}}}} %% running heads: \def\lefthead#1{\gdef\@versohead{#1}} \lefthead{\relax} \def\righthead#1{\gdef\@rectohead{#1}} \righthead{\relax} \let\shorttitle=\lefthead % New AASTEX commands \let\shortauthors\righthead % New AASTEX commands %% MM Create "apjheads" page style: \def\ps@apjheads{\let\@mkboth\markboth \def\@evenfoot{} \def\@evenhead{\lower9mm\hbox to\textwidth{ \rm\thepage\hfil \rm\@rectohead \hfil}}} \def\@oddfoot{} \def\@oddhead{\lower9mm\hbox to\textwidth{ \hfil\rm\@versohead\hfil \rm\thepage}} \@twosidetrue \ps@apjheads %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % TITLE PAGE % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \def\maketitle{\relax}% Because aastex makes its own fron matter \renewenvironment{abstract}[0]{\centering\vskip 0.1in \begin{minipage}{\abstrwidth} \vspace{2pt} \centerline{ABSTRACT} \vspace{3pt} \parindent=3.5mm} {\end{minipage}\par} \BeforeBegin{abstract}{{\footnotesize \vskip 0.1\baselineskip%x \centerline{\it{\@submitted}} }} \def\ps@apjbot{ \def\@oddfoot{\raise7mm\hbox to\textwidth{\hfil\rm\thepage\hfil}} \def\@oddhead{}} \def\title#1{{\thispagestyle{apjbot} \subtitle \vspace{12mm} \par \centering \begin{minipage}{\abstrwidth} \center\uppercase{#1}\endcenter \end{minipage}\par}} \def\author#1{% { \vspace{8pt} \centering \begin{minipage}{0.9\abstrwidth} \def\thempfootnote{\@arabic\c@mpfootnote} \center\small\scshape#1\endcenter \end{minipage} \par } } %\let\authoraddr=\@gobble %\let\authoremail=\@gobble \def\affil#1{\vspace{2pt}{\centering \footnotesize\def\baselinestretch{1.0}% \begin{minipage}{0.9\abstrwidth}% \centering #1\par% \end{minipage}% \par% }} \def\altaffilmark#1{\textsuperscript{#1}} \def\altaffiltext#1#2{\footnotetext[#1]{#2}\stepcounter{footnote}} \def\email#1{{\par\centering\footnotesize#1\par}} % Redefine the LaTeX \and command for this style. %% MM \def\and{\vspace{0pt}{\topsep\z@\center {\sc and}\endcenter}\vspace{3pt}} % **************************************** % * KEYWORDS * % **************************************** \def\@keywordtext{Subject headings} \def\@keyworddelim{---} %% MM,AV \newlength{\kwdtextwidth} \settowidth{\kwdtextwidth}{{\it\@keywordtext:\/}} \def\keywords#1{\begin{center} \begin{minipage}{\abstrwidth} \vspace*{-6pt}\raggedright \par\hangindent=\kwdtextwidth\hangafter=1 \noindent {\it\@keywordtext:\/}\space #1 \end{minipage} \end{center}} \let\subjectheadings=\keywords \def\@kwds#1{#1\relax} % **************************************** % * FOOTNOTES * % **************************************** %% MM \skip\footins 2mm \footnotesep 2ex \let\footnoterule\relax %% ApJ puts a space between the footnotemarm and text. \mbox{} is added to %% fix the bad behavior of AAStex \def\@makefntext#1{\mbox{}\@makefnmark~#1} \def\notetoeditor#1{}% % We do not need notes to editor in the preprint % **************************************** % * SECTIONS * % **************************************** \newif\if@firstsection \@firstsectiontrue %% MM: section vertical indents by eye: \def\section{% \if@firstsection\@firstsectionfalse\begin{slocitlum}{2}\fi% \@startsection{section}{1}{\z@}{10pt plus 2pt minus 1pt}{5pt}{\scshape \center}} \def\subsection{\@startsection{subsection}{2}{\z@}{5pt plus 1pt minus 1pt}{5pt}% {\normalsize\it \center}} \def\subsubsection{\@startsection{subsubsection}{3}{\z@}% {2ex plus 1ex minus .2ex}{1ex plus .2ex}{\normalsize\it \center}} \def\thesection{\@arabic{\c@section}} \def\thesubsection{\thesection.\@arabic{\c@subsection}} \def\thesubsubsection{\thesubsection.\@arabic{\c@subsubsection}} \def\theparagraph{\thesubsubsection.\@arabic{\c@paragraph}} \def\sec@upcase#1{\lowercase{#1}} \def\subsec@upcase#1{\relax{#1}} \def\secnum@size{\small} \def\subsecnum@size{\normalsize} % % How the section number will appear in the section title - AV \def\ApjSectionMarkInTitle#1{#1.\ } \def\ApjSectionpenalty{0} \def\@sect#1#2#3#4#5#6[#7]#8% {\@tempskipa #5\relax \ifdim \@tempskipa >\z@ \begingroup #6\relax \ifnum #2>\c@secnumdepth \def \@svsec {}\else \refstepcounter{#1} \edef \@svsec {\ApjSectionMarkInTitle {\csname the#1\endcsname}}\fi \@hangfrom {\hskip #3\relax \ifnum #2=1\secnum@size {\rm\@svsec~}% \else \subsecnum@size {\rm\@svsec~}\fi }% {\interlinepenalty \@M \ifnum #2=1\sec@upcase{#8}% \else \subsec@upcase{#8}\fi\par}\endgroup \csname #1mark\endcsname {#7}\addcontentsline{toc}{#1}% {\ifnum #2>\c@secnumdepth \else \protect \numberline {\csname the#1\endcsname }\fi #7}% \else \ifnum #2>\c@secnumdepth \def \@svsec {}\else \refstepcounter{#1} \edef \@svsec {\ApjSectionMarkInTitle {\csname the#1\endcsname}}\fi \def \@svsechd {#6\hskip #3% \ifnum #2=1\secnum@size{\rm\@svsec~}\else\subsecnum@size{\rm\@svsec~}\fi% \ifnum #2=1\sec@upcase{#8}\else\subsec@upcase{#8}\fi% \csname #1mark\endcsname {#7}\addcontentsline{toc}{#1}% {\ifnum #2>\c@secnumdepth \else \protect \numberline {\csname the#1\endcsname }\fi #7}}\fi \@xsect {#5} \penalty \ApjSectionpenalty %-refstepcounter is now within a group. So \@currentlabel, which is normally %-set by \refstepcounter is hidden within a group. Need to set it manually. \protected@edef\@currentlabel{\csname p@#1\endcsname\csname the#1\endcsname} } \def\@ssect#1#2#3#4#5{\@tempskipa #3\relax \ifdim \@tempskipa>\z@ \begingroup #4\@hangfrom{\hskip #1}{\interlinepenalty \@M \sec@upcase{#5}\par}\endgroup \else \def\@svsechd{#4\hskip #1\relax \sec@upcase{#5}}\fi \@xsect{#3} % MM: \penalty \ApjSectionpenalty} \def\acknowledgments{\vskip 3ex plus .8ex minus .4ex} \let\acknowledgements=\acknowledgments % second spelling % **************************************** % * APPENDIX * % **************************************** \def\AppendixApjSectionMarkInTitle#1{\relax} \DeclareOption{numberedappendix}{ \def\AppendixApjSectionMarkInTitle#1{#1.\ } } \renewenvironment{appendix}[0]{ \if\inmulticols\inmulticolstest\end{slocitlum}\fi \vskip 10pt plus 2pt minus 1pt \noindent\mbox{}\hfill{\small APPENDIX}\hfill\mbox{}\par \nopagebreak\medskip\@nobreaktrue\def\ApjSectionpenalty{\@M} \@firstsectionfalse \setcounter{section}{0} \setcounter{subsection}{0} \setcounter{equation}{0} % \setcounter{figure}{0} % \setcounter{table}{0} % \def\fnum@figure{Figure \Alph{section}\thefigure:} % \def\fnum@table{Table \Alph{section}\thetable:} \def\thesection{\Alph{section}} \def\theequation{\hbox{\Alph{section}\arabic{equation}}} \def\thefigure{\thesection\@arabic\c@figure} \def\thetable{\thesection\@arabic\c@table} % % Do not use appendix numbers in the titles \def\ApjSectionMarkInTitle{\AppendixApjSectionMarkInTitle} \def\section{\setcounter{equation}{0}\@startsection {section}{1}{\z@} {10pt}{5pt}{\centering\scshape}} % % }{} \BeforeBegin{appendix}{\if\inmulticols\inmulticolstest\end{slocitlum}} % **************************************** % * BIBLIOGRAPHY * % **************************************** \renewenvironment{references}[0]{ \vspace{3pt plus 3pt} % \hbox to \textwidth{\centerline{\footnotesize REFERENCES}} % \vspace{-5pt} \begin{multicols}{2}[\hbox to \textwidth{\centerline{\footnotesize REFERENCES}} \vspace{-5pt}] \parindent=0cm \parskip=0cm \footnotesize \baselineskip=8pt \interlinepenalty \@M \hyphenpenalty=10000 \frenchspacing % AV - to get right spacing after ``et al.'' \def\refpar{\par\hangindent=1.2em\hangafter=1}} {\end{multicols}} % redefine thebibliography \renewenvironment{thebibliography}[1]{ \vspace{3pt plus 3 pt} % AV \begin{multicols}{2}[\hbox % AV to \textwidth{\centerline{\footnotesize % AV REFERENCES}} \vspace{-5pt}] % AV \list{ \@biblabel{\@arabic\c@enumiv}}% { \@openbib@code \parindent=0pt \parskip=0pt \parsep=0pt % AV \bibindent=0pt % \footnotesize \baselineskip=8pt \interlinepenalty \@M % AV \frenchspacing % AV - to get right spacing after ``et al.'' \hyphenpenalty=10000 \itemindent=-1.0em % \itemsep=0pt % \listparindent=0pt % \settowidth\labelwidth{\@biblabel{#1}} % \labelsep=0pt % \leftmargin=1.0em \advance\leftmargin\labelsep \usecounter{enumiv}% \let\p@enumiv\@empty \renewcommand\theenumiv{\@arabic\c@enumiv}}% \sloppy\clubpenalty4000\widowpenalty4000% \sfcode`\.\@m} {\def\@noitemerr {\@latex@warning{Empty `thebibliography' environment}}% \endlist\if\inmulticols\inmulticolstest\end{multicols}\fi} % %% AV: \def\inmulticols{0} \def\inmulticolstest{1} \BeforeBegin{multicols}{\def\inmulticols{1}} \AfterEnd{multicols}{\def\inmulticols{0}} \BeforeBegin{slocitlum}{\def\inmulticols{1}} \AfterEnd{slocitlum}{\def\inmulticols{0}} \BeforeBegin{references}{\if\inmulticols\inmulticolstest\end{slocitlum}% \else\vspace{10pt}\fi} \BeforeBegin{thebibliography}{\if\inmulticols\inmulticolstest\end{slocitlum}% \else\vspace{10pt}\fi} \BeforeEnd{document}{\if\inmulticols\inmulticolstest\end{slocitlum}\fi} \def\reference{\@ifnextchar\bgroup {\@reference} {\@latexerr{Missing key on reference command} {Each reference command should have a key corresponding to a markcite somewhere in the text}}} \def\@reference#1{\relax\refpar} %% subtitle header and journal info: \def\submitted#1{\gdef\@submitted{#1}} \def\journalinfo#1{\gdef\@journalinfo{#1}} \def\subtitle{ \vspace*{-12mm} \noindent {\scriptsize {\sc \@journalinfo} \\ Preprint typeset using \LaTeX\ style emulateapj v.\ \emulapj@ver} } \let\slugcomment\submitted % slugcomment == submitted \submitted{Draft version \today} \journalinfo{\@submitted} %% AV: allow figures to take the whole page \renewcommand{\topfraction}{1.0} \renewcommand{\bottomfraction}{1.0} \renewcommand{\textfraction}{0.0} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % Equations % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % EQNARRAY with reduced spacing around tab characters - AV \def\eqnarray{% \stepcounter{equation}% \def\@currentlabel{\p@equation\theequation}% \global\@eqnswtrue \setlength{\arraycolsep}{0.25\arraycolsep} \m@th \global\@eqcnt\z@ \tabskip\@centering \let\\\@eqncr $$\everycr{}\halign to\displaywidth\bgroup \hskip\@centering$\displaystyle\tabskip\z@skip{##}$\@eqnsel &\global\@eqcnt\@ne\hskip \tw@\arraycolsep \hfil${##}$\hfil &\global\@eqcnt\tw@ \hskip \tw@\arraycolsep $\displaystyle{##}$\hfil\tabskip\@centering &\global\@eqcnt\thr@@ \hb@xt@\z@\bgroup\hss##\egroup \tabskip\z@skip \cr } % **************************************** % * TABLES AND FIGURES * % **************************************** \setcounter{topnumber}{7} \setlength{\belowcaptionskip}{0pt} \setlength{\abovecaptionskip}{5pt} \long\def\@makecaption#1#2{% \noindent\begin{minipage}{0.99\linewidth} %% \noindent is needed because %% otherwise minipage + parindent does not fit into the line and spurious %% vertical skip appear after caption \if\csname ftype@\@captype\endcsname 2 \vskip 2ex\noindent \centering\small\scshape #1 #2\par\medskip \else \vskip \abovecaptionskip\footnotesize\noindent #1 #2\par\vskip \belowcaptionskip \fi \end{minipage} } %%%%%%%%%%%% FIX \cutinhead \renewcommand\cutinhead[1]{% \noalign{\vskip 1.5ex}% \hline \@ptabularcr \noalign{\vskip -1.5ex}% \multicolumn{\pt@ncol}{c}{#1}% \@ptabularcr \noalign{\vskip .8ex}% \hline \@ptabularcr \noalign{\vskip -2ex}% }% %% suggested by Joern Wilms wilms@astro.uni-tuebingen.de %% wilms@rocinante.colorado.edu \def\@figcaption#1{{\def\@captype{figure}\caption{\footnotesize #1}}} \def\@xfigcaption[#1]#2{{\def\@captype{figure}\caption{\footnotesize #2}}} \def\thefigure{\@arabic\c@figure} \def\fnum@figure{{\footnotesize\scshape ~~Fig.\space\thefigure.---}} \def\thetable{\@arabic\c@table} %%% Table captions without making a floating table \def\tablehead#1{\gdef\pt@head{\hline\hline\relax\\[-1.7ex] #1\hskip\tabcolsep\\[.7ex]\hline\relax\\[-1.5ex]}} \def\pt@head{\relax} \def\tabcaption{\@ifnextchar[{\@xtabcaption}{\@tabcaption}} \def\@tabcaption#1{{\def\@captype{table}\caption{#1}}} \def\@xtabcaption[#1]#2{{\def\@captype{table}\caption{#2}}} \def\fnum@table{{\centering{\scshape Table~\thetable}\vskip0.7ex\relax}} \let\fnum@ptable=\fnum@table \def\fnum@ptablecont{{\centering{\scshape Table~\thetable}---{\itshape Continued}}}% \let\tablefontsize=\tabletypesize % for compatibility with old documents \long\def\@make@caption@text#1#2{% {\small\centering#1{\scshape #2}\par\vskip1.4ex} }% \long\def\@makecaption@plano@cont#1#2{% {\small \centering#1\par}\vskip1.4ex\relax }% \ProcessOptions f1.eps0100644000000000000000000010023710376206774010613 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 240 198 %%Title: Graphics produced by IDL %%For: pen@origo, /usr/users/pen/li6.paper/plot.figures %%Creator: IDL Version 6.1 (IRIX mipseb m64) %%CreationDate: Wed Aug 17 12:22:44 2005 %%DocumentData: Clean7bit %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. 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-62 R 76 10 R 176 33 R 97 25 R 94 27 R 223 78 R 448 200 R 188 96 R 87 45 R 34 18 R 112 59 R 106 57 R 52 27 R 27 15 R 128 67 R 214 110 R 10 5 R 490 220 R 185 65 R 83 25 R 22 7 R 127 32 R 251 42 R 434 -10 R 45 -8 R 43 -9 R 80 -20 R 185 -64 R 75 -33 R 301 -182 R 254 -218 R 40 -39 R 26 -27 R 221 -257 R 216 -302 R 144 -231 R 96 -167 R D %%PageTrailer end %%PageResources: font Helvetica %%Trailer %%Pages: 1 %%DocumentNeededResources: font Helvetica %%EOF f10a.eps0100644000000000000000000012712210376206774011036 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/G013-009 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:07:44 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 2023 4200 M 0 182 R D 5590 4200 M 0 182 R D 9157 4200 M 0 182 R D 12723 4200 M 0 182 R D 16290 4200 M 0 182 R D 2915 4200 M 0 91 R D 3806 4200 M 0 91 R D 4698 4200 M 0 91 R D 6481 4200 M 0 91 R D 7373 4200 M 0 91 R D 8265 4200 M 0 91 R D 10048 4200 M 0 91 R D 10940 4200 M 0 91 R D 11832 4200 M 0 91 R D 13615 4200 M 0 91 R D 14507 4200 M 0 91 R D 15399 4200 M 0 91 R D 1800 13300 M 15300 0 R D 2023 13300 M 0 -182 R D 5590 13300 M 0 -182 R D 9157 13300 M 0 -182 R D 12723 13300 M 0 -182 R D 16290 13300 M 0 -182 R D 2915 13300 M 0 -91 R D 3806 13300 M 0 -91 R D 4698 13300 M 0 -91 R D 6481 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end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f10b.eps0100644000000000000000000013353710376206774011046 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/G013-009 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 14:51:53 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 4341 4200 M 0 182 R D 7596 4200 M 0 182 R D 10851 4200 M 0 182 R D 14107 4200 M 0 182 R D 1899 4200 M 0 91 R D 2713 4200 M 0 91 R D 3527 4200 M 0 91 R D 5155 4200 M 0 91 R D 5968 4200 M 0 91 R D 6782 4200 M 0 91 R D 8410 4200 M 0 91 R D 9224 4200 M 0 91 R D 10038 4200 M 0 91 R D 11665 4200 M 0 91 R D 12479 4200 M 0 91 R D 13293 4200 M 0 91 R D 14921 4200 M 0 91 R D 15735 4200 M 0 91 R D 16548 4200 M 0 91 R D 1800 13300 M 15300 0 R D 4341 13300 M 0 -182 R D 7596 13300 M 0 -182 R D 10851 13300 M 0 -182 R D 14107 13300 M 0 -182 R D 1899 13300 M 0 -91 R D 2713 13300 M 0 -91 R D 3527 13300 M 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R D 17100 4200 M -153 0 R D 40 setlinewidth 1800 2707 M 368 -159 R 436 -450 R 436 606 R 436 -620 R 352 -684 R D 4011 1400 M 340 562 R 436 392 R 436 645 R 436 394 R 436 -815 R 437 215 R 436 430 R 436 101 R 436 -84 R 436 -521 R 437 -357 R 436 -73 R 436 169 R 438 -4 R 436 112 R 436 1106 R 437 -368 R 436 -1260 R 436 360 R 436 19 R 437 -768 R 436 -108 R 436 617 R 436 734 R 436 -237 R 437 110 R 437 -128 R 437 108 R 436 134 R 436 -319 R 95 40 R D L1 1800 2712 M 368 -155 R 436 -438 R 436 629 R 436 -571 R 429 -777 R D 3920 1400 M 431 784 R 436 466 R 436 682 R 436 348 R 436 -893 R 437 14 R 436 199 R 436 -45 R 436 -116 R 436 -429 R 437 -189 R 436 80 R 436 358 R 438 42 R 436 149 R 436 1211 R 437 -379 R 436 -1172 R 436 342 R 436 21 R 437 -839 R 436 -188 R 436 535 R 436 655 R 436 -293 R 437 71 R 437 -150 R 437 97 R 436 128 R 436 -321 R 95 40 R D L2 1800 2717 M 368 -150 R 436 -425 R 436 655 R 436 -529 R 437 -713 R 438 854 R 436 529 R 436 710 R 436 295 R 436 -1026 R 437 -178 R 436 24 R 436 -180 R 436 -124 R 436 -330 R 437 -28 R 436 235 R 436 449 R 438 161 R 436 126 R 386 1128 R D 11074 4200 M 258 -205 R 436 -1114 R 436 374 R 436 -19 R 437 -882 R 436 -272 R 436 465 R 436 594 R 436 -340 R 437 44 R 437 -167 R 437 89 R 436 124 R 436 -322 R 95 38 R D 10 setlinewidth L1 1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f10c.eps0100644000000000000000000016476110376206774011052 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, %% /Users/martin/conv/output/1D/G013-009/figures %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:22:12 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 1400 M 15300 0 R D 2164 1400 M 0 238 R D 1481 850 M 273 0 R D 1952 1033 M -46 -16 R -30 -45 R -16 -76 R 0 -46 R 16 -76 R 30 -45 R 46 -15 R 30 0 R 46 15 R 30 45 R 15 76 R 0 46 R -15 76 R -30 45 R -46 16 R -30 0 R -31 -16 R -15 -15 R -15 -30 R -15 -76 R 0 -46 R 15 -76 R 15 -30 R 15 -15 R 31 -15 R D 1982 714 M 30 15 R 16 15 R 15 30 R 15 76 R 0 46 R -15 76 R -15 30 R -16 15 R -30 16 R D 2195 744 M -16 -15 R 16 -15 R 15 15 R -15 15 R D 2362 972 M 30 15 R 46 46 R 0 -319 R D 2423 1017 M 0 -303 R D 2362 714 M 136 0 R D 2711 1033 M -45 -16 R -31 -45 R -15 -76 R 0 -46 R 15 -76 R 31 -45 R 45 -15 R 30 0 R 46 15 R 30 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R 3 14 R 1 15 R F 11747 1977 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 12475 1519 M -1 15 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 5 13 R 2 15 R 1 14 R F 13204 1405 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R 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1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 10 R 8 13 R 6 13 R 5 13 R 3 15 R 1 14 R F L0 7342 13299 M 12 -54 R 12 -54 R 11 -54 R 12 -53 R 12 -54 R 11 -53 R 12 -53 R 12 -53 R 11 -53 R 12 -53 R 12 -52 R 11 -53 R 12 -52 R 12 -52 R 11 -52 R 12 -52 R 12 -51 R 11 -52 R 12 -51 R 12 -52 R 11 -51 R 12 -51 R 12 -50 R 11 -51 R 12 -51 R 12 -50 R 11 -50 R 12 -50 R 12 -50 R 11 -50 R 12 -50 R 12 -49 R 11 -50 R 12 -49 R 12 -49 R 11 -49 R 12 -49 R 12 -48 R 11 -49 R 12 -48 R 12 -48 R 11 -49 R 12 -48 R 12 -47 R 11 -48 R 12 -48 R 12 -47 R 11 -47 R 12 -47 R 12 -47 R 11 -47 R 12 -47 R 12 -47 R 11 -46 R 12 -47 R 12 -46 R 11 -46 R 12 -46 R 12 -45 R 11 -46 R 12 -46 R 12 -45 R 11 -45 R 12 -45 R 12 -45 R 11 -45 R 12 -45 R 12 -45 R 11 -44 R 12 -45 R 12 -44 R 11 -44 R 12 -44 R 12 -44 R 11 -43 R 12 -44 R 12 -43 R 11 -44 R 12 -43 R 12 -43 R 11 -43 R 12 -42 R 12 -43 R 12 -43 R 11 -42 R 12 -42 R 12 -42 R 11 -42 R 12 -42 R 12 -42 R 11 -42 R 12 -41 R 12 -42 R 11 -41 R 12 -41 R 12 -41 R 11 -41 R 12 -41 R 12 -40 R 11 -41 R 12 -40 R 12 -41 R 11 -40 R 12 -40 R 12 -40 R 11 -39 R 12 -40 R 12 -40 R 11 -39 R 12 -39 R 12 -39 R 11 -40 R 12 -38 R 12 -39 R 11 -39 R 12 -38 R 12 -39 R 11 -38 R 12 -38 R 12 -39 R 11 -38 R 12 -37 R 12 -38 R 11 -38 R 12 -37 R 12 -38 R 11 -37 R 12 -37 R 12 -37 R 11 -37 R 12 -37 R 12 -36 R 11 -37 R 12 -36 R 12 -36 R 11 -37 R 12 -36 R 12 -35 R 11 -36 R 12 -36 R 12 -35 R 11 -36 R 12 -35 R 12 -35 R 11 -35 R 12 -35 R 12 -35 R 11 -35 R 12 -34 R 12 -35 R 11 -34 R 12 -34 R 12 -34 R 11 -34 R 12 -34 R 12 -34 R 11 -34 R 12 -33 R 12 -33 R 11 -34 R 12 -33 R 12 -33 R 11 -32 R 12 -33 R 12 -33 R 11 -32 R 12 -32 R 12 -33 R 11 -32 R 12 -32 R 12 -31 R 11 -32 R 12 -32 R 12 -31 R 11 -32 R 12 -31 R 12 -31 R 11 -31 R 12 -31 R 12 -30 R 11 -31 R 12 -30 R 12 -31 R 11 -30 R 12 -30 R 12 -30 R 11 -30 R 12 -29 R 12 -30 R 11 -29 R 12 -29 R 12 -30 R 11 -29 R 12 -29 R 12 -28 R 11 -29 R 12 -29 R 12 -28 R 11 -28 R 12 -29 R 12 -28 R 11 -28 R 12 -28 R 12 -27 R 11 -28 R 12 -27 R 12 -28 R 11 -27 R 12 -27 R 12 -27 R 11 -27 R 12 -27 R 12 -26 R 11 -27 R 12 -26 R 12 -26 R 11 -26 R 12 -26 R 12 -26 R 11 -26 R 12 -26 R 12 -25 R 11 -26 R 12 -25 R 12 -25 R 11 -25 R 12 -25 R 12 -25 R 11 -25 R 12 -25 R 12 -24 R 11 -25 R 12 -24 R 12 -24 R 11 -24 R 12 -24 R 12 -24 R 11 -24 R 12 -23 R 12 -24 R 12 -23 R 11 -23 R 12 -24 R 12 -23 R 11 -23 R 12 -22 R 12 -23 R 11 -23 R 12 -22 R 12 -23 R 11 -22 R 12 -22 R 12 -22 R 11 -22 R 12 -22 R 12 -22 R 11 -21 R 12 -22 R 12 -21 R 11 -21 R 12 -22 R 12 -21 R 11 -21 R 12 -21 R 12 -20 R 11 -21 R 12 -21 R 12 -20 R 11 -20 R 12 -21 R 12 -20 R 11 -20 R 12 -20 R 12 -19 R 11 -20 R 12 -20 R 12 -19 R 11 -20 R 12 -19 R 12 -19 R 11 -19 R 12 -19 R 12 -19 R 11 -19 R 12 -19 R 12 -18 R 11 -19 R 12 -18 R 12 -18 R 11 -19 R 12 -18 R 12 -18 R 11 -18 R 12 -17 R 12 -18 R 11 -18 R 12 -17 R 12 -18 R 11 -17 R 12 -17 R 12 -17 R 11 -17 R 12 -17 R 12 -17 R 11 -17 R 12 -16 R 12 -17 R 11 -16 R 12 -17 R 12 -16 R 11 -16 R 12 -16 R 12 -16 R 11 -16 R 12 -16 R 12 -15 R 11 -16 R 12 -16 R 12 -15 R 11 -15 R 12 -15 R 12 -15 R 11 -15 R 12 -15 R 12 -15 R 11 -15 R 12 -14 R 12 -15 R 11 -14 R 12 -15 R 12 -14 R 11 -14 R 12 -14 R 12 -14 R 11 -14 R 12 -13 R 12 -14 R 11 -13 R 12 -14 R 12 -13 R 11 -13 R 12 -13 R 12 -13 R 11 -13 R 12 -13 R 12 -13 R 11 -12 R 12 -13 R 12 -12 R 11 -13 R 12 -12 R 12 -12 R 11 -12 R 12 -12 R 12 -11 R 11 -12 R 12 -12 R 12 -11 R 11 -11 R 12 -12 R 12 -11 R 11 -11 R 12 -11 R 12 -11 R 11 -10 R 12 -11 R 12 -11 R 11 -10 R 12 -10 R 12 -11 R 11 -10 R 12 -10 R 12 -10 R 11 -9 R 12 -10 R 12 -10 R 11 -9 R 12 -9 R 12 -10 R 11 -9 R 12 -9 R 12 -9 R 11 -9 R 12 -9 R 12 -8 R 11 -9 R 12 -8 R 12 -9 R 11 -8 R 12 -8 R 12 -8 R 11 -8 R 12 -8 R 12 -8 R 12 -8 R 11 -7 R 12 -8 R 12 -7 R 11 -8 R 12 -7 R 12 -7 R 11 -7 R 12 -7 R 12 -7 R 11 -7 R 12 -6 R 12 -7 R 11 -6 R 12 -7 R 12 -6 R 11 -6 R 12 -7 R 12 -6 R 11 -6 R 12 -5 R 12 -6 R 11 -6 R 12 -6 R 12 -5 R 11 -5 R 12 -6 R 12 -5 R 11 -5 R 12 -5 R 12 -5 R 11 -5 R 12 -5 R 12 -5 R 11 -5 R 12 -4 R 12 -5 R 11 -4 R 12 -4 R 12 -5 R 11 -4 R 12 -4 R 12 -4 R 11 -4 R 12 -4 R 12 -3 R 11 -4 R 12 -4 R 12 -3 R 11 -3 R 12 -4 R 12 -3 R 11 -3 R 12 -3 R 12 -3 R 11 -3 R 12 -3 R 12 -3 R 11 -2 R 12 -3 R 12 -2 R 11 -3 R 12 -2 R 12 -2 R 11 -2 R 12 -2 R 12 -2 R 11 -2 R 12 -2 R 12 -2 R 11 -1 R 12 -2 R 12 -1 R 11 -2 R 12 -1 R 12 -1 R 11 -1 R 12 -1 R 12 -1 R 11 -1 R 12 0 R 12 -1 R 11 -1 R 12 0 R 12 0 R 11 -1 R 12 0 R 12 0 R 11 0 R 12 0 R 12 0 R 11 1 R 12 0 R 12 0 R 11 1 R 12 1 R 12 0 R 11 1 R 12 1 R 12 1 R 11 1 R 12 1 R 12 2 R 11 1 R 12 1 R 12 2 R 11 2 R 12 1 R 12 2 R 11 2 R 12 2 R 12 2 R 11 2 R 12 3 R 12 2 R 11 2 R 12 3 R 12 3 R 11 2 R 12 3 R 12 3 R 11 3 R 12 3 R 12 3 R 11 3 R 12 4 R 12 3 R 11 4 R 12 3 R 12 4 R 11 4 R 12 3 R 12 4 R 11 4 R 12 4 R 12 5 R 11 4 R 12 4 R 12 5 R 11 4 R 12 5 R 12 4 R 11 5 R 12 5 R 12 5 R 11 5 R 12 5 R 12 5 R 11 5 R 12 5 R 12 6 R 11 5 R 12 6 R 12 5 R 11 6 R 12 6 R 12 6 R 12 6 R 11 6 R 12 6 R 12 6 R 11 6 R 12 7 R 12 6 R 11 6 R 12 7 R 12 7 R 11 6 R 12 7 R 12 7 R 11 7 R 12 7 R 12 7 R 11 7 R 12 7 R 12 8 R 11 7 R 12 8 R 12 7 R 11 8 R 12 7 R 12 8 R 11 8 R 12 8 R 12 8 R 11 8 R 12 8 R 12 8 R 11 8 R 12 8 R 12 9 R 11 8 R 12 9 R 12 8 R 11 9 R 12 8 R 12 9 R 11 9 R 12 9 R 12 9 R 11 9 R 12 9 R 12 9 R 11 9 R 12 10 R 12 9 R 11 9 R 12 10 R 12 9 R 11 10 R 12 9 R 12 10 R 11 10 R 12 10 R 12 9 R 11 10 R 12 10 R 12 10 R 11 11 R 12 10 R 12 10 R 11 10 R 12 10 R 12 11 R 11 10 R 12 11 R 12 10 R 11 11 R 12 11 R 12 10 R 11 11 R 12 11 R 12 11 R 11 11 R 12 11 R 12 11 R 11 11 R 12 11 R 12 12 R 11 11 R 12 11 R 12 12 R 11 11 R 12 12 R 12 12 R 11 11 R 12 12 R 12 12 R 11 12 R 12 12 R 12 12 R 11 12 R 12 12 R 12 13 R 11 12 R 12 12 R 12 13 R 11 12 R 12 13 R 12 13 R 11 13 R 12 12 R 12 13 R 11 13 R 12 13 R 12 14 R 11 13 R 12 13 R 12 14 R 11 13 R 12 14 R 12 13 R 11 14 R 12 14 R 12 14 R 11 13 R 12 14 R 12 15 R 11 14 R 12 14 R 12 14 R 11 15 R 12 14 R 12 15 R 11 15 R 12 14 R 12 15 R 11 15 R 12 15 R 12 15 R 11 16 R 12 15 R 12 15 R 11 16 R 12 15 R 12 16 R 11 15 R 12 16 R 12 16 R 11 16 R 12 16 R 12 16 R 11 16 R 12 17 R 12 16 R 11 16 R 12 17 R 12 16 R 11 17 R 12 17 R 12 17 R 12 16 R 11 17 R 12 17 R 12 17 R 11 18 R 12 17 R 12 17 R 11 17 R 12 18 R 12 17 R 11 18 R 12 18 R 12 17 R 11 18 R 12 18 R 12 18 R 11 18 R 12 18 R 12 18 R 11 18 R 12 19 R 12 18 R 11 18 R 12 19 R 12 18 R 11 19 R 12 19 R 12 18 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 20 R 12 19 R 12 19 R 11 20 R 12 19 R 12 20 R 11 20 R 12 19 R D 16094 4157 M 12 20 R 11 20 R 12 20 R 12 20 R 11 20 R 12 20 R 12 20 R 11 20 R 12 20 R 12 20 R 11 20 R 12 20 R 12 21 R 11 20 R 12 20 R 12 21 R 11 20 R 12 21 R 12 20 R 11 21 R 12 20 R 12 21 R 11 20 R 12 21 R 12 21 R 11 21 R 12 20 R 12 21 R 11 21 R 12 21 R 12 20 R 11 21 R 12 21 R 12 21 R 11 21 R 12 21 R 12 21 R 11 21 R 12 21 R 12 21 R 11 21 R 12 21 R 12 21 R 11 21 R 12 21 R 12 21 R 11 21 R 12 21 R 12 21 R 11 22 R 12 21 R 12 21 R 11 21 R 12 21 R 12 21 R D 8104 11492 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 15 2 R 13 5 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 8832 8701 M -1 15 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 5 R -14 2 R -15 1 R -14 -1 R -14 -2 R -14 -5 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 9 12 R 6 13 R 5 14 R 2 14 R 1 14 R D 9561 6414 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -12 8 R -14 7 R -13 4 R -15 3 R -14 1 R -14 -1 R -15 -3 R -13 -4 R -14 -7 R -12 -8 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 4 -13 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 12 -8 R 14 -6 R 13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 14 6 R 12 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 13 R 3 15 R 1 14 R D 10290 4584 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 9 R -13 6 R -14 5 R -14 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -6 R -12 -9 R -11 -9 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R D 11018 3212 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 13 R 3 15 R 1 14 R D 11747 2229 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 12475 1657 M -1 14 R -2 15 R -5 13 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 8 12 R 7 13 R 5 14 R 2 14 R 1 15 R D 13204 1405 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -13 4 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 0 -5 R D 13203 1400 M 1 5 R D 13932 1520 M -1 14 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -9 R 13 -6 R 14 -5 R 14 -2 R 14 -1 R 15 1 R 14 2 R 14 5 R 13 6 R 12 9 R 11 9 R 9 11 R 9 12 R 6 13 R 5 14 R 2 14 R 1 15 R D 14661 1908 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -13 9 R -13 6 R -13 5 R -15 2 R -14 1 R -14 -1 R -15 -2 R -13 -5 R -13 -6 R -13 -9 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 13 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R D 15390 2595 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -9 R 12 -9 R 13 -6 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 6 R 12 9 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 16118 3578 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -13 R 10 -10 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 10 R 8 13 R 7 13 R 4 13 R 3 15 R 1 14 R D 16847 4745 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 0 R 14 0 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D L2 7580 13299 M 7 -32 R 12 -53 R 12 -54 R 11 -53 R 12 -53 R 12 -53 R 11 -53 R 12 -52 R 12 -53 R 11 -52 R 12 -52 R 12 -52 R 11 -52 R 12 -52 R 12 -51 R 11 -52 R 12 -51 R 12 -51 R 11 -51 R 12 -51 R 12 -51 R 11 -51 R 12 -50 R 12 -51 R 11 -50 R 12 -50 R 12 -50 R 11 -50 R 12 -49 R 12 -50 R 11 -49 R 12 -50 R 12 -49 R 11 -49 R 12 -49 R 12 -48 R 11 -49 R 12 -49 R 12 -48 R 11 -48 R 12 -48 R 12 -48 R 11 -48 R 12 -48 R 12 -48 R 11 -47 R 12 -48 R 12 -47 R 11 -47 R 12 -47 R 12 -47 R 11 -46 R 12 -47 R 12 -47 R 11 -46 R 12 -46 R 12 -46 R 11 -46 R 12 -46 R 12 -46 R 11 -45 R 12 -46 R 12 -45 R 12 -45 R 11 -45 R 12 -45 R 12 -45 R 11 -44 R 12 -45 R 12 -44 R 11 -44 R 12 -45 R 12 -44 R 11 -43 R 12 -44 R 12 -44 R 11 -43 R 12 -43 R 12 -44 R 11 -43 R 12 -43 R 12 -42 R 11 -43 R 12 -43 R 12 -42 R 11 -42 R 12 -42 R 12 -42 R 11 -42 R 12 -42 R 12 -42 R 11 -41 R 12 -41 R 12 -42 R 11 -41 R 12 -41 R 12 -40 R 11 -41 R 12 -41 R 12 -40 R 11 -40 R 12 -40 R 12 -40 R 11 -40 R 12 -40 R 12 -40 R 11 -39 R 12 -39 R 12 -40 R 11 -39 R 12 -39 R 12 -38 R 11 -39 R 12 -39 R 12 -38 R 11 -38 R 12 -39 R 12 -38 R 11 -38 R 12 -37 R 12 -38 R 11 -38 R 12 -37 R 12 -37 R 11 -38 R 12 -37 R 12 -37 R 11 -36 R 12 -37 R 12 -37 R 11 -36 R 12 -36 R 12 -37 R 11 -36 R 12 -36 R 12 -35 R 11 -36 R 12 -36 R 12 -35 R 11 -36 R 12 -35 R 12 -35 R 11 -35 R 12 -35 R 12 -35 R 11 -34 R 12 -35 R 12 -34 R 11 -34 R 12 -35 R 12 -34 R 11 -34 R 12 -33 R 12 -34 R 11 -34 R 12 -33 R 12 -34 R 11 -33 R 12 -33 R 12 -33 R 11 -33 R 12 -33 R 12 -33 R 11 -32 R 12 -33 R 12 -32 R 11 -32 R 12 -33 R 12 -32 R 11 -32 R 12 -31 R 12 -32 R 11 -32 R 12 -31 R 12 -32 R 11 -31 R 12 -31 R 12 -31 R 11 -31 R 12 -31 R 12 -30 R 11 -31 R 12 -30 R 12 -31 R 11 -30 R 12 -30 R 12 -30 R 11 -30 R 12 -30 R 12 -29 R 11 -30 R 12 -29 R 12 -29 R 11 -29 R 12 -30 R 12 -28 R 11 -29 R 12 -29 R 12 -28 R 11 -29 R 12 -28 R 12 -28 R 11 -28 R 12 -28 R 12 -28 R 11 -28 R 12 -27 R 12 -28 R 11 -27 R 12 -27 R 12 -28 R 11 -27 R 12 -26 R 12 -27 R 11 -27 R 12 -26 R 12 -27 R 11 -26 R 12 -26 R 12 -26 R 12 -26 R 11 -25 R 12 -26 R 12 -25 R 11 -26 R 12 -25 R 12 -25 R 11 -25 R 12 -25 R 12 -25 R 11 -24 R 12 -25 R 12 -24 R 11 -24 R 12 -24 R 12 -24 R 11 -24 R 12 -24 R 12 -24 R 11 -23 R 12 -24 R 12 -23 R 11 -23 R 12 -23 R 12 -23 R 11 -23 R 12 -23 R 12 -22 R 11 -23 R 12 -22 R 12 -23 R 11 -22 R 12 -22 R 12 -22 R 11 -22 R 12 -21 R 12 -22 R 11 -22 R 12 -21 R 12 -21 R 11 -22 R 12 -21 R 12 -21 R 11 -21 R 12 -20 R 12 -21 R 11 -21 R 12 -20 R 12 -21 R 11 -20 R 12 -20 R 12 -20 R 11 -20 R 12 -20 R 12 -20 R 11 -20 R 12 -20 R 12 -19 R 11 -20 R 12 -19 R 12 -19 R 11 -19 R 12 -20 R 12 -19 R 11 -18 R 12 -19 R 12 -19 R 11 -19 R 12 -18 R 12 -19 R 11 -18 R 12 -18 R 12 -19 R 11 -18 R 12 -18 R 12 -18 R 11 -17 R 12 -18 R 12 -18 R 11 -17 R 12 -18 R 12 -17 R 11 -18 R 12 -17 R 12 -17 R 11 -17 R 12 -17 R 12 -16 R 11 -17 R 12 -17 R 12 -16 R 11 -16 R 12 -17 R 12 -16 R 11 -16 R 12 -16 R 12 -16 R 11 -16 R 12 -15 R 12 -16 R 11 -15 R 12 -15 R 12 -16 R 11 -15 R 12 -15 R 12 -15 R 11 -15 R 12 -14 R 12 -15 R 11 -14 R 12 -15 R 12 -14 R 11 -14 R 12 -14 R 12 -14 R 11 -14 R 12 -13 R 12 -14 R 11 -13 R 12 -14 R 12 -13 R 11 -13 R 12 -13 R 12 -13 R 11 -13 R 12 -12 R 12 -13 R 11 -12 R 12 -12 R 12 -13 R 11 -12 R 12 -12 R 12 -11 R 11 -12 R 12 -12 R 12 -11 R 11 -11 R 12 -12 R 12 -11 R 11 -11 R 12 -11 R 12 -10 R 11 -11 R 12 -11 R 12 -10 R 11 -11 R 12 -10 R 12 -10 R 11 -10 R 12 -10 R 12 -10 R 11 -10 R 12 -9 R 12 -10 R 12 -9 R 11 -10 R 12 -9 R 12 -9 R 11 -9 R 12 -9 R 12 -9 R 11 -9 R 12 -8 R 12 -9 R 11 -9 R 12 -8 R 12 -8 R 11 -9 R 12 -8 R 12 -8 R 11 -8 R 12 -8 R 12 -8 R 11 -8 R 12 -7 R 12 -8 R 11 -7 R 12 -8 R 12 -7 R 11 -8 R 12 -7 R 12 -7 R 11 -7 R 12 -7 R 12 -7 R 11 -7 R 12 -7 R 12 -6 R 11 -7 R 12 -7 R 12 -6 R 11 -7 R 12 -6 R 12 -6 R 11 -7 R 12 -6 R 12 -6 R 11 -6 R 12 -6 R 12 -6 R 11 -6 R 12 -6 R 12 -5 R 11 -6 R 12 -5 R 12 -6 R 11 -5 R 12 -6 R 12 -5 R 11 -5 R 12 -5 R 12 -5 R 11 -5 R 12 -5 R 12 -5 R 11 -4 R 12 -5 R 12 -4 R 11 -5 R 12 -4 R 12 -4 R 11 -4 R 12 -4 R 12 -4 R 11 -4 R 12 -4 R 12 -4 R 11 -3 R 12 -4 R 12 -3 R 11 -4 R 12 -3 R 12 -3 R 11 -3 R 12 -3 R 12 -3 R 11 -3 R 12 -2 R 12 -3 R 11 -2 R 12 -3 R 12 -2 R 11 -2 R 12 -2 R 12 -2 R 11 -2 R 12 -2 R 12 -1 R 11 -2 R 12 -1 R 12 -2 R 11 -1 R 12 -1 R 12 -1 R 11 -1 R 12 -1 R 12 0 R 11 -1 R 12 0 R 12 -1 R 11 0 R 12 0 R 12 0 R 11 0 R 12 0 R 12 1 R 11 0 R 12 0 R 12 1 R 11 1 R 12 0 R 12 1 R 11 1 R 12 1 R 12 1 R 11 1 R 12 2 R 12 1 R 11 2 R 12 1 R 12 2 R 11 2 R 12 1 R 12 2 R 11 2 R 12 2 R 12 3 R 11 2 R 12 2 R 12 3 R 11 2 R 12 3 R 12 2 R 11 3 R 12 3 R 12 3 R 11 3 R 12 3 R 12 3 R 11 3 R 12 3 R 12 4 R 11 3 R 12 3 R 12 4 R 11 3 R 12 4 R 12 4 R 11 4 R 12 3 R 12 4 R 12 4 R 11 4 R 12 4 R 12 5 R 11 4 R 12 4 R 12 4 R 11 5 R 12 4 R 12 5 R 11 4 R 12 5 R 12 5 R 11 4 R 12 5 R 12 5 R 11 5 R 12 5 R 12 5 R 11 5 R 12 5 R 12 5 R 11 6 R 12 5 R 12 6 R 11 5 R 12 6 R 12 5 R 11 6 R 12 6 R 12 6 R 11 5 R 12 6 R 12 6 R 11 7 R 12 6 R 12 6 R 11 6 R 12 7 R 12 6 R 11 7 R 12 6 R 12 7 R 11 7 R 12 6 R 12 7 R 11 7 R 12 7 R 12 7 R 11 8 R 12 7 R 12 7 R 11 8 R 12 7 R 12 8 R 11 7 R 12 8 R 12 8 R 11 8 R 12 7 R 12 8 R 11 9 R 12 8 R 12 8 R 11 8 R 12 9 R 12 8 R 11 9 R 12 8 R 12 9 R 11 9 R 12 9 R 12 9 R 11 9 R 12 9 R 12 9 R 11 9 R 12 9 R 12 10 R 11 9 R 12 10 R 12 10 R 11 9 R 12 10 R 12 10 R 11 10 R 12 10 R 12 10 R 11 11 R 12 10 R 12 10 R 11 11 R 12 10 R 12 11 R 11 11 R 12 10 R 12 11 R 11 11 R 12 11 R 12 11 R 11 12 R 12 11 R 12 11 R 11 12 R 12 11 R 12 12 R 11 11 R 12 12 R 12 12 R 11 12 R 12 12 R 12 12 R 11 12 R 12 12 R 12 13 R 11 12 R 12 13 R 12 12 R 11 13 R 12 13 R 12 12 R 11 13 R 12 13 R 12 13 R 11 13 R 12 14 R 12 13 R 11 13 R 12 14 R 12 13 R 11 14 R 12 14 R 12 14 R 11 13 R 12 14 R 12 14 R 11 15 R 12 14 R 12 14 R 11 14 R 12 15 R 12 14 R 11 15 R 12 15 R 12 14 R 11 15 R 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R 11 15 R 12 16 R 12 15 R 12 16 R 11 15 R 12 16 R 12 15 R 11 16 R 12 16 R 12 16 R 11 15 R 12 16 R 12 17 R 11 16 R 12 16 R 12 16 R 11 16 R 12 17 R 12 16 R 11 17 R 12 16 R 12 17 R 11 16 R 12 17 R 12 17 R 11 17 R 12 17 R 12 17 R 11 17 R 12 17 R 12 17 R 11 17 R 12 17 R 12 17 R 11 18 R 12 17 R 12 18 R 11 17 R 12 18 R 12 17 R 11 18 R 12 17 R 12 18 R 11 18 R 12 18 R 12 18 R 11 18 R 12 18 R 12 18 R 11 18 R 12 18 R 12 18 R 11 18 R 12 18 R 12 19 R 11 18 R 12 18 R 12 19 R 11 18 R 12 18 R 12 19 R 11 18 R 12 19 R 12 19 R 11 18 R 12 19 R 12 19 R 11 18 R D 16327 4078 M 12 19 R 12 19 R 11 18 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 20 R 12 19 R 11 19 R 12 19 R 12 19 R 11 20 R 12 19 R 12 19 R 11 19 R 12 19 R 12 20 R D L0 7375 12544 M -1 14 R -2 15 R -5 13 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 8 12 R 7 13 R 5 14 R 2 14 R 1 15 R D 8104 9548 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R 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30 R -15 15 R -30 16 R -61 0 R -30 -16 R -16 -15 R 0 -30 R 16 -15 R 30 -15 R 76 -31 R 30 -15 R 16 -15 R D 14130 11179 M 16 -15 R 30 -15 R 76 -31 R 30 -15 R 16 -15 R 0 -46 R -16 -15 R -30 -15 R -61 0 R -30 15 R -15 15 R -16 31 R 0 -61 R 16 30 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f11a.eps0100644000000000000000000012604610376206774011043 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/G020-024 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:07:44 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 1997 4200 M 0 182 R D 5564 4200 M 0 182 R D 9131 4200 M 0 182 R D 12697 4200 M 0 182 R D 16264 4200 M 0 182 R D 2889 4200 M 0 91 R D 3780 4200 M 0 91 R D 4672 4200 M 0 91 R D 6455 4200 M 0 91 R D 7347 4200 M 0 91 R D 8239 4200 M 0 91 R D 10022 4200 M 0 91 R D 10914 4200 M 0 91 R D 11806 4200 M 0 91 R D 13589 4200 M 0 91 R D 14481 4200 M 0 91 R D 15372 4200 M 0 91 R D 1800 13300 M 15300 0 R D 1997 13300 M 0 -182 R D 5564 13300 M 0 -182 R D 9131 13300 M 0 -182 R D 12697 13300 M 0 -182 R D 16264 13300 M 0 -182 R D 2889 13300 M 0 -91 R D 3780 13300 M 0 -91 R D 4672 13300 M 0 -91 R D 6455 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%%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 4367 4200 M 0 182 R D 7622 4200 M 0 182 R D 10878 4200 M 0 182 R D 14133 4200 M 0 182 R D 1925 4200 M 0 91 R D 2739 4200 M 0 91 R D 3553 4200 M 0 91 R D 5181 4200 M 0 91 R D 5994 4200 M 0 91 R D 6808 4200 M 0 91 R D 8436 4200 M 0 91 R D 9250 4200 M 0 91 R D 10064 4200 M 0 91 R D 11691 4200 M 0 91 R D 12505 4200 M 0 91 R D 13319 4200 M 0 91 R D 14947 4200 M 0 91 R D 15761 4200 M 0 91 R D 16574 4200 M 0 91 R D 1800 13300 M 15300 0 R D 4367 13300 M 0 -182 R D 7622 13300 M 0 -182 R D 10878 13300 M 0 -182 R D 14133 13300 M 0 -182 R D 1925 13300 M 0 -91 R D 2739 13300 M 0 -91 R D 3553 13300 M 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107 R D 17100 1400 M 0 2800 R D 17100 1680 M -306 0 R D 17100 2240 M -306 0 R D 17100 2800 M -306 0 R D 17100 3360 M -306 0 R D 17100 3920 M -306 0 R D 17100 1400 M -153 0 R D 17100 1540 M -153 0 R D 17100 1820 M -153 0 R D 17100 1960 M -153 0 R D 17100 2100 M -153 0 R D 17100 2380 M -153 0 R D 17100 2520 M -153 0 R D 17100 2660 M -153 0 R D 17100 2940 M -153 0 R D 17100 3080 M -153 0 R D 17100 3220 M -153 0 R D 17100 3500 M -153 0 R D 17100 3640 M -153 0 R D 17100 3780 M -153 0 R D 17100 4060 M -153 0 R D 17100 4200 M -153 0 R D 40 setlinewidth 1800 3260 M 290 584 R 436 -452 R 436 -1429 R 436 226 R 437 29 R 436 554 R 436 236 R 436 -227 R 436 -280 R 438 -385 R 436 340 R 437 596 R 436 -225 R 436 678 R 436 157 R 437 -545 R 436 69 R 438 -686 R 436 684 R 436 -1384 R 317 -400 R D 10893 1400 M 361 703 R 436 50 R 436 844 R 436 -1275 R 438 408 R 436 -11 R 436 -312 R 437 186 R 436 201 R 436 559 R 436 -769 R 437 -451 R 436 1053 R 438 -298 R 171 7 R D L1 1800 3263 M 290 585 R 436 -445 R 436 -1414 R 436 255 R 437 72 R 436 623 R 436 302 R 436 -185 R 436 -266 R 438 -506 R 436 146 R 437 367 R 436 -382 R 436 648 R 436 257 R 437 -338 R 436 299 R 438 -510 R 436 747 R 436 -1285 R 436 -557 R 437 924 R 436 63 R 436 880 R 436 -1311 R 438 333 R 436 -101 R 436 -421 R 437 99 R 436 135 R 436 519 R 436 -792 R 437 -462 R 436 1048 R 438 -300 R 171 7 R D L2 1800 3267 M 290 587 R 436 -437 R 436 -1394 R 436 300 R 437 128 R 436 709 R 436 395 R 436 -126 R 436 -291 R 438 -583 R 436 -85 R 437 88 R 436 -559 R 436 609 R 436 369 R 437 -140 R 436 470 R 438 -329 R 436 754 R 436 -1263 R 436 -466 R 437 920 R 436 165 R 436 872 R 436 -1302 R 438 255 R 436 -183 R 436 -502 R 437 22 R 436 88 R 436 487 R 436 -807 R 437 -470 R 436 1044 R 438 -301 R 171 5 R D 10 setlinewidth L1 1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f11c.eps0100644000000000000000000013772010376206774011046 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, %% /Users/martin/conv/output/1D/G020-024/figures %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:22:14 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 1400 M 15300 0 R D 2164 1400 M 0 238 R D 1481 850 M 273 0 R D 1952 1033 M -46 -16 R -30 -45 R -16 -76 R 0 -46 R 16 -76 R 30 -45 R 46 -15 R 30 0 R 46 15 R 30 45 R 15 76 R 0 46 R -15 76 R -30 45 R -46 16 R -30 0 R -31 -16 R -15 -15 R -15 -30 R -15 -76 R 0 -46 R 15 -76 R 15 -30 R 15 -15 R 31 -15 R D 1982 714 M 30 15 R 16 15 R 15 30 R 15 76 R 0 46 R -15 76 R -15 30 R -16 15 R -30 16 R D 2195 744 M -16 -15 R 16 -15 R 15 15 R -15 15 R D 2362 972 M 30 15 R 46 46 R 0 -319 R D 2423 1017 M 0 -303 R D 2362 714 M 136 0 R D 2711 1033 M -45 -16 R -31 -45 R -15 -76 R 0 -46 R 15 -76 R 31 -45 R 45 -15 R 30 0 R 46 15 R 30 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1124 7167 M 137 0 R D 1473 7486 M -45 -15 R -31 -46 R -15 -76 R 0 -45 R 15 -76 R 31 -46 R 45 -15 R 31 0 R 45 15 R 31 46 R 15 76 R 0 45 R -15 76 R -31 46 R -45 15 R -31 0 R -30 -15 R -15 -15 R -15 -31 R -16 -76 R 0 -45 R 16 -76 R 15 -31 R 15 -15 R 30 -15 R D 1504 7167 M 30 15 R 15 15 R 16 31 R 15 76 R 0 45 R -15 76 R -16 31 R -15 15 R -30 15 R D 1800 10325 M 306 0 R D 1124 10400 M 30 15 R 46 46 R 0 -319 R D 1185 10446 M 0 -304 R D 1124 10142 M 137 0 R D 1413 10461 M -31 -152 R 31 30 R 45 16 R 46 0 R 45 -16 R 31 -30 R 15 -46 R 0 -30 R -15 -45 R -31 -31 R -45 -15 R -46 0 R -45 15 R -16 15 R -15 31 R 0 15 R 15 15 R 16 -15 R -16 -15 R D 1504 10355 M 30 -16 R 31 -30 R 15 -46 R 0 -30 R -15 -45 R -31 -31 R -30 -15 R D 1413 10461 M 152 0 R D 1413 10446 M 76 0 R 76 15 R D 1800 13300 M 306 0 R D 1094 13238 M 15 -15 R -15 -15 R -15 15 R 0 15 R 15 30 R 15 15 R 45 16 R 61 0 R 46 -16 R 15 -15 R 15 -30 R 0 -30 R -15 -31 R -46 -30 R -76 -31 R -30 -15 R -30 -30 R -15 -46 R 0 -45 R D 1215 13299 M 31 -16 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R D 10290 12807 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 11018 9148 M -1 14 R -3 15 R -4 13 R -7 14 R -8 12 R -9 10 R -11 10 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -10 R -10 -10 R -8 -12 R -6 -14 R -5 -13 R -3 -15 R -1 -14 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -13 R 10 -10 R 11 -10 R 12 -8 R 13 -7 R 13 -4 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 10 R 9 10 R 8 13 R 7 13 R 4 13 R 3 15 R 1 14 R F 11747 6289 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R 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R 5 14 R 3 14 R 1 15 R F 13932 1708 M -1 14 R -2 15 R -5 13 R -6 13 R -9 13 R -9 10 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -10 R -8 -13 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 9 12 R 6 13 R 5 14 R 2 14 R 1 15 R F 14661 1400 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 10 R -13 8 R -13 6 R -13 5 R -15 3 R -14 0 R -14 0 R -15 -3 R -13 -5 R -13 -6 R -13 -8 R -10 -10 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 222 0 R F 15390 1646 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 0 R -15 0 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F 16118 2415 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -13 R 10 -10 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 10 R 8 13 R 7 13 R 4 13 R 3 15 R 1 14 R F 16847 3645 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -5 -13 R -2 -15 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F L0 10090 13299 M 6 -31 R 12 -66 R 11 -65 R 12 -66 R 12 -65 R 12 -66 R 11 -65 R 12 -64 R 12 -65 R 11 -64 R 12 -65 R 12 -64 R 11 -64 R 12 -63 R 12 -64 R 11 -63 R 12 -63 R 12 -63 R 11 -63 R 12 -63 R 12 -62 R 11 -62 R 12 -62 R 12 -62 R 11 -62 R 12 -61 R 12 -61 R 11 -61 R 12 -61 R 12 -61 R 11 -60 R 12 -61 R 12 -60 R 11 -60 R 12 -59 R 12 -60 R 11 -59 R 12 -59 R 12 -59 R 11 -59 R 12 -58 R 12 -58 R 11 -58 R 12 -58 R 12 -58 R 11 -57 R 12 -57 R 12 -57 R 11 -57 R 12 -57 R 12 -56 R 11 -56 R 12 -56 R 12 -56 R 11 -56 R 12 -55 R 12 -55 R 11 -55 R 12 -55 R 12 -54 R 11 -54 R 12 -54 R 12 -54 R 11 -54 R 12 -53 R 12 -53 R 11 -53 R 12 -53 R 12 -53 R 11 -52 R 12 -52 R 12 -52 R 11 -51 R 12 -52 R 12 -51 R 11 -51 R 12 -51 R 12 -50 R 11 -51 R 12 -50 R 12 -50 R 11 -49 R 12 -50 R 12 -49 R 11 -49 R 12 -49 R 12 -49 R 11 -48 R 12 -48 R 12 -48 R 11 -48 R 12 -48 R 12 -47 R 11 -48 R 12 -47 R 12 -46 R 11 -47 R 12 -46 R 12 -47 R 11 -46 R 12 -46 R 12 -45 R 11 -46 R 12 -45 R 12 -45 R 11 -45 R 12 -45 R 12 -44 R 11 -45 R 12 -44 R 12 -44 R 11 -44 R 12 -43 R 12 -44 R 11 -43 R 12 -43 R 12 -43 R 11 -43 R 12 -42 R 12 -43 R 11 -42 R 12 -42 R 12 -42 R 11 -42 R 12 -41 R 12 -42 R 11 -41 R 12 -41 R 12 -41 R 11 -41 R 12 -40 R 12 -40 R 11 -41 R 12 -40 R 12 -40 R 11 -39 R 12 -40 R 12 -40 R 11 -39 R 12 -39 R 12 -39 R 11 -39 R 12 -38 R 12 -39 R 11 -38 R 12 -38 R 12 -38 R 11 -38 R 12 -38 R 12 -37 R 11 -37 R 12 -38 R 12 -37 R 11 -36 R 12 -37 R 12 -36 R 11 -37 R 12 -36 R 12 -36 R 12 -36 R 11 -35 R 12 -36 R 12 -35 R 11 -35 R 12 -35 R 12 -35 R 11 -35 R 12 -34 R 12 -34 R 11 -34 R 12 -34 R 12 -34 R 11 -34 R 12 -33 R 12 -33 R 11 -33 R 12 -33 R 12 -33 R 11 -33 R 12 -32 R 12 -32 R 11 -32 R 12 -32 R 12 -32 R 11 -31 R 12 -31 R 12 -31 R 11 -31 R 12 -31 R 12 -31 R 11 -30 R 12 -30 R 12 -30 R 11 -30 R 12 -30 R 12 -29 R 11 -30 R 12 -29 R 12 -29 R 11 -29 R 12 -28 R 12 -29 R 11 -28 R 12 -28 R 12 -28 R 11 -27 R 12 -28 R 12 -27 R 11 -27 R 12 -27 R 12 -27 R 11 -27 R 12 -26 R 12 -27 R 11 -26 R 12 -26 R 12 -25 R 11 -26 R 12 -25 R 12 -26 R 11 -25 R 12 -25 R 12 -24 R 11 -25 R 12 -24 R 12 -25 R 11 -24 R 12 -24 R 12 -23 R 11 -24 R 12 -23 R 12 -24 R 11 -23 R 12 -23 R 12 -22 R 11 -23 R 12 -22 R 12 -23 R 11 -22 R 12 -22 R 12 -21 R 11 -22 R 12 -21 R 12 -22 R 11 -21 R 12 -21 R 12 -21 R 11 -20 R 12 -21 R 12 -20 R 11 -20 R 12 -20 R 12 -20 R 11 -20 R 12 -19 R 12 -20 R 11 -19 R 12 -19 R 12 -19 R 11 -19 R 12 -18 R 12 -19 R 11 -18 R 12 -18 R 12 -18 R 11 -18 R 12 -18 R 12 -18 R 11 -17 R 12 -17 R 12 -17 R 11 -17 R 12 -17 R 12 -17 R 11 -16 R 12 -16 R 12 -17 R 11 -16 R 12 -16 R 12 -15 R 11 -16 R 12 -15 R 12 -16 R 11 -15 R 12 -15 R 12 -14 R 11 -15 R 12 -15 R 12 -14 R 11 -14 R 12 -14 R 12 -14 R 11 -14 R 12 -13 R 12 -14 R 11 -13 R 12 -13 R 12 -13 R 11 -13 R 12 -13 R 12 -12 R 11 -13 R 12 -12 R 12 -12 R 11 -12 R 12 -12 R 12 -11 R 11 -12 R 12 -11 R 12 -11 R 11 -11 R 12 -11 R 12 -11 R 11 -10 R 12 -11 R 12 -10 R 12 -10 R 11 -10 R 12 -10 R 12 -10 R 11 -9 R 12 -10 R 12 -9 R 11 -9 R 12 -9 R 12 -8 R 11 -9 R 12 -9 R 12 -8 R 11 -8 R 12 -8 R 12 -8 R 11 -8 R 12 -7 R 12 -8 R 11 -7 R 12 -7 R 12 -7 R 11 -7 R 12 -6 R 12 -7 R 11 -6 R 12 -7 R 12 -6 R 11 -6 R 12 -5 R 12 -6 R 11 -5 R 12 -6 R 12 -5 R 11 -5 R 12 -5 R 12 -5 R 11 -4 R 12 -5 R 12 -4 R 11 -4 R 12 -4 R 12 -4 R 11 -4 R 12 -3 R 12 -4 R 11 -3 R 12 -3 R 12 -3 R 11 -3 R 12 -3 R 12 -2 R 11 -3 R 12 -2 R 12 -2 R 11 -2 R 12 -2 R 12 -2 R 11 -1 R 12 -2 R 12 -1 R 11 -1 R 12 -1 R 12 -1 R 11 -1 R 12 0 R 12 -1 R 11 0 R 12 0 R 12 0 R 11 0 R 12 0 R 12 1 R 11 1 R 12 0 R 12 1 R 11 1 R 12 1 R 12 2 R 11 1 R 12 2 R 12 1 R 11 2 R 12 2 R 12 2 R 11 3 R 12 2 R 12 3 R 11 2 R 12 3 R 12 3 R 11 3 R 12 3 R 12 4 R 11 3 R 12 4 R 12 4 R 11 4 R 12 4 R 12 4 R 11 4 R 12 5 R 12 4 R 11 5 R 12 5 R 12 5 R 11 5 R 12 5 R 12 6 R 11 5 R 12 6 R 12 6 R 11 6 R 12 6 R 12 6 R 11 6 R 12 7 R 12 6 R 11 7 R 12 7 R 12 7 R 11 7 R 12 7 R 12 8 R 11 7 R 12 8 R 12 8 R 11 7 R 12 8 R 12 9 R 11 8 R 12 8 R 12 9 R 11 9 R 12 8 R 12 9 R 11 9 R 12 10 R 12 9 R 11 9 R 12 10 R 12 10 R 11 10 R 12 10 R 12 10 R 11 10 R 12 10 R 12 11 R 11 11 R 12 10 R 12 11 R 11 11 R 12 12 R 12 11 R 12 11 R 11 12 R 12 12 R 12 12 R 11 12 R 12 12 R 12 12 R 11 12 R 12 13 R 12 13 R 11 13 R 12 13 R 12 13 R 11 13 R 12 13 R 12 14 R 11 14 R 12 13 R 12 14 R 11 14 R 12 15 R 12 14 R 11 14 R 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R 11 16 R 12 15 R 12 16 R 11 16 R 12 15 R 12 17 R 11 16 R 12 16 R 12 17 R 11 16 R 12 17 R 12 17 R 11 17 R 12 17 R 12 18 R 11 17 R 12 18 R 12 18 R 11 18 R 12 18 R 12 18 R 11 18 R 12 18 R 12 19 R 11 18 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 20 R 11 19 R 12 20 R 12 19 R 11 20 R 12 20 R 12 20 R 11 20 R 12 20 R 12 20 R 11 20 R 12 21 R 12 20 R 11 20 R 12 21 R 12 20 R 11 21 R 12 20 R 12 21 R 11 21 R 12 21 R 12 20 R 11 21 R 12 21 R 12 21 R 11 21 R 12 21 R 12 21 R 11 21 R 12 21 R 12 21 R 11 21 R 12 22 R 12 21 R 11 21 R 12 21 R 12 21 R 11 21 R 12 22 R 12 21 R D 11018 12222 M -1 14 R -3 15 R -4 13 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 13 -4 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 15 R D 11747 8717 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -15 R 5 -13 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 13 R 3 15 R 1 14 R D 12475 5950 M -1 15 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 5 13 R 2 15 R 1 14 R D 13204 3890 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -13 4 R 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7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D L2 10711 13299 M 4 -18 R 11 -65 R 12 -66 R 12 -65 R 11 -66 R 12 -65 R 12 -64 R 11 -65 R 12 -64 R 12 -65 R 11 -64 R 12 -63 R 12 -64 R 11 -63 R 12 -63 R 12 -63 R 11 -63 R 12 -62 R 12 -63 R 11 -62 R 12 -61 R 12 -62 R 11 -61 R 12 -62 R 12 -61 R 11 -60 R 12 -61 R 12 -60 R 11 -61 R 12 -59 R 12 -60 R 11 -60 R 12 -59 R 12 -59 R 11 -59 R 12 -59 R 12 -58 R 11 -59 R 12 -58 R 12 -58 R 11 -57 R 12 -58 R 12 -57 R 11 -57 R 12 -57 R 12 -57 R 11 -56 R 12 -57 R 12 -56 R 11 -56 R 12 -55 R 12 -56 R 11 -55 R 12 -55 R 12 -55 R 11 -55 R 12 -54 R 12 -55 R 11 -54 R 12 -54 R 12 -54 R 11 -53 R 12 -54 R 12 -53 R 11 -53 R 12 -53 R 12 -52 R 11 -53 R 12 -52 R 12 -52 R 11 -52 R 12 -51 R 12 -52 R 11 -51 R 12 -51 R 12 -51 R 11 -51 R 12 -50 R 12 -51 R 11 -50 R 12 -50 R 12 -50 R 11 -49 R 12 -50 R 12 -49 R 11 -49 R 12 -49 R 12 -49 R 11 -48 R 12 -49 R 12 -48 R 11 -48 R 12 -48 R 12 -47 R 11 -48 R 12 -47 R 12 -47 R 11 -47 R 12 -47 R 12 -46 R 11 -46 R 12 -47 R 12 -46 R 11 -45 R 12 -46 R 12 -45 R 12 -45 R 11 -45 R 12 -45 R 12 -45 R 11 -44 R 12 -45 R 12 -44 R 11 -44 R 12 -43 R 12 -44 R 11 -43 R 12 -43 R 12 -43 R 11 -43 R 12 -43 R 12 -42 R 11 -42 R 12 -42 R 12 -42 R 11 -42 R 12 -41 R 12 -42 R 11 -41 R 12 -40 R 12 -41 R 11 -41 R 12 -40 R 12 -40 R 11 -40 R 12 -40 R 12 -39 R 11 -40 R 12 -39 R 12 -39 R 11 -39 R 12 -38 R 12 -39 R 11 -38 R 12 -38 R 12 -38 R 11 -38 R 12 -37 R 12 -37 R 11 -38 R 12 -37 R 12 -36 R 11 -37 R 12 -36 R 12 -36 R 11 -36 R 12 -36 R 12 -36 R 11 -35 R 12 -36 R 12 -35 R 11 -35 R 12 -35 R 12 -34 R 11 -35 R 12 -34 R 12 -34 R 11 -34 R 12 -34 R 12 -33 R 11 -34 R 12 -33 R 12 -33 R 11 -33 R 12 -32 R 12 -33 R 11 -32 R 12 -33 R 12 -32 R 11 -32 R 12 -31 R 12 -32 R 11 -31 R 12 -32 R 12 -31 R 11 -31 R 12 -30 R 12 -31 R 11 -30 R 12 -31 R 12 -30 R 11 -30 R 12 -30 R 12 -29 R 11 -30 R 12 -29 R 12 -29 R 11 -30 R 12 -28 R 12 -29 R 11 -29 R 12 -28 R 12 -29 R 11 -28 R 12 -28 R 12 -28 R 11 -28 R 12 -27 R 12 -28 R 11 -27 R 12 -27 R 12 -27 R 11 -27 R 12 -27 R 12 -26 R 11 -27 R 12 -26 R 12 -26 R 11 -26 R 12 -26 R 12 -26 R 11 -25 R 12 -26 R 12 -25 R 11 -25 R 12 -25 R 12 -24 R 11 -25 R 12 -24 R 12 -25 R 11 -24 R 12 -24 R 12 -24 R 11 -23 R 12 -24 R 12 -23 R 11 -23 R 12 -23 R 12 -23 R 11 -23 R 12 -22 R 12 -23 R 11 -22 R 12 -22 R 12 -22 R 11 -21 R 12 -22 R 12 -21 R 11 -21 R 12 -21 R 12 -21 R 11 -21 R 12 -20 R 12 -21 R 11 -20 R 12 -20 R 12 -20 R 11 -19 R 12 -20 R 12 -19 R 11 -19 R 12 -19 R 12 -19 R 12 -18 R 11 -19 R 12 -18 R 12 -18 R 11 -18 R 12 -18 R 12 -17 R 11 -18 R 12 -17 R 12 -17 R 11 -17 R 12 -16 R 12 -17 R 11 -16 R 12 -16 R 12 -16 R 11 -16 R 12 -16 R 12 -15 R 11 -16 R 12 -15 R 12 -15 R 11 -15 R 12 -14 R 12 -15 R 11 -14 R 12 -14 R 12 -14 R 11 -14 R 12 -14 R 12 -13 R 11 -13 R 12 -14 R 12 -13 R 11 -12 R 12 -13 R 12 -13 R 11 -12 R 12 -12 R 12 -12 R 11 -12 R 12 -12 R 12 -12 R 11 -11 R 12 -11 R 12 -11 R 11 -11 R 12 -11 R 12 -11 R 11 -11 R 12 -10 R 12 -10 R 11 -10 R 12 -10 R 12 -10 R 11 -10 R 12 -9 R 12 -10 R 11 -9 R 12 -9 R 12 -9 R 11 -9 R 12 -8 R 12 -9 R 11 -8 R 12 -8 R 12 -9 R 11 -8 R 12 -7 R 12 -8 R 11 -8 R 12 -7 R 12 -7 R 11 -7 R 12 -7 R 12 -7 R 11 -7 R 12 -7 R 12 -6 R 11 -6 R 12 -7 R 12 -6 R 11 -6 R 12 -5 R 12 -6 R 11 -6 R 12 -5 R 12 -5 R 11 -5 R 12 -5 R 12 -5 R 11 -5 R 12 -4 R 12 -5 R 11 -4 R 12 -5 R 12 -4 R 11 -4 R 12 -3 R 12 -4 R 11 -4 R 12 -3 R 12 -3 R 11 -3 R 12 -4 R 12 -2 R 11 -3 R 12 -3 R 12 -2 R 11 -3 R 12 -2 R 12 -2 R 11 -2 R 12 -2 R 12 -2 R 11 -2 R 12 -1 R 12 -2 R 11 -1 R 12 -1 R 12 -1 R 11 -1 R 12 -1 R 12 0 R 11 -1 R 12 0 R 12 -1 R 11 0 R 12 0 R 12 0 R 11 0 R 12 1 R 12 0 R 11 1 R 12 0 R 12 1 R 11 1 R 12 1 R 12 1 R 11 2 R 12 1 R 12 2 R 11 1 R 12 2 R 12 2 R 11 2 R 12 3 R 12 2 R 11 2 R 12 3 R 12 3 R 11 3 R 12 3 R 12 3 R 12 4 R 11 3 R 12 4 R 12 4 R 11 4 R 12 4 R 12 4 R 11 5 R 12 4 R 12 5 R 11 5 R 12 5 R 12 5 R 11 6 R 12 5 R 12 6 R 11 6 R 12 6 R 12 6 R 11 6 R 12 7 R 12 6 R 11 7 R 12 7 R 12 8 R 11 7 R 12 7 R 12 8 R 11 8 R 12 8 R 12 8 R 11 9 R 12 8 R 12 9 R 11 9 R 12 9 R 12 9 R 11 10 R 12 10 R 12 9 R 11 10 R 12 11 R 12 10 R 11 10 R 12 11 R 12 11 R 11 11 R 12 11 R 12 11 R 11 12 R 12 12 R 12 11 R 11 12 R 12 12 R 12 12 R 11 13 R 12 12 R 12 13 R 11 12 R 12 13 R 12 13 R 11 13 R 12 13 R 12 13 R 11 14 R 12 13 R 12 14 R 11 13 R 12 14 R 12 14 R 11 14 R 12 14 R 12 14 R 11 14 R 12 15 R 12 14 R 11 14 R 12 15 R 12 14 R 11 15 R 12 14 R 12 15 R 11 15 R 12 15 R 12 14 R 11 15 R 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R 11 15 R 12 16 R 12 15 R 11 15 R 12 15 R 12 15 R 11 15 R 12 16 R 12 15 R D L0 9339 13299 M 1 -10 R 3 -15 R 4 -13 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 12 -8 R 14 -6 R 13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 14 6 R 12 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 13 R 3 15 R 0 10 R D 10290 9552 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 5 R -14 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R D 11018 6539 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 9 R -13 6 R -14 5 R -14 2 R -15 1 R -14 -1 R -15 -2 R -13 -5 R -13 -6 R -12 -9 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R D 11747 4295 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -15 R 5 -13 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 13 R 3 15 R 1 14 R D 12475 2696 M -1 15 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 9 R -13 6 R -14 5 R -14 2 R -15 1 R -14 -1 R -14 -2 R -14 -5 R -13 -6 R -12 -9 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 5 14 R 2 14 R 1 14 R D 13204 1774 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -13 4 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 4 -13 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 13 R 3 15 R 1 14 R D 13932 1405 M -1 15 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 0 -5 R D 13931 1400 M 1 5 R D 14661 1620 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -13 9 R -13 6 R -13 5 R -15 2 R -14 1 R -14 -1 R -15 -2 R -13 -5 R -13 -6 R -13 -9 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 13 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R D 15390 2358 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R D 16118 3557 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -9 R 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12 -59 R 11 -58 R 12 -59 R 12 -58 R 11 -57 R 12 -58 R 12 -58 R 11 -57 R 12 -57 R 12 -57 R 11 -57 R 12 -56 R 12 -57 R 11 -56 R 12 -56 R 12 -56 R 11 -55 R 12 -56 R 12 -55 R 11 -55 R 12 -55 R 12 -55 R 12 -55 R 11 -54 R 12 -54 R 12 -54 R 11 -54 R 12 -54 R 12 -53 R 11 -54 R 12 -53 R 12 -53 R 11 -53 R 12 -52 R 12 -53 R 11 -52 R 12 -52 R 12 -52 R 11 -52 R 12 -51 R 12 -52 R 11 -51 R 12 -51 R 12 -51 R 11 -50 R 12 -51 R 12 -50 R 11 -50 R 12 -50 R 12 -50 R 11 -49 R 12 -49 R 12 -49 R 11 -49 R 12 -49 R 12 -49 R 11 -48 R 12 -48 R 12 -48 R 11 -48 R 12 -47 R 12 -48 R 11 -47 R 12 -47 R 12 -46 R 11 -47 R 12 -46 R 12 -46 R 11 -46 R 12 -46 R 12 -46 R 11 -45 R 12 -45 R 12 -45 R 11 -45 R 12 -44 R 12 -44 R 11 -44 R 12 -44 R 12 -44 R 11 -43 R 12 -44 R 12 -43 R 11 -42 R 12 -43 R 12 -42 R 11 -43 R 12 -42 R 12 -41 R 11 -42 R 12 -41 R 12 -41 R 11 -41 R 12 -41 R 12 -40 R 11 -41 R 12 -40 R 12 -39 R 11 -40 R 12 -40 R 12 -39 R 11 -39 R 12 -39 R 12 -38 R 11 -39 R 12 -38 R 12 -38 R 11 -38 R 12 -38 R 12 -37 R 11 -37 R 12 -37 R 12 -37 R 11 -37 R 12 -37 R 12 -36 R 11 -36 R 12 -36 R 12 -36 R 11 -36 R 12 -35 R 12 -35 R 11 -35 R 12 -35 R 12 -35 R 11 -35 R 12 -34 R 12 -34 R 11 -34 R 12 -34 R 12 -34 R 11 -33 R 12 -34 R 12 -33 R 11 -33 R 12 -33 R 12 -33 R 11 -32 R 12 -33 R 12 -32 R 11 -32 R 12 -32 R 12 -32 R 11 -31 R 12 -32 R 12 -31 R 11 -31 R 12 -31 R 12 -31 R 11 -31 R 12 -30 R 12 -31 R 11 -30 R 12 -30 R 12 -30 R 11 -30 R 12 -30 R 12 -29 R 11 -30 R 12 -29 R 12 -29 R 11 -29 R 12 -29 R 12 -28 R 11 -29 R 12 -28 R 12 -28 R 11 -28 R 12 -28 R 12 -27 R 11 -28 R 12 -27 R 12 -27 R 11 -27 R 12 -27 R 12 -27 R 12 -26 R 11 -27 R 12 -26 R 12 -26 R 11 -26 R 12 -25 R 12 -26 R 11 -25 R 12 -25 R 12 -25 R 11 -25 R 12 -25 R 12 -24 R 11 -25 R 12 -24 R 12 -24 R 11 -23 R 12 -24 R 12 -23 R 11 -24 R 12 -23 R 12 -22 R 11 -23 R 12 -23 R 12 -22 R 11 -22 R 12 -22 R 12 -22 R 11 -21 R 12 -22 R 12 -21 R 11 -21 R 12 -21 R 12 -20 R 11 -21 R 12 -20 R 12 -20 R 11 -20 R 12 -20 R 12 -19 R 11 -19 R 12 -19 R 12 -19 R 11 -19 R 12 -19 R 12 -18 R 11 -18 R 12 -18 R 12 -18 R 11 -18 R 12 -17 R 12 -17 R 11 -18 R 12 -17 R 12 -16 R 11 -17 R 12 -16 R 12 -17 R 11 -16 R 12 -16 R 12 -15 R 11 -16 R 12 -15 R 12 -16 R 11 -15 R 12 -15 R 12 -14 R 11 -15 R 12 -14 R 12 -15 R 11 -14 R 12 -14 R 12 -14 R 11 -13 R 12 -14 R 12 -13 R 11 -13 R 12 -14 R 12 -12 R 11 -13 R 12 -13 R 12 -12 R 11 -13 R 12 -12 R 12 -12 R 11 -12 R 12 -12 R 12 -11 R 11 -12 R 12 -11 R 12 -12 R 11 -11 R 12 -11 R 12 -10 R 11 -11 R 12 -11 R 12 -10 R 11 -11 R 12 -10 R 12 -10 R 11 -10 R 12 -10 R 12 -9 R 11 -10 R 12 -9 R 12 -10 R 11 -9 R 12 -9 R 12 -9 R 11 -9 R 12 -8 R 12 -9 R 11 -8 R 12 -9 R 12 -8 R 11 -8 R 12 -8 R 12 -7 R 11 -8 R 12 -7 R 12 -8 R 11 -7 R 12 -7 R 12 -7 R 11 -7 R 12 -6 R 12 -7 R 11 -6 R 12 -6 R 12 -7 R 11 -5 R 12 -6 R 12 -6 R 11 -5 R 12 -6 R 12 -5 R 11 -5 R 12 -5 R 12 -5 R 11 -4 R 12 -5 R 12 -4 R 11 -4 R 12 -4 R 12 -4 R 11 -4 R 12 -4 R 12 -3 R 11 -3 R 12 -3 R 12 -3 R 11 -3 R 12 -3 R 12 -2 R 11 -3 R 12 -2 R 12 -2 R 12 -2 R 11 -2 R 12 -1 R 12 -2 R 11 -1 R 12 -1 R 12 -1 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15 R D 12201 11194 M -45 -15 R -15 -15 R -16 -30 R 0 -61 R 16 -31 R 15 -15 R 45 -15 R 61 0 R 46 15 R 15 15 R 15 31 R 0 61 R -15 30 R -15 15 R -46 15 R D 12201 11194 M -30 -15 R -15 -15 R -15 -30 R 0 -61 R 15 -31 R 15 -15 R 30 -15 R D 12262 11012 M 31 15 R 15 15 R 15 31 R 0 61 R -15 30 R -15 15 R -31 15 R D 12429 11331 M 0 -91 R D 12429 11270 M 15 31 R 31 30 R 30 0 R 76 -46 R 31 0 R 15 16 R 15 30 R D 12444 11301 M 31 15 R 30 0 R 76 -31 R D 12642 11331 M 0 -46 R -15 -45 R -61 -76 R -15 -30 R -15 -46 R 0 -76 R D 12627 11240 M -76 -76 R -15 -30 R -16 -46 R 0 -76 R D 13006 11331 M 0 -319 R D 13022 11331 M 0 -319 R D 13174 11225 M -152 -152 R D 13098 11134 M 91 -122 R D 13082 11134 M 92 -122 R D 12961 11331 M 61 0 R D 13128 11225 M 91 0 R D 12961 11012 M 106 0 R D 13128 11012 M 91 0 R D 13325 11225 M 0 -213 R D 13341 11225 M 0 -213 R D 13341 11179 M 30 30 R 46 16 R 30 0 R 45 -16 R 16 -30 R 0 -167 R D 13447 11225 M 30 -16 R 15 -30 R 0 -167 R D 13508 11179 M 30 30 R 46 16 R 30 0 R 46 -16 R 15 -30 R 0 -167 R D 13614 11225 M 30 -16 R 16 -30 R 0 -167 R D 13280 11225 M 61 0 R D 13280 11012 M 106 0 R D 13447 11012 M 106 0 R D 13614 11012 M 106 0 R D 14055 11392 M -274 -502 R D 14282 11194 M 16 31 R 0 -61 R -16 30 R -15 15 R -30 16 R -61 0 R -30 -16 R -16 -15 R 0 -30 R 16 -15 R 30 -15 R 76 -31 R 30 -15 R 16 -15 R D 14130 11179 M 16 -15 R 30 -15 R 76 -31 R 30 -15 R 16 -15 R 0 -46 R -16 -15 R -30 -15 R -61 0 R -30 15 R -15 15 R -16 31 R 0 -61 R 16 30 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f12a.eps0100644000000000000000000012505310376206774011041 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/LP815-43 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:07:48 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 1997 4200 M 0 182 R D 5564 4200 M 0 182 R D 9131 4200 M 0 182 R D 12697 4200 M 0 182 R D 16264 4200 M 0 182 R D 2889 4200 M 0 91 R D 3780 4200 M 0 91 R D 4672 4200 M 0 91 R D 6455 4200 M 0 91 R D 7347 4200 M 0 91 R D 8239 4200 M 0 91 R D 10022 4200 M 0 91 R D 10914 4200 M 0 91 R D 11806 4200 M 0 91 R D 13589 4200 M 0 91 R D 14481 4200 M 0 91 R D 15372 4200 M 0 91 R D 1800 13300 M 15300 0 R D 1997 13300 M 0 -182 R D 5564 13300 M 0 -182 R D 9131 13300 M 0 -182 R D 12697 13300 M 0 -182 R D 16264 13300 M 0 -182 R D 2889 13300 M 0 -91 R D 3780 13300 M 0 -91 R D 4672 13300 M 0 -91 R D 6455 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%%DocumentNeededResources: font Times-Roman %%EOF f12b.eps0100644000000000000000000013250310376206774011040 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/LP815-43 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 14:51:57 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 4276 4200 M 0 182 R D 7531 4200 M 0 182 R D 10786 4200 M 0 182 R D 14042 4200 M 0 182 R D 1834 4200 M 0 91 R D 2648 4200 M 0 91 R D 3462 4200 M 0 91 R D 5090 4200 M 0 91 R D 5903 4200 M 0 91 R D 6717 4200 M 0 91 R D 8345 4200 M 0 91 R D 9159 4200 M 0 91 R D 9973 4200 M 0 91 R D 11600 4200 M 0 91 R D 12414 4200 M 0 91 R D 13228 4200 M 0 91 R D 14856 4200 M 0 91 R D 15669 4200 M 0 91 R D 16483 4200 M 0 91 R D 1800 13300 M 15300 0 R D 4276 13300 M 0 -182 R D 7531 13300 M 0 -182 R D 10786 13300 M 0 -182 R D 14042 13300 M 0 -182 R D 1834 13300 M 0 -91 R D 2648 13300 M 0 -91 R D 3462 13300 M 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All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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R 3 14 R 1 15 R F 11018 2433 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -13 R 10 -10 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 10 R 8 13 R 7 13 R 4 13 R 3 15 R 1 14 R F 11747 1781 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 9 R -13 6 R -14 5 R -14 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -6 R -12 -9 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F 12475 1456 M -1 14 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R 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3 -14 R 4 -14 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 13 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R F 15390 2922 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -9 -12 R -6 -13 R -5 -13 R -2 -15 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 16118 3899 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R F 16847 5072 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -15 R 5 -13 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 13 R 3 15 R 1 14 R F L0 6760 13299 M 11 -44 R 11 -51 R 12 -50 R 12 -50 R 11 -50 R 12 -50 R 12 -50 R 11 -50 R 12 -49 R 12 -50 R 11 -49 R 12 -49 R 12 -49 R 11 -49 R 12 -49 R 12 -49 R 11 -48 R 12 -49 R 12 -48 R 11 -48 R 12 -48 R 12 -48 R 11 -48 R 12 -48 R 12 -48 R 11 -47 R 12 -47 R 12 -47 R 11 -48 R 12 -46 R 12 -47 R 11 -47 R 12 -47 R 12 -46 R 11 -46 R 12 -46 R 12 -46 R 11 -46 R 12 -46 R 12 -46 R 11 -45 R 12 -45 R 12 -46 R 11 -45 R 12 -45 R 12 -44 R 11 -45 R 12 -45 R 12 -44 R 11 -44 R 12 -44 R 12 -44 R 11 -44 R 12 -44 R 12 -44 R 11 -43 R 12 -43 R 12 -44 R 11 -43 R 12 -43 R 12 -43 R 11 -42 R 12 -43 R 12 -42 R 11 -43 R 12 -42 R 12 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R 12 0 R 12 1 R 11 1 R 12 1 R 12 1 R 11 1 R 12 1 R 12 1 R 11 2 R 12 1 R 12 2 R 11 1 R 12 2 R 12 2 R 11 1 R 12 2 R 12 2 R 11 2 R 12 3 R 12 2 R 11 2 R 12 3 R 12 2 R 11 3 R 12 2 R 12 3 R 11 3 R 12 3 R 12 3 R 11 3 R 12 3 R 12 3 R 11 3 R 12 3 R 12 4 R 11 3 R 12 4 R 12 4 R 11 3 R 12 4 R 12 4 R 11 4 R 12 4 R 12 4 R 11 4 R 12 4 R 12 4 R 11 4 R 12 5 R 12 4 R 11 5 R 12 4 R 12 5 R 11 5 R 12 4 R 12 5 R 11 5 R 12 5 R 12 5 R 11 5 R 12 5 R 12 5 R 11 5 R 12 6 R 12 5 R 11 5 R 12 6 R 12 5 R 11 6 R 12 5 R 12 6 R 11 6 R 12 6 R 12 5 R 12 6 R 11 6 R 12 6 R 12 6 R 11 6 R 12 6 R 12 6 R 11 7 R 12 6 R 12 6 R 11 7 R 12 6 R 12 6 R 11 7 R 12 7 R 12 6 R 11 7 R 12 7 R 12 6 R 11 7 R 12 7 R 12 7 R 11 7 R 12 7 R 12 7 R 11 7 R 12 8 R 12 7 R 11 7 R 12 8 R 12 7 R 11 8 R 12 7 R 12 8 R 11 7 R 12 8 R 12 8 R 11 8 R 12 8 R 12 8 R 11 8 R 12 8 R 12 8 R 11 9 R 12 8 R 12 8 R 11 9 R 12 8 R 12 9 R 11 9 R 12 8 R 12 9 R 11 9 R 12 9 R 12 9 R 11 9 R 12 9 R 12 9 R 11 10 R 12 9 R 12 9 R 11 10 R 12 9 R 12 10 R 11 10 R 12 10 R 12 9 R 11 10 R 12 10 R 12 11 R 11 10 R 12 10 R 12 10 R 11 11 R 12 10 R 12 11 R 11 10 R 12 11 R 12 11 R 11 11 R 12 10 R 12 11 R 11 11 R 12 11 R 12 12 R 11 11 R 12 11 R 12 12 R 11 11 R 12 12 R 12 11 R 11 12 R 12 11 R 12 12 R 11 12 R 12 12 R 12 12 R 11 12 R 12 12 R 12 12 R 11 12 R 12 13 R 12 12 R 11 12 R 12 13 R 12 12 R 11 13 R 12 13 R 12 12 R 11 13 R 12 13 R 12 13 R 11 13 R 12 13 R 12 13 R 11 13 R 12 13 R 12 14 R 11 13 R 12 13 R 12 14 R 11 13 R 12 14 R 12 13 R 11 14 R 12 14 R 12 13 R 11 14 R 12 14 R 12 14 R 11 14 R 12 14 R 12 14 R 11 14 R 12 14 R 12 15 R 11 14 R 12 14 R 12 15 R 11 14 R 12 15 R 12 14 R 11 15 R 12 15 R 12 14 R 11 15 R 12 15 R 12 15 R 11 15 R D 15510 3209 M 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R 12 16 R 11 15 R 12 15 R 12 16 R 11 15 R 12 16 R 12 16 R 11 15 R 12 16 R 12 16 R 11 16 R 12 16 R 12 16 R 11 16 R 12 16 R 12 16 R 11 16 R 12 17 R 12 16 R 11 16 R 12 17 R 12 16 R 11 17 R 12 17 R 12 16 R 11 17 R 12 17 R 12 17 R 11 17 R 12 17 R 12 17 R 11 17 R 12 17 R 12 17 R 11 18 R 12 17 R 12 17 R 11 18 R 12 17 R 12 18 R 11 18 R 12 18 R 12 17 R 11 18 R 12 18 R 12 18 R 11 18 R 12 18 R 12 18 R 11 18 R 12 19 R 12 18 R 11 18 R 12 19 R 12 18 R 11 18 R 12 19 R 12 18 R 11 19 R 12 19 R 12 18 R 11 19 R 12 19 R 12 18 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 19 R 12 19 R 11 19 R 12 20 R 12 19 R 11 19 R 12 19 R 12 19 R 11 20 R 12 19 R 12 19 R 11 20 R 12 19 R 12 19 R 11 20 R 12 19 R 12 19 R 11 20 R 12 19 R 12 20 R 11 19 R 12 20 R 12 19 R 11 19 R 12 20 R 12 19 R D 8104 11092 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 15 2 R 13 5 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 8832 8550 M -1 15 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R 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-6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 13 R 3 15 R 1 14 R D 11018 3402 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R D 11747 2425 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -5 -13 R -2 -15 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 12475 1806 M -1 14 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 8 12 R 7 13 R 5 14 R 2 14 R 1 15 R D 13204 1480 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 1 -1 R D 13169 1400 M 2 1 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 13932 1415 M -1 14 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R D 13931 1400 M 1 15 R D 14661 1675 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -13 9 R -13 6 R -13 5 R -15 2 R -14 1 R -14 -1 R -15 -2 R -13 -5 R -13 -6 R -13 -9 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 13 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R D 15390 2132 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 16118 2881 M -1 14 R -3 15 R -4 13 R -7 13 R -8 13 R -9 10 R -11 10 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -12 -8 R -11 -10 R -10 -10 R -8 -13 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 13 -4 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 15 R D 16847 3793 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R D L2 7445 13299 M 2 -5 R 12 -50 R 12 -49 R 11 -50 R 12 -49 R 12 -50 R 11 -49 R 12 -49 R 12 -49 R 11 -49 R 12 -49 R 12 -48 R 11 -49 R 12 -48 R 12 -48 R 11 -49 R 12 -48 R 12 -47 R 11 -48 R 12 -48 R 12 -48 R 11 -47 R 12 -47 R 12 -48 R 11 -47 R 12 -47 R 12 -47 R 11 -46 R 12 -47 R 12 -47 R 11 -46 R 12 -46 R 12 -46 R 11 -46 R 12 -46 R 12 -46 R 11 -46 R 12 -45 R 12 -46 R 11 -45 R 12 -45 R 12 -45 R 11 -45 R 12 -45 R 12 -45 R 11 -45 R 12 -44 R 12 -44 R 11 -45 R 12 -44 R 12 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-21 R 12 -21 R 12 -21 R 11 -20 R 12 -21 R 12 -20 R 11 -20 R 12 -21 R 12 -20 R 11 -20 R 12 -20 R 12 -20 R 11 -19 R 12 -20 R 12 -20 R 11 -19 R 12 -19 R 12 -20 R 11 -19 R 12 -19 R 12 -19 R 11 -19 R 12 -19 R 12 -19 R 11 -18 R 12 -19 R 12 -18 R 11 -19 R 12 -18 R 12 -18 R 11 -19 R 12 -18 R 12 -17 R 11 -18 R 12 -18 R 12 -18 R 11 -17 R 12 -18 R 12 -17 R 11 -17 R 12 -18 R 12 -17 R 11 -17 R 12 -17 R 12 -16 R 11 -17 R 12 -17 R 12 -16 R 11 -17 R 12 -16 R 12 -16 R 11 -16 R 12 -16 R 12 -16 R 11 -16 R 12 -16 R 12 -16 R 11 -15 R 12 -16 R 12 -15 R 11 -16 R 12 -15 R 12 -15 R 11 -15 R 12 -15 R 12 -15 R 11 -14 R 12 -15 R 12 -15 R 11 -14 R 12 -14 R 12 -15 R 11 -14 R 12 -14 R 12 -14 R 11 -14 R 12 -14 R 12 -13 R 11 -14 R 12 -13 R 12 -14 R 11 -13 R 12 -13 R 12 -13 R 11 -13 R 12 -13 R 12 -13 R 11 -13 R 12 -13 R 12 -12 R 11 -13 R 12 -12 R 12 -12 R 11 -12 R 12 -12 R 12 -12 R 11 -12 R 12 -12 R 12 -12 R 11 -11 R 12 -12 R 12 -11 R 11 -12 R 12 -11 R 12 -11 R 11 -11 R 12 -11 R 12 -11 R 11 -11 R 12 -10 R 12 -11 R 11 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11 -2 R 12 -2 R 12 -1 R 11 -2 R 12 -1 R 12 -2 R 11 -1 R 12 -2 R 12 -1 R 11 -1 R 12 -1 R 12 -1 R 11 -1 R 12 -1 R 12 0 R 11 -1 R 12 -1 R 12 0 R 11 0 R 12 -1 R 12 0 R 11 0 R 12 0 R 12 0 R 11 0 R 12 0 R 12 1 R 11 0 R 12 1 R 12 0 R 11 1 R 12 1 R 12 1 R 11 1 R 12 1 R 12 1 R 12 2 R 11 1 R 12 2 R 12 1 R 11 2 R 12 2 R 12 2 R 11 2 R 12 2 R 12 2 R 11 3 R 12 2 R 12 3 R 11 2 R 12 3 R 12 3 R 11 3 R 12 3 R 12 3 R 11 3 R 12 3 R 12 4 R 11 3 R 12 4 R 12 3 R 11 4 R 12 4 R 12 4 R 11 3 R 12 4 R 12 4 R 11 5 R 12 4 R 12 4 R 11 4 R 12 5 R 12 4 R 11 5 R 12 4 R 12 5 R 11 5 R 12 4 R 12 5 R 11 5 R 12 5 R 12 5 R 11 5 R 12 5 R 12 5 R 11 5 R 12 6 R 12 5 R 11 5 R 12 5 R 12 6 R 11 5 R 12 6 R 12 5 R 11 6 R 12 5 R 12 6 R 11 6 R 12 5 R 12 6 R 11 6 R 12 5 R 12 6 R 11 6 R 12 6 R 12 6 R 11 6 R 12 6 R 12 5 R 11 6 R 12 6 R 12 6 R 11 7 R 12 6 R 12 6 R 11 6 R 12 6 R 12 7 R 11 6 R 12 6 R 12 7 R 11 6 R 12 7 R 12 6 R 11 7 R 12 6 R 12 7 R 11 7 R 12 7 R 12 6 R 11 7 R 12 7 R 12 7 R 11 8 R 12 7 R 12 7 R 11 7 R 12 7 R 12 8 R 11 7 R 12 8 R 12 8 R 11 7 R 12 8 R 12 8 R 11 8 R 12 8 R 12 8 R 11 8 R 12 8 R 12 8 R 11 9 R 12 8 R 12 9 R 11 8 R 12 9 R 12 9 R 11 9 R 12 9 R 12 9 R 11 9 R 12 9 R 12 9 R 11 10 R 12 9 R 12 10 R 11 10 R 12 10 R 12 9 R 11 10 R 12 10 R 12 11 R 11 10 R 12 10 R 12 11 R 11 10 R 12 11 R 12 11 R 11 10 R 12 11 R 12 11 R 11 11 R 12 11 R 12 12 R 11 11 R 12 11 R 12 12 R 11 11 R 12 12 R 12 12 R 12 11 R 11 12 R 12 12 R 12 12 R 11 12 R 12 12 R 12 12 R 11 12 R 12 13 R 12 12 R 11 13 R 12 12 R 12 13 R 11 12 R 12 13 R 12 13 R 11 12 R 12 13 R 12 13 R 11 13 R 12 13 R 12 13 R 11 13 R 12 14 R 12 13 R 11 13 R 12 13 R 12 14 R 11 13 R 12 14 R 12 13 R 11 14 R 12 13 R 12 14 R 11 14 R 12 13 R 12 14 R 11 14 R 12 14 R 12 14 R 11 14 R 12 14 R 12 14 R 11 14 R 12 14 R 12 14 R 11 14 R 12 14 R 12 14 R 11 15 R 12 14 R 12 14 R 11 14 R D 16187 3098 M 12 15 R 12 14 R 11 14 R 12 15 R 12 14 R 11 15 R 12 14 R 12 15 R 11 14 R 12 15 R 12 15 R 11 14 R 12 15 R 12 15 R 11 14 R 12 15 R 12 15 R 11 14 R 12 15 R 12 15 R 11 15 R 12 15 R 12 14 R 11 15 R 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R 11 15 R 12 14 R 12 15 R 11 15 R 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R 11 15 R 12 15 R 12 15 R D L0 6647 11389 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -5 -13 R -2 -15 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R D 7375 8750 M -1 14 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -5 R 14 -2 R 14 -1 R 15 1 R 14 2 R 14 5 R 13 7 R 12 8 R 11 9 R 9 11 R 8 12 R 7 13 R 5 14 R 2 14 R 1 15 R D 8104 6534 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -13 4 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 4 -13 R 7 -13 R 8 -13 R 9 -10 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 10 R 8 13 R 6 13 R 5 13 R 3 15 R 1 14 R D 8832 4775 M -1 14 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -9 R 13 -6 R 14 -5 R 14 -2 R 14 -1 R 15 1 R 14 2 R 14 5 R 13 6 R 12 9 R 11 9 R 9 11 R 9 12 R 6 13 R 5 14 R 2 14 R 1 15 R D 9561 3406 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -12 8 R -14 7 R -13 4 R -15 3 R -14 1 R -14 -1 R -15 -3 R -13 -4 R -14 -7 R -12 -8 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R 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R 1 14 R D 11747 1451 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -14 R 5 -14 R 4 -9 R D 11733 1400 M 5 9 R 5 14 R 3 14 R 1 14 R D 12475 1419 M -1 14 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -14 R 1 -15 R 0 -4 R D 12473 1400 M 1 4 R 1 15 R D 13204 1679 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -13 5 R -15 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R D 13932 2233 M -1 15 R -2 14 R -5 14 R -6 13 R -9 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 9 12 R 6 13 R 5 13 R 2 15 R 1 14 R D 14661 2983 M -1 14 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 10 R -13 8 R -13 6 R -13 5 R -15 3 R -14 1 R -14 -1 R -15 -3 R -13 -5 R -13 -6 R -13 -8 R -10 -10 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 10 -11 R 10 -9 R 13 -9 R 13 -6 R 13 -5 R 15 -2 R 14 -1 R 14 1 R 15 2 R 13 5 R 13 6 R 13 9 R 10 9 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 15 R D 15390 3993 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -14 R 1 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R 0 -61 R 16 30 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f13a.eps0100644000000000000000000006227610376206774011051 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 14:58:52 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 4667 1830 M 0 186 R D 4120 1463 M -30 -152 R 30 31 R 46 15 R 45 0 R 46 -15 R 30 -31 R 16 -45 R 0 -31 R -16 -45 R -30 -31 R -46 -15 R -45 0 R -46 15 R -15 15 R -15 31 R 0 15 R 15 15 R 15 -15 R -15 -15 R D 4211 1357 M 31 -15 R 30 -31 R 15 -45 R 0 -31 R -15 -45 R -30 -31 R -31 -15 R D 4120 1463 M 152 0 R D 4120 1448 M 76 0 R 76 15 R D 4470 1463 M -46 -15 R -15 -31 R 0 -45 R 15 -30 R 46 -16 R 60 0 R 46 16 R 15 30 R 0 45 R -15 31 R -46 15 R -60 0 R -31 -15 R -15 -31 R 0 -45 R 15 -30 R 31 -16 R D 4530 1326 M 31 16 R 15 30 R 0 45 R -15 31 R -31 15 R D 4470 1326 M -46 -15 R -15 -15 R -15 -30 R 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D 11293 6560 M 1781 0 R D 6395 5429 M 0 1029 R D 5504 5944 M 1781 0 R D 9333 6663 M 0 1337 R D 8443 7332 M 1781 0 R D L1 2886 4915 M 14248 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f13b.eps0100644000000000000000000005655610376206774011056 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 14:58:52 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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8514 M 647 0 R D 10658 6406 M 0 1337 R D 10334 7075 M 648 0 R D 5218 6149 M 0 2262 R D 4894 7280 M 647 0 R D 10464 5841 M 0 1439 R D 10140 6560 M 647 0 R D 14479 5429 M 0 1029 R D 14155 5944 M 648 0 R D 14868 6663 M 0 1337 R D 14544 7332 M 647 0 R D L1 2886 4915 M 14248 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f13c.eps0100644000000000000000000003205510376206774011043 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.local, %% /Users/martin/conv/output/50x50x82/LP815-43/figures %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Fri Oct 21 22:34:23 2005 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 1200 M 15300 0 R D 1800 1200 M 0 204 R D 1116 650 M 274 0 R D 1587 833 M -45 -16 R -31 -45 R -15 -76 R 0 -46 R 15 -76 R 31 -45 R 45 -15 R 31 0 R 45 15 R 31 45 R 15 76 R 0 46 R -15 76 R -31 45 R -45 16 R -31 0 R -30 -16 R -15 -15 R -15 -30 R -16 -76 R 0 -46 R 16 -76 R 15 -30 R 15 -15 R 30 -15 R D 1618 514 M 30 15 R 15 15 R 15 30 R 16 76 R 0 46 R -16 76 R -15 30 R -15 15 R -30 16 R D 1830 544 M -15 -15 R 15 -15 R 16 15 R -16 15 R D 2043 833 M -46 -16 R -30 -45 R -15 -76 R 0 -46 R 15 -76 R 30 -45 R 46 -15 R 30 0 R 46 15 R 30 45 R 16 76 R 0 46 R -16 76 R -30 45 R -46 16 R -30 0 R -30 -16 R -16 -15 R -15 -30 R 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4175 M -153 0 R D 17100 5025 M -153 0 R D 17100 5450 M -153 0 R D 17100 5875 M -153 0 R D 17100 6725 M -153 0 R D 17100 7150 M -153 0 R D 17100 7575 M -153 0 R D 17100 8425 M -153 0 R D 17100 8850 M -153 0 R D 17100 9275 M -153 0 R D 17100 10125 M -153 0 R D 17100 10550 M -153 0 R D 17100 10975 M -153 0 R D 1800 1200 M 510 0 R 510 0 R 0 850 R 510 0 R 510 0 R 0 -850 R 510 0 R 510 0 R 510 0 R 510 0 R 510 0 R 510 0 R 0 3400 R 510 0 R 510 0 R 0 3400 R 510 0 R 510 0 R 0 -4250 R 510 0 R 510 0 R 510 0 R 510 0 R 0 850 R 510 0 R 510 0 R 0 -3400 R 510 0 R 510 0 R 510 0 R 510 0 R 0 850 R 510 0 R 510 0 R 0 -850 R 510 0 R 510 0 R 510 0 R 509 0 R D L1 1800 1200 M 15299 0 R D 6900 1200 M 0 10199 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f14a.eps0100644000000000000000000006206010376206774011041 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.local, %% /Users/martin/conv/output/1D/LP815-43/figures %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Thu Oct 20 16:20:36 2005 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 2887 1830 M 0 186 R D 2416 1417 M -16 -15 R 16 -15 R 15 15 R 0 15 R -15 31 R -31 15 R -45 0 R -46 -15 R -30 -31 R -15 -30 R -16 -61 R 0 -91 R 16 -45 R 30 -31 R 46 -15 R 30 0 R 45 15 R 31 31 R 15 45 R 0 15 R -15 46 R -31 30 R -45 16 R -15 0 R -46 -16 R -30 -30 R -15 -46 R D 2340 1463 M -31 -15 R -30 -31 R -15 -30 R -15 -61 R 0 -91 R 15 -45 R 30 -31 R 31 -15 R D 2355 1144 M 30 15 R 31 31 R 15 45 R 0 15 R -15 46 R -31 30 R -30 16 R D 2719 1417 M -15 -15 R 15 -15 R 16 15 R 0 15 R -16 31 R -30 15 R -46 0 R -45 -15 R -30 -31 R -16 -30 R -15 -61 R 0 -91 R 15 -45 R 31 -31 R 45 -15 R 31 0 R 45 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end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f14b.eps0100644000000000000000000006422310376206774011045 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 14:51:50 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 2887 1830 M 0 186 R D 2416 1417 M -15 -15 R 15 -15 R 15 15 R 0 15 R -15 31 R -30 15 R -46 0 R -45 -15 R -31 -31 R -15 -30 R -15 -61 R 0 -91 R 15 -45 R 30 -31 R 46 -15 R 30 0 R 46 15 R 30 31 R 15 45 R 0 15 R -15 46 R -30 30 R -46 16 R -15 0 R -45 -16 R -31 -30 R -15 -46 R D 2340 1463 M -30 -15 R -31 -31 R -15 -30 R -15 -61 R 0 -91 R 15 -45 R 31 -31 R 30 -15 R D 2355 1144 M 31 15 R 30 31 R 15 45 R 0 15 R -15 46 R -30 30 R -31 16 R D 2538 1463 M 0 -91 R D 2538 1402 M 15 31 R 30 30 R 31 0 R 75 -46 R 31 0 R 15 16 R 15 30 R D 2553 1433 M 30 15 R 31 0 R 75 -31 R D 2750 1463 M 0 -46 R -15 -45 R 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5851 10326 M 30 -15 R 15 -15 R 46 -106 R 15 -15 R 15 0 R 15 15 R D 5881 10311 M 15 -30 R 30 -106 R 16 -16 R 30 0 R 15 31 R 0 15 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f14c.eps0100644000000000000000000005574610376206774011060 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.local, %% /Users/martin/conv/output/1D/LP815-43/figures %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Thu Oct 20 16:20:36 2005 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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f15.eps0100644000000000000000000005135110376206774010702 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 14:52:02 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 2886 1830 M 0 226 R D 2203 1281 M 273 0 R D 2673 1463 M -45 -15 R -31 -46 R -15 -76 R 0 -45 R 15 -76 R 31 -46 R 45 -15 R 31 0 R 45 15 R 31 46 R 15 76 R 0 45 R -15 76 R -31 46 R -45 15 R -31 0 R -30 -15 R -15 -15 R -15 -31 R -16 -76 R 0 -45 R 16 -76 R 15 -31 R 15 -15 R 30 -15 R D 2704 1144 M 30 15 R 15 15 R 16 31 R 15 76 R 0 45 R -15 76 R -16 31 R -15 15 R -30 15 R D 2916 1174 M -15 -15 R 15 -15 R 16 15 R -16 15 R D 3084 1402 M 30 15 R 46 46 R 0 -319 R D 3144 1448 M 0 -304 R D 3084 1144 M 136 0 R D 3433 1463 M -46 -15 R -30 -46 R -15 -76 R 0 -45 R 15 -76 R 30 -46 R 46 -15 R 30 0 R 46 15 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%%CreationDate: Wed Feb 15 15:00:29 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 2864 4200 M 0 182 R D 6407 4200 M 0 182 R D 9951 4200 M 0 182 R D 13495 4200 M 0 182 R D 17039 4200 M 0 182 R D 1978 4200 M 0 91 R D 3750 4200 M 0 91 R D 4636 4200 M 0 91 R D 5522 4200 M 0 91 R D 7293 4200 M 0 91 R D 8179 4200 M 0 91 R D 9065 4200 M 0 91 R D 10837 4200 M 0 91 R D 11723 4200 M 0 91 R D 12609 4200 M 0 91 R D 14381 4200 M 0 91 R D 15267 4200 M 0 91 R D 16153 4200 M 0 91 R D 1800 13300 M 15300 0 R D 2864 13300 M 0 -182 R D 6407 13300 M 0 -182 R D 9951 13300 M 0 -182 R D 13495 13300 M 0 -182 R D 17039 13300 M 0 -182 R D 1978 13300 M 0 -91 R D 3750 13300 M 0 -91 R D 4636 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%%DocumentNeededResources: font Times-Roman %%EOF f16b.eps0100644000000000000000000010550110376206774011042 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/HD160617 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:00:30 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 2838 4200 M 0 182 R D 6381 4200 M 0 182 R D 9925 4200 M 0 182 R D 13469 4200 M 0 182 R D 17013 4200 M 0 182 R D 1952 4200 M 0 91 R D 3724 4200 M 0 91 R D 4610 4200 M 0 91 R D 5496 4200 M 0 91 R D 7267 4200 M 0 91 R D 8153 4200 M 0 91 R D 9039 4200 M 0 91 R D 10811 4200 M 0 91 R D 11697 4200 M 0 91 R D 12583 4200 M 0 91 R D 14355 4200 M 0 91 R D 15241 4200 M 0 91 R D 16127 4200 M 0 91 R D 1800 13300 M 15300 0 R D 2838 13300 M 0 -182 R D 6381 13300 M 0 -182 R D 9925 13300 M 0 -182 R D 13469 13300 M 0 -182 R D 17013 13300 M 0 -182 R D 1952 13300 M 0 -91 R D 3724 13300 M 0 -91 R D 4610 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2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f17a.eps0100644000000000000000000010520710376206774011045 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/G020-024 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:00:32 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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M -153 0 R D 40 setlinewidth 1800 2721 M 248 -6 R 437 20 R 438 147 R 436 217 R 437 -35 R 436 -187 R 438 -212 R 438 114 R 435 153 R 438 -54 R 436 -199 R 438 -11 R 437 90 R 436 86 R 438 -111 R 437 235 R 436 -61 R 438 -178 R 436 -48 R 437 -63 R 438 302 R 436 94 R 438 -68 R 435 -212 R 438 -285 R 438 123 R 436 284 R 437 0 R 436 -125 R 438 9 R 437 140 R 436 112 R 438 -191 R 436 -234 R 437 66 R 195 34 R D L2 1800 2735 M 248 -6 R 437 22 R 438 148 R 436 219 R 437 -31 R 436 -185 R 438 -211 R 438 107 R 435 124 R 438 -107 R 436 -256 R 438 6 R 437 266 R 436 285 R 438 -189 R 437 -79 R 436 -427 R 438 -130 R 436 489 R 437 391 R 438 112 R 436 -571 R 438 -443 R 435 -372 R 438 -61 R 438 376 R 436 485 R 437 108 R 436 -77 R 438 27 R 437 143 R 436 112 R 438 -193 R 436 -236 R 437 64 R 195 33 R D 10 setlinewidth L1 1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f17b.eps0100644000000000000000000007737410376206774011063 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/G075-031 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:00:32 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 2844 4200 M 0 182 R D 6388 4200 M 0 182 R D 9932 4200 M 0 182 R D 13475 4200 M 0 182 R D 17019 4200 M 0 182 R D 1958 4200 M 0 91 R D 3730 4200 M 0 91 R D 4616 4200 M 0 91 R D 5502 4200 M 0 91 R D 7274 4200 M 0 91 R D 8160 4200 M 0 91 R D 9046 4200 M 0 91 R D 10818 4200 M 0 91 R D 11703 4200 M 0 91 R D 12589 4200 M 0 91 R D 14361 4200 M 0 91 R D 15247 4200 M 0 91 R D 16133 4200 M 0 91 R D 1800 13300 M 15300 0 R D 2844 13300 M 0 -182 R D 6388 13300 M 0 -182 R D 9932 13300 M 0 -182 R D 13475 13300 M 0 -182 R D 17019 13300 M 0 -182 R D 1958 13300 M 0 -91 R D 3730 13300 M 0 -91 R D 4616 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f18a.eps0100644000000000000000000013121410376206774011043 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, %% /Users/martin/conv/output/50x50x82/G020-024 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 14:40:43 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 4224 4200 M 0 182 R D 7479 4200 M 0 182 R D 10734 4200 M 0 182 R D 13990 4200 M 0 182 R D 2596 4200 M 0 91 R D 3410 4200 M 0 91 R D 5037 4200 M 0 91 R D 5851 4200 M 0 91 R D 6665 4200 M 0 91 R D 8293 4200 M 0 91 R D 9107 4200 M 0 91 R D 9921 4200 M 0 91 R D 11548 4200 M 0 91 R D 12362 4200 M 0 91 R D 13176 4200 M 0 91 R D 14804 4200 M 0 91 R D 15617 4200 M 0 91 R D 16431 4200 M 0 91 R D 1800 13300 M 15300 0 R D 4224 13300 M 0 -182 R D 7479 13300 M 0 -182 R D 10734 13300 M 0 -182 R D 13990 13300 M 0 -182 R D 2596 13300 M 0 -91 R D 3410 13300 M 0 -91 R D 5037 13300 M 0 -91 R D 5851 13300 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437 -303 R 315 11 R D 10 setlinewidth L1 1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f18b.eps0100644000000000000000000012523110376206774011046 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, %% /Users/martin/conv/output/50x50x82/LP815-43 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 14:40:46 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f19a.eps0100644000000000000000000025061410376206774011052 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 13:08:00 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. 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18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 -19 R 10 0 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 -18 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 0 R 9 -19 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -18 R 9 -19 R 5 0 R 9 -18 R 5 -18 R 9 -18 R 10 0 R 4 -18 R 10 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 14 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 -18 R 10 0 R 4 -19 R 10 0 R 4 -18 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 9 0 R 10 -19 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -18 R 14 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 14 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 19 R 5 0 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 19 R 10 0 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 19 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 19 R 5 0 R 9 18 R 5 0 R 14 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 19 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 19 R 9 0 R 5 18 R 14 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 19 R 5 0 R 9 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 18 R 10 0 R 5 0 R 9 19 R 9 0 R 10 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 19 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R D 9887 11462 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R D 15625 11480 M 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11316 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 14 -18 R 5 0 R 9 -18 R 5 -18 R 9 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 9 -18 R 10 -19 R 4 -18 R 10 -18 R 4 -18 R 10 -18 R 9 -19 R 5 -18 R 9 -36 R 5 -18 R 9 -37 R 9 -18 R 10 -36 R 9 -19 R 5 -36 R 9 -36 R 5 -37 R 9 -36 R 9 -37 R 5 -36 R 9 -36 R 5 -55 R 9 -36 R 10 -55 R 4 -36 R 10 -55 R 4 -55 R 10 -54 R 9 -55 R 5 -54 R 9 -73 R 5 -55 R 14 -73 R 4 -72 R 10 -73 R 9 -73 R 5 -73 R 9 -73 R 5 -91 R 9 -91 R 9 -91 R 5 -91 R 9 -91 R 5 -109 R 9 -91 R 10 -109 R 4 -109 R 10 -109 R 4 -128 R 10 -109 R 9 -127 R 5 -128 R 9 -145 R 9 -128 R 10 -145 R 4 -146 R 10 -146 R 9 -163 R 5 -146 R 9 -164 R 5 -164 R 9 -182 R 9 -163 R 5 -182 R 9 -182 R 5 -201 R 9 -182 R 10 -200 R 4 -200 R 10 -218 R 4 -201 R 10 -218 R 9 -218 R 1 -55 R D 4156 4200 M 2 36 R 4 237 R 10 218 R 9 201 R 5 218 R 9 200 R 5 200 R 9 182 R 9 201 R 5 182 R 9 182 R 5 163 R 10 182 R 9 164 R 5 164 R 9 146 R 5 163 R 9 146 R 9 146 R 5 145 R 14 128 R 5 145 R 9 128 R 5 127 R 9 109 R 9 128 R 5 109 R 9 109 R 5 109 R 9 91 R 10 109 R 4 91 R 10 91 R 4 91 R 10 91 R 9 91 R 5 73 R 9 73 R 5 73 R 9 73 R 9 72 R 10 73 R 9 55 R 5 73 R 9 54 R 5 55 R 9 54 R 9 55 R 5 55 R 9 54 R 5 37 R 9 54 R 10 37 R 4 36 R 10 36 R 4 37 R 10 36 R 9 37 R 5 36 R 9 36 R 5 37 R 14 18 R 4 36 R 10 19 R 9 36 R 5 18 R 9 18 R 5 19 R 9 36 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 10 0 R 4 18 R 10 18 R 4 19 R 10 18 R 9 0 R 5 18 R 9 18 R 9 0 R 10 18 R 4 0 R 10 19 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 -19 R 10 0 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 -18 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 0 R 9 -19 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -18 R 9 -19 R 5 0 R 9 -18 R 5 -18 R 9 -18 R 10 0 R 4 -18 R 10 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 14 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 -18 R 10 0 R 4 -19 R 10 0 R 4 -18 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 9 0 R 10 -19 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -18 R 14 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 14 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 19 R 5 0 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 19 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 9 0 R 10 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 19 R 9 0 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 19 R 9 0 R 5 18 R 14 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 19 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 19 R 5 0 R 14 18 R 4 0 R 10 18 R 4 0 R 10 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 19 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 18 R 10 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 19 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 -19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 14 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R D 9887 10843 M 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 19 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 19 R 9 0 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 5 18 R 9 0 R 10 18 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 19 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 5 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 10 0 R 4 0 R 10 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R D 15625 11480 M 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11316 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 14 -18 R 5 0 R 9 -18 R 5 -18 R 9 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 9 -18 R 10 -19 R 4 -18 R 10 -18 R 4 -18 R 10 -18 R 9 -19 R 5 -18 R 9 -36 R 5 -18 R 9 -37 R 9 -18 R 10 -36 R 9 -19 R 5 -36 R 9 -36 R 5 -37 R 9 -36 R 9 -37 R 5 -36 R 9 -36 R 5 -55 R 9 -36 R 10 -55 R 4 -36 R 10 -55 R 4 -55 R 10 -54 R 9 -55 R 5 -54 R 9 -73 R 5 -55 R 14 -73 R 4 -72 R 10 -73 R 9 -73 R 5 -73 R 9 -73 R 5 -91 R 9 -91 R 9 -91 R 5 -91 R 9 -91 R 5 -109 R 9 -91 R 10 -109 R 4 -109 R 10 -109 R 4 -128 R 10 -109 R 9 -127 R 5 -128 R 9 -145 R 9 -128 R 10 -145 R 4 -146 R 10 -146 R 9 -163 R 5 -146 R 9 -164 R 5 -164 R 9 -182 R 9 -163 R 5 -182 R 9 -182 R 5 -201 R 9 -182 R 10 -200 R 4 -200 R 10 -218 R 4 -201 R 10 -218 R 9 -218 R 1 -55 R D 4156 4200 M 2 36 R 4 237 R 10 218 R 9 201 R 5 218 R 9 200 R 5 200 R 9 182 R 9 201 R 5 182 R 9 182 R 5 163 R 10 182 R 9 164 R 5 164 R 9 146 R 5 163 R 9 146 R 9 146 R 5 145 R 14 128 R 5 145 R 9 128 R 5 127 R 9 109 R 9 128 R 5 109 R 9 109 R 5 109 R 9 91 R 10 109 R 4 91 R 10 91 R 4 91 R 10 91 R 9 91 R 5 73 R 9 73 R 5 73 R 9 73 R 9 72 R 10 73 R 9 55 R 5 73 R 9 54 R 5 55 R 9 54 R 9 55 R 5 55 R 9 54 R 5 37 R 9 54 R 10 37 R 4 36 R 10 36 R 4 37 R 10 36 R 9 37 R 5 36 R 9 36 R 5 37 R 14 18 R 4 36 R 10 19 R 9 36 R 5 18 R 9 18 R 5 19 R 9 36 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 10 0 R 4 18 R 10 18 R 4 19 R 10 18 R 9 0 R 5 18 R 9 18 R 9 0 R 10 18 R 4 0 R 10 19 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 -19 R 10 0 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 -18 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 0 R 9 -19 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -18 R 9 -19 R 5 0 R 9 -18 R 5 -18 R 9 -18 R 10 0 R 4 -18 R 10 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 14 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 -18 R 10 0 R 4 -19 R 10 0 R 4 -18 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 9 0 R 10 -19 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -18 R 14 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 14 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 19 R 5 0 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 19 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 9 0 R 10 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 19 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 0 R 10 18 R 4 0 R 10 18 R 9 0 R 5 19 R 9 0 R 5 18 R 14 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 9 19 R 5 0 R 9 18 R 5 0 R 9 18 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-18 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 -19 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 14 0 R 4 -19 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 -18 R D 9887 10479 M 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 9 0 R 5 19 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 18 R 4 0 R 10 0 R 4 18 R 10 0 R 9 19 R 5 0 R 9 0 R 5 18 R 14 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 19 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 19 R 9 0 R 5 18 R 9 0 R 9 18 R 10 18 R 4 0 R 10 18 R 9 0 R 5 19 R 9 0 R 5 18 R 9 18 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 19 R 4 18 R 10 0 R 4 18 R 10 0 R 9 18 R 9 0 R 10 18 R 4 19 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 18 R 5 18 R 9 0 R 10 19 R 4 0 R 10 18 R 4 0 R 10 18 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 19 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 18 R 9 0 R 5 18 R 9 0 R 5 19 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 14 0 R 4 19 R 10 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 18 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0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R D 15625 11480 M 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11316 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 14 -18 R 5 0 R 9 -18 R 5 -18 R 9 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 9 -18 R 10 -19 R 4 -18 R 10 -18 R 4 -18 R 10 -18 R 9 -19 R 5 -18 R 9 -36 R 5 -18 R 9 -37 R 9 -18 R 10 -36 R 9 -19 R 5 -36 R 9 -36 R 5 -37 R 9 -36 R 9 -37 R 5 -36 R 9 -36 R 5 -55 R 9 -36 R 10 -55 R 4 -36 R 10 -55 R 4 -55 R 10 -54 R 9 -55 R 5 -54 R 9 -73 R 5 -55 R 14 -73 R 4 -72 R 10 -73 R 9 -73 R 5 -73 R 9 -73 R 5 -91 R 9 -91 R 9 -91 R 5 -91 R 9 -91 R 5 -109 R 9 -91 R 10 -109 R 4 -109 R 10 -109 R 4 -128 R 10 -109 R 9 -127 R 5 -128 R 9 -145 R 9 -128 R 10 -145 R 4 -146 R 10 -146 R 9 -163 R 5 -146 R 9 -164 R 5 -164 R 9 -182 R 9 -163 R 5 -182 R 9 -182 R 5 -201 R 9 -182 R 10 -200 R 4 -200 R 10 -218 R 4 -201 R 10 -218 R 9 -218 R 1 -55 R D 4156 4200 M 2 36 R 4 237 R 10 218 R 9 201 R 5 218 R 9 200 R 5 200 R 9 182 R 9 201 R 5 182 R 9 182 R 5 163 R 10 182 R 9 164 R 5 164 R 9 146 R 5 163 R 9 146 R 9 146 R 5 145 R 14 128 R 5 145 R 9 128 R 5 127 R 9 109 R 9 128 R 5 109 R 9 109 R 5 109 R 9 91 R 10 109 R 4 91 R 10 91 R 4 91 R 10 91 R 9 91 R 5 73 R 9 73 R 5 73 R 9 73 R 9 72 R 10 73 R 9 55 R 5 73 R 9 54 R 5 55 R 9 54 R 9 55 R 5 55 R 9 54 R 5 37 R 9 54 R 10 37 R 4 36 R 10 36 R 4 37 R 10 36 R 9 37 R 5 36 R 9 36 R 5 37 R 14 18 R 4 36 R 10 19 R 9 36 R 5 18 R 9 18 R 5 19 R 9 36 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 10 0 R 4 18 R 10 18 R 4 19 R 10 18 R 9 0 R 5 18 R 9 18 R 9 0 R 10 18 R 4 0 R 10 19 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 -19 R 10 0 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 -18 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 0 R 9 -19 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -18 R 9 -19 R 5 0 R 9 -18 R 5 -18 R 9 -18 R 10 0 R 4 -18 R 10 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 14 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 -18 R 10 0 R 4 -19 R 10 0 R 4 -18 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 9 0 R 10 -19 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -18 R 14 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 14 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 9 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 5 0 R 9 18 R 5 0 R 9 18 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 9 19 R 5 0 R 9 0 R 5 18 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 19 R 5 0 R 14 18 R 4 0 R 10 18 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 9 0 R 5 19 R 9 0 R 5 18 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 14 19 R 4 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 19 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 5 18 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 19 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -19 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 14 0 R 4 -19 R 10 0 R 5 0 R 9 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 10 0 R 9 -19 R 5 0 R 9 -18 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -19 R 10 0 R 4 -18 R 10 -18 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 14 -18 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -18 R 10 0 R 4 -18 R 10 -19 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 9 0 R 10 -18 R 4 -19 R 10 0 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -19 R 5 -18 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 -18 R 10 0 R 9 -19 R 5 0 R 14 -18 R 4 0 R 10 -18 R 4 -18 R 10 0 R 9 -18 R 5 0 R 9 -19 R 5 -18 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 0 R 10 -18 R 9 -19 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 -18 R D 9887 9915 M 9 -18 R 5 0 R 9 -19 R 5 0 R 9 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 -18 R 4 0 R 10 -19 R 4 -18 R 10 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 -19 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 -19 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 14 0 R 4 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 0 R 10 19 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 19 R 10 0 R 4 18 R 10 18 R 4 0 R 10 18 R 9 18 R 5 0 R 9 19 R 5 18 R 14 0 R 4 18 R 10 18 R 9 0 R 5 18 R 9 19 R 5 18 R 9 18 R 9 0 R 5 18 R 9 18 R 5 19 R 9 18 R 10 0 R 4 18 R 10 18 R 4 18 R 10 19 R 9 18 R 5 0 R 9 18 R 9 18 R 10 18 R 4 19 R 10 18 R 9 18 R 5 18 R 9 0 R 5 18 R 9 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 10 18 R 4 18 R 10 0 R 4 18 R 10 18 R 9 19 R 9 18 R 10 18 R 4 18 R 10 18 R 4 19 R 10 18 R 9 0 R 5 18 R 9 18 R 5 18 R 9 19 R 10 18 R 4 18 R 10 0 R 4 18 R 10 18 R 9 19 R 5 18 R 9 18 R 5 0 R 9 18 R 9 18 R 10 19 R 9 18 R 5 0 R 9 18 R 5 18 R 9 18 R 9 0 R 5 19 R 9 18 R 5 18 R 9 0 R 10 18 R 4 18 R 10 19 R 4 0 R 10 18 R 9 18 R 5 0 R 9 18 R 5 0 R 14 18 R 4 19 R 10 0 R 9 18 R 5 18 R 9 0 R 5 18 R 9 0 R 9 18 R 5 0 R 9 19 R 5 0 R 9 18 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 19 R 9 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 19 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 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Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 13:08:04 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R D 9662 11480 M 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 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10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R D 15401 11480 M 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11425 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 14 -18 R 5 -18 R 9 0 R 5 -18 R 9 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 9 0 R 10 -18 R 4 -19 R 10 -18 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -36 R 9 -19 R 10 -18 R 9 -18 R 5 -36 R 9 -19 R 5 -36 R 9 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -36 R 10 -18 R 4 -37 R 10 -36 R 4 -36 R 10 -37 R 9 -36 R 5 -55 R 9 -36 R 5 -37 R 14 -54 R 4 -37 R 10 -36 R 9 -55 R 5 -54 R 9 -37 R 5 -54 R 9 -55 R 9 -54 R 5 -55 R 9 -55 R 5 -54 R 9 -55 R 10 -73 R 4 -54 R 10 -55 R 4 -73 R 10 -54 R 9 -73 R 5 -73 R 9 -73 R 9 -72 R 10 -73 R 4 -73 R 10 -73 R 9 -73 R 5 -72 R 9 -91 R 5 -73 R 9 -91 R 9 -73 R 5 -91 R 9 -91 R 5 -73 R 9 -91 R 10 -91 R 4 -91 R 10 -91 R 4 -109 R 10 -91 R 9 -91 R 5 -91 R 14 -109 R 5 -91 R 9 -109 R 5 -110 R 9 -91 R 9 -109 R 5 -109 R 9 -109 R 5 -91 R 9 -109 R 10 -110 R 4 -109 R 10 -109 R 4 -127 R 10 -110 R 9 -109 R 5 -109 R 9 -109 R 5 -109 R 9 -128 R 9 -109 R 10 -109 R 9 -128 R 5 -109 R 9 -109 R 5 -109 R 9 -128 R 9 -109 R 0 -18 R D 3932 4200 M 2 18 R 4 109 R 10 128 R 9 109 R 5 109 R 9 109 R 5 128 R 14 109 R 4 109 R 10 109 R 9 128 R 5 109 R 9 109 R 5 109 R 9 110 R 9 109 R 5 127 R 9 109 R 5 110 R 9 91 R 10 109 R 4 109 R 10 109 R 4 109 R 10 91 R 9 110 R 5 109 R 9 91 R 9 91 R 10 109 R 4 91 R 10 91 R 9 109 R 5 91 R 9 91 R 5 91 R 9 91 R 9 73 R 5 91 R 9 91 R 5 73 R 10 91 R 9 73 R 5 91 R 9 72 R 5 73 R 9 73 R 9 73 R 5 73 R 14 72 R 5 73 R 9 73 R 5 73 R 9 54 R 9 73 R 5 55 R 9 54 R 5 73 R 9 55 R 10 54 R 4 55 R 10 55 R 4 54 R 10 55 R 9 54 R 5 37 R 9 54 R 5 55 R 9 36 R 9 37 R 10 54 R 9 37 R 5 36 R 9 55 R 5 36 R 9 37 R 9 36 R 5 36 R 9 37 R 5 18 R 9 36 R 10 37 R 4 36 R 10 18 R 4 37 R 10 18 R 9 36 R 5 19 R 9 36 R 5 18 R 14 18 R 4 19 R 10 36 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 10 0 R 4 18 R 10 18 R 4 19 R 10 0 R 9 18 R 5 18 R 9 0 R 9 18 R 10 0 R 4 18 R 10 19 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 18 R 5 0 R 14 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -19 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 14 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -19 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R D 9662 10825 M 10 -18 R 4 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 -19 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 19 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 19 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 0 R 5 19 R 9 0 R 9 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 9 0 R 5 19 R 9 0 R 5 18 R 9 0 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 18 R 9 0 R 10 0 R 4 19 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 18 R 4 0 R 10 19 R 4 0 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 10 0 R 9 18 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 19 R 5 0 R 14 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 19 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 19 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R D 15401 11480 M 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11425 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 14 -18 R 5 -18 R 9 0 R 5 -18 R 9 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 9 0 R 10 -18 R 4 -19 R 10 -18 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -36 R 9 -19 R 10 -18 R 9 -18 R 5 -36 R 9 -19 R 5 -36 R 9 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -36 R 10 -18 R 4 -37 R 10 -36 R 4 -36 R 10 -37 R 9 -36 R 5 -55 R 9 -36 R 5 -37 R 14 -54 R 4 -37 R 10 -36 R 9 -55 R 5 -54 R 9 -37 R 5 -54 R 9 -55 R 9 -54 R 5 -55 R 9 -55 R 5 -54 R 9 -55 R 10 -73 R 4 -54 R 10 -55 R 4 -73 R 10 -54 R 9 -73 R 5 -73 R 9 -73 R 9 -72 R 10 -73 R 4 -73 R 10 -73 R 9 -73 R 5 -72 R 9 -91 R 5 -73 R 9 -91 R 9 -73 R 5 -91 R 9 -91 R 5 -73 R 9 -91 R 10 -91 R 4 -91 R 10 -91 R 4 -109 R 10 -91 R 9 -91 R 5 -91 R 14 -109 R 5 -91 R 9 -109 R 5 -110 R 9 -91 R 9 -109 R 5 -109 R 9 -109 R 5 -91 R 9 -109 R 10 -110 R 4 -109 R 10 -109 R 4 -127 R 10 -110 R 9 -109 R 5 -109 R 9 -109 R 5 -109 R 9 -128 R 9 -109 R 10 -109 R 9 -128 R 5 -109 R 9 -109 R 5 -109 R 9 -128 R 9 -109 R 0 -18 R D 3932 4200 M 2 18 R 4 109 R 10 128 R 9 109 R 5 109 R 9 109 R 5 128 R 14 109 R 4 109 R 10 109 R 9 128 R 5 109 R 9 109 R 5 109 R 9 110 R 9 109 R 5 127 R 9 109 R 5 110 R 9 91 R 10 109 R 4 109 R 10 109 R 4 109 R 10 91 R 9 110 R 5 109 R 9 91 R 9 91 R 10 109 R 4 91 R 10 91 R 9 109 R 5 91 R 9 91 R 5 91 R 9 91 R 9 73 R 5 91 R 9 91 R 5 73 R 10 91 R 9 73 R 5 91 R 9 72 R 5 73 R 9 73 R 9 73 R 5 73 R 14 72 R 5 73 R 9 73 R 5 73 R 9 54 R 9 73 R 5 55 R 9 54 R 5 73 R 9 55 R 10 54 R 4 55 R 10 55 R 4 54 R 10 55 R 9 54 R 5 37 R 9 54 R 5 55 R 9 36 R 9 37 R 10 54 R 9 37 R 5 36 R 9 55 R 5 36 R 9 37 R 9 36 R 5 36 R 9 37 R 5 18 R 9 36 R 10 37 R 4 36 R 10 18 R 4 37 R 10 18 R 9 36 R 5 19 R 9 36 R 5 18 R 14 18 R 4 19 R 10 36 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 10 0 R 4 18 R 10 18 R 4 19 R 10 0 R 9 18 R 5 18 R 9 0 R 9 18 R 10 0 R 4 18 R 10 19 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 18 R 5 0 R 14 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -19 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 14 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 14 -19 R 4 0 R 10 0 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -19 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 -18 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 10 0 R 4 -18 R 10 0 R 4 -19 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 -18 R 10 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 10 0 R 4 -18 R 10 0 R 9 -19 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R D 9662 10443 M 10 -19 R 4 0 R 10 -18 R 4 0 R 10 -18 R 9 0 R 5 -18 R 14 0 R 4 -18 R 10 0 R 4 -19 R 10 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 10 0 R 4 -18 R 10 0 R 4 -19 R 10 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -19 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 0 R 10 19 R 4 0 R 10 18 R 4 0 R 10 18 R 9 0 R 5 18 R 9 0 R 5 18 R 14 0 R 4 19 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 18 R 9 18 R 5 0 R 9 19 R 5 0 R 9 18 R 10 18 R 4 0 R 10 18 R 4 0 R 10 18 R 9 19 R 5 0 R 9 18 R 9 18 R 10 0 R 4 18 R 10 18 R 9 0 R 5 19 R 9 18 R 5 0 R 9 18 R 9 18 R 5 0 R 9 18 R 5 19 R 9 0 R 10 18 R 4 18 R 10 0 R 4 18 R 10 18 R 9 0 R 9 19 R 10 18 R 4 0 R 10 18 R 4 18 R 10 0 R 9 18 R 5 19 R 9 0 R 5 18 R 9 18 R 10 0 R 4 18 R 10 18 R 4 0 R 10 19 R 9 18 R 5 0 R 9 18 R 5 0 R 9 18 R 9 18 R 10 0 R 9 19 R 5 18 R 9 0 R 5 18 R 9 0 R 9 18 R 5 18 R 9 0 R 5 19 R 9 0 R 10 18 R 4 0 R 10 18 R 4 18 R 10 0 R 9 18 R 5 0 R 9 19 R 5 0 R 14 18 R 4 0 R 10 18 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 19 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 0 R 10 18 R 4 0 R 10 18 R 9 0 R 5 0 R 9 19 R 9 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 19 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 14 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R D 15401 11480 M 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11425 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 0 R 9 -18 R 5 0 R 14 -18 R 5 -18 R 9 0 R 5 -18 R 9 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 9 0 R 10 -18 R 4 -19 R 10 -18 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -36 R 9 -19 R 10 -18 R 9 -18 R 5 -36 R 9 -19 R 5 -36 R 9 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -36 R 10 -18 R 4 -37 R 10 -36 R 4 -36 R 10 -37 R 9 -36 R 5 -55 R 9 -36 R 5 -37 R 14 -54 R 4 -37 R 10 -36 R 9 -55 R 5 -54 R 9 -37 R 5 -54 R 9 -55 R 9 -54 R 5 -55 R 9 -55 R 5 -54 R 9 -55 R 10 -73 R 4 -54 R 10 -55 R 4 -73 R 10 -54 R 9 -73 R 5 -73 R 9 -73 R 9 -72 R 10 -73 R 4 -73 R 10 -73 R 9 -73 R 5 -72 R 9 -91 R 5 -73 R 9 -91 R 9 -73 R 5 -91 R 9 -91 R 5 -73 R 9 -91 R 10 -91 R 4 -91 R 10 -91 R 4 -109 R 10 -91 R 9 -91 R 5 -91 R 14 -109 R 5 -91 R 9 -109 R 5 -110 R 9 -91 R 9 -109 R 5 -109 R 9 -109 R 5 -91 R 9 -109 R 10 -110 R 4 -109 R 10 -109 R 4 -127 R 10 -110 R 9 -109 R 5 -109 R 9 -109 R 5 -109 R 9 -128 R 9 -109 R 10 -109 R 9 -128 R 5 -109 R 9 -109 R 5 -109 R 9 -128 R 9 -109 R 0 -18 R D 3932 4200 M 2 18 R 4 109 R 10 128 R 9 109 R 5 109 R 9 109 R 5 128 R 14 109 R 4 109 R 10 109 R 9 128 R 5 109 R 9 109 R 5 109 R 9 110 R 9 109 R 5 127 R 9 109 R 5 110 R 9 91 R 10 109 R 4 109 R 10 109 R 4 109 R 10 91 R 9 110 R 5 109 R 9 91 R 9 91 R 10 109 R 4 91 R 10 91 R 9 109 R 5 91 R 9 91 R 5 91 R 9 91 R 9 73 R 5 91 R 9 91 R 5 73 R 10 91 R 9 73 R 5 91 R 9 72 R 5 73 R 9 73 R 9 73 R 5 73 R 14 72 R 5 73 R 9 73 R 5 73 R 9 54 R 9 73 R 5 55 R 9 54 R 5 73 R 9 55 R 10 54 R 4 55 R 10 55 R 4 54 R 10 55 R 9 54 R 5 37 R 9 54 R 5 55 R 9 36 R 9 37 R 10 54 R 9 37 R 5 36 R 9 55 R 5 36 R 9 37 R 9 36 R 5 36 R 9 37 R 5 18 R 9 36 R 10 37 R 4 36 R 10 18 R 4 37 R 10 18 R 9 36 R 5 19 R 9 36 R 5 18 R 14 18 R 4 19 R 10 36 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 10 0 R 4 18 R 10 18 R 4 19 R 10 0 R 9 18 R 5 18 R 9 0 R 9 18 R 10 0 R 4 18 R 10 19 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 9 0 R 5 18 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 18 R 5 0 R 14 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -19 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 14 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 14 -19 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 -18 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 -18 R 9 -18 R 5 0 R 14 -18 R 4 0 R 10 -18 R 5 0 R 9 -19 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 10 -18 R 4 0 R 10 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 9 -19 R 9 0 R 10 -18 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 9 0 R 10 -18 R 4 -19 R 10 0 R 4 -18 R 10 -18 R 9 -18 R 5 0 R 9 -18 R 5 -19 R 14 -18 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 -19 R 5 0 R 9 -18 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 9 -19 R 10 -18 R 4 -18 R 10 0 R 4 -18 R 10 -18 R 9 -19 R 5 -18 R 9 0 R 9 -18 R 10 -18 R 4 -18 R 10 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 9 -18 R 9 0 R 5 -19 R 9 -18 R 5 -18 R 9 0 R D 9662 9842 M 10 -18 R 4 -18 R 10 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 14 -18 R 4 -19 R 10 0 R 4 -18 R 10 -18 R 9 -18 R 5 0 R 9 -18 R 5 -19 R 9 -18 R 10 0 R 4 -18 R 10 -18 R 4 -18 R 10 0 R 9 -19 R 5 -18 R 9 -18 R 5 0 R 9 -18 R 9 -18 R 10 -19 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -18 R 9 -18 R 5 -19 R 9 0 R 5 -18 R 9 -18 R 10 0 R 4 -18 R 10 -18 R 4 0 R 10 -19 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 -18 R 10 0 R 9 -19 R 5 0 R 9 -18 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 -19 R 10 0 R 4 -18 R 10 0 R 4 -18 R 10 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 10 -19 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 19 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 18 R 4 0 R 10 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 19 R 9 0 R 10 18 R 9 0 R 5 18 R 9 18 R 5 0 R 9 18 R 9 0 R 5 19 R 9 18 R 5 0 R 9 18 R 10 18 R 4 0 R 10 18 R 4 19 R 10 18 R 9 0 R 5 18 R 9 18 R 5 18 R 14 19 R 4 0 R 10 18 R 9 18 R 5 18 R 9 18 R 5 19 R 9 18 R 9 0 R 5 18 R 9 18 R 5 18 R 9 19 R 10 18 R 4 18 R 10 18 R 4 18 R 10 19 R 9 18 R 5 18 R 9 18 R 9 18 R 10 19 R 4 18 R 10 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 10 36 R 4 19 R 10 18 R 4 18 R 10 18 R 9 18 R 9 19 R 10 18 R 4 18 R 10 18 R 4 18 R 10 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 10 18 R 4 18 R 10 36 R 4 19 R 10 18 R 9 18 R 5 18 R 9 18 R 5 19 R 9 18 R 9 18 R 10 18 R 9 18 R 5 0 R 9 19 R 5 18 R 9 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 10 18 R 4 18 R 10 19 R 4 18 R 10 0 R 9 18 R 5 18 R 9 18 R 5 19 R 14 18 R 4 0 R 10 18 R 9 18 R 5 18 R 9 19 R 5 0 R 9 18 R 9 18 R 5 0 R 9 18 R 5 18 R 9 19 R 10 0 R 4 18 R 10 18 R 4 0 R 10 18 R 9 18 R 5 0 R 9 19 R 9 18 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 18 R 5 19 R 9 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 18 R 10 0 R 4 0 R 10 19 R 9 0 R 5 18 R 14 0 R 4 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 18 R 9 0 R 5 0 R 9 19 R 9 0 R 5 0 R 10 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 19 R 5 0 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 19 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R D 15401 11480 M 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 1400 M 15300 0 R D 1800 1400 M 0 56 R D 1177 987 M -15 -15 R 15 -15 R 15 15 R 0 15 R -15 30 R -30 16 R -46 0 R -45 -16 R -31 -30 R -15 -30 R -15 -61 R 0 -91 R 15 -46 R 31 -30 R 45 -15 R 30 0 R 46 15 R 30 30 R 16 46 R 0 15 R -16 45 R -30 31 R -46 15 R -15 0 R -45 -15 R -31 -31 R -15 -45 R D 1101 1033 M -30 -16 R -30 -30 R -16 -30 R -15 -61 R 0 -91 R 15 -46 R 31 -30 R 30 -15 R D 1116 714 M 31 15 R 30 30 R 15 46 R 0 15 R -15 45 R -30 31 R -31 15 R D 1344 972 M 31 15 R 45 46 R 0 -319 R D 1405 1017 M 0 -303 R D 1344 714 M 137 0 R D 1694 1033 M -46 -16 R -30 -45 R -15 -76 R 0 -46 R 15 -76 R 30 -45 R 46 -15 R 30 0 R 46 15 R 30 45 R 15 76 R 0 46 R -15 76 R -30 45 R -46 16 R -30 0 R -31 -16 R -15 -15 R -15 -30 R -15 -76 R 0 -46 R 15 -76 R 15 -30 R 15 -15 R 31 -15 R D 1724 714 M 30 15 R 16 15 R 15 30 R 15 76 R 0 46 R -15 76 R -15 30 R -16 15 R -30 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187 214 R 186 16 R 187 -13 R 187 -65 R 187 97 R 187 -310 R 186 -52 R 188 152 R 41 10 R D L1 1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f2.eps0100644000000000000000000010044510376206774010615 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 240 255 %%Title: Graphics produced by IDL %%For: pen@origo, /usr/users/pen/li6.paper/plot.figures %%Creator: IDL Version 6.1 (IRIX mipseb m64) %%CreationDate: Wed Aug 17 12:23:00 2005 %%DocumentData: Clean7bit %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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46 -39 R 45 -47 R 46 155 R 45 -16 R 46 -163 R 46 -239 R 45 70 R 46 56 R 46 249 R 45 32 R 46 -125 R 46 -95 R 45 -28 R 46 139 R 46 -12 R 45 -23 R 46 74 R 46 -405 R 45 69 R 46 116 R 46 32 R 45 -169 R 46 106 R 45 229 R 46 15 R 46 -88 R 45 -42 R 46 78 R 46 -134 R 44 -283 R 46 160 R 46 257 R 45 5 R 46 -42 R 46 -26 R 45 -91 R 46 167 R 46 8 R 45 9 R 46 -29 R 46 -17 R 45 69 R 46 -43 R 45 -115 R 46 44 R 46 108 R 45 55 R 46 63 R 46 -303 R 45 67 R 46 -54 R 46 1 R 45 175 R D %%PageTrailer end %%PageResources: font Helvetica %%Trailer %%Pages: 1 %%DocumentNeededResources: font Helvetica %%EOF f20a.eps0100644000000000000000000026061210376206774011041 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 13:08:23 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R D 13276 11480 M 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 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10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11444 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 14 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 -18 R 10 0 R 4 -18 R 10 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 0 R 10 -18 R 4 -19 R 10 -18 R 4 0 R 10 -18 R 9 -18 R 5 -18 R 9 -19 R 5 -18 R 14 0 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -18 R 10 -18 R 4 -19 R 10 -36 R 4 -18 R 10 -18 R 9 -19 R 5 -18 R 9 -18 R 9 -36 R 10 -19 R 4 -18 R 10 -18 R 9 -18 R 5 -37 R 9 -18 R 5 -18 R 9 -36 R 9 -19 R 5 -18 R 9 -36 R 5 -18 R 9 -19 R 10 -36 R 4 -18 R 10 -37 R 4 -18 R 10 -18 R 9 -36 R 5 -19 R 14 -36 R 5 -18 R 9 -37 R 5 -18 R 9 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -19 R 10 -36 R 4 -18 R 10 -37 R 4 -18 R 10 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -19 R 9 -36 R 10 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -18 R 9 -37 R 9 -18 R 5 -36 R 9 -19 R 5 -36 R 9 -18 R 10 -18 R 4 -37 R 10 -18 R 4 -18 R 10 -37 R 9 -18 R 5 -18 R 9 -36 R 5 -19 R 9 -18 R 9 -36 R 10 -18 R 9 -19 R 5 -18 R 9 -18 R 5 -36 R 9 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 9 -19 R 10 -18 R 4 -18 R 10 -18 R 4 -18 R 10 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 14 0 R 4 -18 R 10 -19 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 19 R 9 18 R 10 0 R 9 18 R 5 18 R 9 18 R 5 0 R 9 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 10 18 R 4 18 R 10 18 R 4 18 R 10 19 R 9 36 R 5 18 R 9 18 R 5 19 R 9 18 R 9 36 R 10 18 R 9 19 R 5 18 R 9 36 R 5 18 R 9 19 R 9 36 R 5 18 R 9 37 R 5 18 R 9 18 R 10 36 R 4 19 R 10 36 R 4 18 R 10 37 R 9 18 R 5 36 R 9 18 R 5 37 R 14 18 R 4 36 R 10 19 R 9 36 R 5 18 R 9 37 R 5 18 R 9 36 R 9 18 R 5 37 R 9 18 R 5 36 R 9 19 R 10 36 R 4 18 R 10 37 R 4 18 R 10 36 R 9 18 R 5 37 R 9 18 R 9 36 R 10 19 R 4 18 R 10 36 R 9 18 R 5 37 R 9 18 R 5 36 R 9 19 R 9 18 R 5 36 R 9 18 R 5 19 R 10 36 R 9 18 R 5 18 R 9 37 R 5 18 R 9 18 R 9 18 R 5 19 R 14 36 R 5 18 R 9 18 R 5 19 R 9 18 R 9 18 R 5 36 R 9 19 R 5 18 R 9 18 R 10 18 R 4 18 R 10 19 R 4 18 R 10 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 10 0 R 9 18 R 5 19 R 9 18 R 5 18 R 9 18 R 9 0 R 5 18 R 9 19 R 5 18 R 9 0 R 10 18 R 4 18 R 10 0 R 4 18 R 10 19 R 9 0 R 5 18 R 9 18 R 5 0 R 14 18 R 4 0 R 10 18 R 9 0 R 5 19 R 9 0 R 5 18 R 9 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 18 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 19 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 14 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R D 7538 11353 M 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -19 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 19 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R D 13276 11480 M 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11444 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 14 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 -18 R 10 0 R 4 -18 R 10 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 0 R 10 -18 R 4 -19 R 10 -18 R 4 0 R 10 -18 R 9 -18 R 5 -18 R 9 -19 R 5 -18 R 14 0 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -18 R 10 -18 R 4 -19 R 10 -36 R 4 -18 R 10 -18 R 9 -19 R 5 -18 R 9 -18 R 9 -36 R 10 -19 R 4 -18 R 10 -18 R 9 -18 R 5 -37 R 9 -18 R 5 -18 R 9 -36 R 9 -19 R 5 -18 R 9 -36 R 5 -18 R 9 -19 R 10 -36 R 4 -18 R 10 -37 R 4 -18 R 10 -18 R 9 -36 R 5 -19 R 14 -36 R 5 -18 R 9 -37 R 5 -18 R 9 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -19 R 10 -36 R 4 -18 R 10 -37 R 4 -18 R 10 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -19 R 9 -36 R 10 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -18 R 9 -37 R 9 -18 R 5 -36 R 9 -19 R 5 -36 R 9 -18 R 10 -18 R 4 -37 R 10 -18 R 4 -18 R 10 -37 R 9 -18 R 5 -18 R 9 -36 R 5 -19 R 9 -18 R 9 -36 R 10 -18 R 9 -19 R 5 -18 R 9 -18 R 5 -36 R 9 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 9 -19 R 10 -18 R 4 -18 R 10 -18 R 4 -18 R 10 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 14 0 R 4 -18 R 10 -19 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 19 R 9 18 R 10 0 R 9 18 R 5 18 R 9 18 R 5 0 R 9 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 10 18 R 4 18 R 10 18 R 4 18 R 10 19 R 9 36 R 5 18 R 9 18 R 5 19 R 9 18 R 9 36 R 10 18 R 9 19 R 5 18 R 9 36 R 5 18 R 9 19 R 9 36 R 5 18 R 9 37 R 5 18 R 9 18 R 10 36 R 4 19 R 10 36 R 4 18 R 10 37 R 9 18 R 5 36 R 9 18 R 5 37 R 14 18 R 4 36 R 10 19 R 9 36 R 5 18 R 9 37 R 5 18 R 9 36 R 9 18 R 5 37 R 9 18 R 5 36 R 9 19 R 10 36 R 4 18 R 10 37 R 4 18 R 10 36 R 9 18 R 5 37 R 9 18 R 9 36 R 10 19 R 4 18 R 10 36 R 9 18 R 5 37 R 9 18 R 5 36 R 9 19 R 9 18 R 5 36 R 9 18 R 5 19 R 10 36 R 9 18 R 5 18 R 9 37 R 5 18 R 9 18 R 9 18 R 5 19 R 14 36 R 5 18 R 9 18 R 5 19 R 9 18 R 9 18 R 5 36 R 9 19 R 5 18 R 9 18 R 10 18 R 4 18 R 10 19 R 4 18 R 10 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 10 0 R 9 18 R 5 19 R 9 18 R 5 18 R 9 18 R 9 0 R 5 18 R 9 19 R 5 18 R 9 0 R 10 18 R 4 18 R 10 0 R 4 18 R 10 19 R 9 0 R 5 18 R 9 18 R 5 0 R 14 18 R 4 0 R 10 18 R 9 0 R 5 19 R 9 0 R 5 18 R 9 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 18 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 19 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 14 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R D 7538 11353 M 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 14 0 R 4 0 R 10 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 14 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -19 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 -19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 14 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 19 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 19 R 9 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 19 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 19 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R D 13276 11480 M 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11444 M 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 14 0 R 5 -18 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 -18 R 10 0 R 4 -18 R 10 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 0 R 9 -18 R 5 -18 R 9 0 R 10 -18 R 4 -19 R 10 -18 R 4 0 R 10 -18 R 9 -18 R 5 -18 R 9 -19 R 5 -18 R 14 0 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 9 -18 R 10 -18 R 4 -19 R 10 -36 R 4 -18 R 10 -18 R 9 -19 R 5 -18 R 9 -18 R 9 -36 R 10 -19 R 4 -18 R 10 -18 R 9 -18 R 5 -37 R 9 -18 R 5 -18 R 9 -36 R 9 -19 R 5 -18 R 9 -36 R 5 -18 R 9 -19 R 10 -36 R 4 -18 R 10 -37 R 4 -18 R 10 -18 R 9 -36 R 5 -19 R 14 -36 R 5 -18 R 9 -37 R 5 -18 R 9 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -19 R 10 -36 R 4 -18 R 10 -37 R 4 -18 R 10 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -19 R 9 -36 R 10 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -18 R 9 -37 R 9 -18 R 5 -36 R 9 -19 R 5 -36 R 9 -18 R 10 -18 R 4 -37 R 10 -18 R 4 -18 R 10 -37 R 9 -18 R 5 -18 R 9 -36 R 5 -19 R 9 -18 R 9 -36 R 10 -18 R 9 -19 R 5 -18 R 9 -18 R 5 -36 R 9 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 9 -19 R 10 -18 R 4 -18 R 10 -18 R 4 -18 R 10 -19 R 9 0 R 5 -18 R 9 -18 R 5 -18 R 14 0 R 4 -18 R 10 -19 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 9 -18 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -19 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 19 R 9 18 R 10 0 R 9 18 R 5 18 R 9 18 R 5 0 R 9 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 10 18 R 4 18 R 10 18 R 4 18 R 10 19 R 9 36 R 5 18 R 9 18 R 5 19 R 9 18 R 9 36 R 10 18 R 9 19 R 5 18 R 9 36 R 5 18 R 9 19 R 9 36 R 5 18 R 9 37 R 5 18 R 9 18 R 10 36 R 4 19 R 10 36 R 4 18 R 10 37 R 9 18 R 5 36 R 9 18 R 5 37 R 14 18 R 4 36 R 10 19 R 9 36 R 5 18 R 9 37 R 5 18 R 9 36 R 9 18 R 5 37 R 9 18 R 5 36 R 9 19 R 10 36 R 4 18 R 10 37 R 4 18 R 10 36 R 9 18 R 5 37 R 9 18 R 9 36 R 10 19 R 4 18 R 10 36 R 9 18 R 5 37 R 9 18 R 5 36 R 9 19 R 9 18 R 5 36 R 9 18 R 5 19 R 10 36 R 9 18 R 5 18 R 9 37 R 5 18 R 9 18 R 9 18 R 5 19 R 14 36 R 5 18 R 9 18 R 5 19 R 9 18 R 9 18 R 5 36 R 9 19 R 5 18 R 9 18 R 10 18 R 4 18 R 10 19 R 4 18 R 10 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 10 0 R 9 18 R 5 19 R 9 18 R 5 18 R 9 18 R 9 0 R 5 18 R 9 19 R 5 18 R 9 0 R 10 18 R 4 18 R 10 0 R 4 18 R 10 19 R 9 0 R 5 18 R 9 18 R 5 0 R 14 18 R 4 0 R 10 18 R 9 0 R 5 19 R 9 0 R 5 18 R 9 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 18 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 19 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 14 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R D 7538 11353 M 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -19 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 14 0 R 4 -18 R 10 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 -19 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 -19 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 -18 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 -19 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 -18 R 5 0 R 14 0 R 4 -18 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 -19 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 -19 R 9 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 -19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 19 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 14 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 0 R 4 18 R 10 0 R 4 18 R 10 0 R 9 0 R 5 19 R 9 0 R 9 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 9 19 R 5 0 R 9 0 R 5 18 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 18 R 9 0 R 9 0 R 10 19 R 4 0 R 10 18 R 4 0 R 10 18 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 0 R 4 19 R 10 0 R 4 18 R 10 0 R 9 18 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 10 0 R 9 19 R 5 0 R 9 18 R 5 0 R 9 18 R 9 0 R 5 0 R 9 18 R 5 0 R 9 18 R 10 0 R 4 0 R 10 19 R 4 0 R 10 18 R 9 0 R 5 0 R 9 18 R 5 0 R 14 18 R 4 0 R 10 0 R 9 18 R 5 0 R 9 19 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 19 R 9 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 19 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R D 13276 11480 M 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 1400 M 15300 0 R D 1800 1400 M 0 56 R D 1177 987 M -15 -15 R 15 -15 R 15 15 R 0 15 R -15 30 R -30 16 R -46 0 R -45 -16 R -31 -30 R -15 -30 R -15 -61 R 0 -91 R 15 -46 R 31 -30 R 45 -15 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f20b.eps0100644000000000000000000026267310376206774011053 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 13:08:34 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 19 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 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9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 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0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11462 M 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -18 R 14 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 9 -18 R 10 -19 R 4 -18 R 10 0 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 14 -18 R 4 -18 R 10 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 9 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -37 R 9 -18 R 10 -18 R 4 -18 R 10 -37 R 4 -18 R 10 -18 R 9 -36 R 5 -19 R 9 -18 R 9 -36 R 10 -18 R 4 -19 R 10 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -18 R 10 -36 R 4 -37 R 10 -18 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 14 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -36 R 9 -18 R 5 -37 R 9 -36 R 5 -37 R 9 -36 R 10 -18 R 4 -37 R 10 -36 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 9 -37 R 5 -36 R 9 -37 R 9 -36 R 10 -18 R 9 -37 R 5 -36 R 9 -36 R 5 -37 R 9 -18 R 9 -36 R 5 -37 R 9 -36 R 5 -18 R 9 -37 R 10 -36 R 4 -37 R 10 -18 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 9 -18 R 5 -37 R 9 -36 R 9 -18 R 10 -37 R 9 -18 R 5 -36 R 9 -19 R 5 -18 R 9 -36 R 9 -18 R 5 -19 R 9 -36 R 5 -18 R 9 -18 R 10 -19 R 4 -36 R 10 -18 R 4 -18 R 10 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 14 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 -18 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 19 R 9 0 R 5 18 R 9 18 R 5 18 R 9 0 R 9 18 R 10 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 9 18 R 5 18 R 9 18 R 5 37 R 9 18 R 10 18 R 4 18 R 10 37 R 4 18 R 10 36 R 9 18 R 5 19 R 9 36 R 5 18 R 9 37 R 9 18 R 10 36 R 9 37 R 5 18 R 9 36 R 5 18 R 9 37 R 9 36 R 5 18 R 9 37 R 5 36 R 9 37 R 10 18 R 4 36 R 10 37 R 4 36 R 10 18 R 9 37 R 5 36 R 9 36 R 5 37 R 14 18 R 4 36 R 10 37 R 9 36 R 5 37 R 9 36 R 5 18 R 9 37 R 9 36 R 5 36 R 9 37 R 5 18 R 9 36 R 10 37 R 4 36 R 10 37 R 4 18 R 10 36 R 9 37 R 5 36 R 9 18 R 9 37 R 10 36 R 4 18 R 10 37 R 9 36 R 5 18 R 9 37 R 5 36 R 9 18 R 9 37 R 5 18 R 9 36 R 5 37 R 10 18 R 9 36 R 5 18 R 9 37 R 5 18 R 9 36 R 9 19 R 5 18 R 14 36 R 5 18 R 9 19 R 5 36 R 9 18 R 9 18 R 5 37 R 9 18 R 5 18 R 9 18 R 10 37 R 4 18 R 10 18 R 4 18 R 10 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 9 18 R 10 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 5 18 R 9 0 R 5 19 R 9 18 R 10 18 R 4 0 R 10 18 R 4 18 R 10 19 R 9 0 R 5 18 R 9 18 R 5 0 R 14 18 R 4 0 R 10 18 R 9 19 R 5 0 R 9 18 R 5 0 R 9 18 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 19 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 9 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 14 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R D 7538 11298 M 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 19 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 5 -18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -19 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -19 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 9 0 R 5 0 R 9 19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 19 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 19 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R D 13276 11480 M 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11462 M 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -18 R 14 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 9 -18 R 10 -19 R 4 -18 R 10 0 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 14 -18 R 4 -18 R 10 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 9 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -37 R 9 -18 R 10 -18 R 4 -18 R 10 -37 R 4 -18 R 10 -18 R 9 -36 R 5 -19 R 9 -18 R 9 -36 R 10 -18 R 4 -19 R 10 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -18 R 10 -36 R 4 -37 R 10 -18 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 14 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -36 R 9 -18 R 5 -37 R 9 -36 R 5 -37 R 9 -36 R 10 -18 R 4 -37 R 10 -36 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 9 -37 R 5 -36 R 9 -37 R 9 -36 R 10 -18 R 9 -37 R 5 -36 R 9 -36 R 5 -37 R 9 -18 R 9 -36 R 5 -37 R 9 -36 R 5 -18 R 9 -37 R 10 -36 R 4 -37 R 10 -18 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 9 -18 R 5 -37 R 9 -36 R 9 -18 R 10 -37 R 9 -18 R 5 -36 R 9 -19 R 5 -18 R 9 -36 R 9 -18 R 5 -19 R 9 -36 R 5 -18 R 9 -18 R 10 -19 R 4 -36 R 10 -18 R 4 -18 R 10 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 14 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 -18 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 19 R 9 0 R 5 18 R 9 18 R 5 18 R 9 0 R 9 18 R 10 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 9 18 R 5 18 R 9 18 R 5 37 R 9 18 R 10 18 R 4 18 R 10 37 R 4 18 R 10 36 R 9 18 R 5 19 R 9 36 R 5 18 R 9 37 R 9 18 R 10 36 R 9 37 R 5 18 R 9 36 R 5 18 R 9 37 R 9 36 R 5 18 R 9 37 R 5 36 R 9 37 R 10 18 R 4 36 R 10 37 R 4 36 R 10 18 R 9 37 R 5 36 R 9 36 R 5 37 R 14 18 R 4 36 R 10 37 R 9 36 R 5 37 R 9 36 R 5 18 R 9 37 R 9 36 R 5 36 R 9 37 R 5 18 R 9 36 R 10 37 R 4 36 R 10 37 R 4 18 R 10 36 R 9 37 R 5 36 R 9 18 R 9 37 R 10 36 R 4 18 R 10 37 R 9 36 R 5 18 R 9 37 R 5 36 R 9 18 R 9 37 R 5 18 R 9 36 R 5 37 R 10 18 R 9 36 R 5 18 R 9 37 R 5 18 R 9 36 R 9 19 R 5 18 R 14 36 R 5 18 R 9 19 R 5 36 R 9 18 R 9 18 R 5 37 R 9 18 R 5 18 R 9 18 R 10 37 R 4 18 R 10 18 R 4 18 R 10 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 9 18 R 10 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 5 18 R 9 0 R 5 19 R 9 18 R 10 18 R 4 0 R 10 18 R 4 18 R 10 19 R 9 0 R 5 18 R 9 18 R 5 0 R 14 18 R 4 0 R 10 18 R 9 19 R 5 0 R 9 18 R 5 0 R 9 18 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 19 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 9 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 14 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R D 7538 11298 M 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 14 0 R 4 0 R 10 0 R 5 0 R 9 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 14 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 -19 R 5 0 R 9 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 14 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 0 R 9 -18 R 10 0 R 4 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -19 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 -18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 -19 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 -18 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 19 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 14 18 R 4 0 R 10 0 R 9 0 R 5 19 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 18 R 9 0 R 10 0 R 4 19 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 19 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 19 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 19 R 4 0 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 18 R 14 0 R 4 0 R 10 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 19 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 19 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 18 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 18 R 9 0 R 5 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 19 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 18 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R D 13276 11480 M 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 11462 M 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 -19 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 -18 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 -18 R 9 0 R 5 0 R 9 0 R 9 0 R 5 -18 R 10 0 R 4 0 R 10 0 R 9 -19 R 5 0 R 9 0 R 5 -18 R 9 0 R 9 0 R 5 -18 R 14 0 R 5 0 R 9 -18 R 5 0 R 9 0 R 9 -18 R 5 0 R 9 -19 R 5 0 R 9 0 R 10 -18 R 4 0 R 10 -18 R 4 0 R 10 -18 R 9 0 R 5 -18 R 9 0 R 5 -19 R 9 -18 R 9 0 R 10 -18 R 9 0 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 -18 R 5 -18 R 9 0 R 5 -18 R 9 -18 R 10 -19 R 4 -18 R 10 0 R 4 -18 R 10 -18 R 9 -18 R 5 -19 R 9 -18 R 5 -18 R 14 -18 R 4 -18 R 10 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 9 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -37 R 9 -18 R 10 -18 R 4 -18 R 10 -37 R 4 -18 R 10 -18 R 9 -36 R 5 -19 R 9 -18 R 9 -36 R 10 -18 R 4 -19 R 10 -36 R 9 -18 R 5 -37 R 9 -18 R 5 -36 R 9 -18 R 9 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -18 R 10 -36 R 4 -37 R 10 -18 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 14 -37 R 5 -18 R 9 -36 R 5 -37 R 9 -36 R 9 -18 R 5 -37 R 9 -36 R 5 -37 R 9 -36 R 10 -18 R 4 -37 R 10 -36 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 9 -37 R 5 -36 R 9 -37 R 9 -36 R 10 -18 R 9 -37 R 5 -36 R 9 -36 R 5 -37 R 9 -18 R 9 -36 R 5 -37 R 9 -36 R 5 -18 R 9 -37 R 10 -36 R 4 -37 R 10 -18 R 4 -36 R 10 -37 R 9 -18 R 5 -36 R 9 -18 R 5 -37 R 9 -36 R 9 -18 R 10 -37 R 9 -18 R 5 -36 R 9 -19 R 5 -18 R 9 -36 R 9 -18 R 5 -19 R 9 -36 R 5 -18 R 9 -18 R 10 -19 R 4 -36 R 10 -18 R 4 -18 R 10 -19 R 9 -18 R 5 -18 R 9 -18 R 5 -18 R 14 -19 R 4 -18 R 10 0 R 9 -18 R 5 -18 R 9 -18 R 5 0 R 9 -19 R 9 0 R 5 -18 R 9 0 R 5 -18 R 9 0 R 10 0 R 4 -18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 -18 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 18 R 4 0 R 10 18 R 4 0 R 10 19 R 9 0 R 5 18 R 9 18 R 5 18 R 9 0 R 9 18 R 10 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 9 18 R 5 18 R 9 18 R 5 37 R 9 18 R 10 18 R 4 18 R 10 37 R 4 18 R 10 36 R 9 18 R 5 19 R 9 36 R 5 18 R 9 37 R 9 18 R 10 36 R 9 37 R 5 18 R 9 36 R 5 18 R 9 37 R 9 36 R 5 18 R 9 37 R 5 36 R 9 37 R 10 18 R 4 36 R 10 37 R 4 36 R 10 18 R 9 37 R 5 36 R 9 36 R 5 37 R 14 18 R 4 36 R 10 37 R 9 36 R 5 37 R 9 36 R 5 18 R 9 37 R 9 36 R 5 36 R 9 37 R 5 18 R 9 36 R 10 37 R 4 36 R 10 37 R 4 18 R 10 36 R 9 37 R 5 36 R 9 18 R 9 37 R 10 36 R 4 18 R 10 37 R 9 36 R 5 18 R 9 37 R 5 36 R 9 18 R 9 37 R 5 18 R 9 36 R 5 37 R 10 18 R 9 36 R 5 18 R 9 37 R 5 18 R 9 36 R 9 19 R 5 18 R 14 36 R 5 18 R 9 19 R 5 36 R 9 18 R 9 18 R 5 37 R 9 18 R 5 18 R 9 18 R 10 37 R 4 18 R 10 18 R 4 18 R 10 19 R 9 18 R 5 18 R 9 18 R 5 18 R 9 19 R 9 18 R 10 18 R 9 18 R 5 18 R 9 19 R 5 18 R 9 18 R 9 18 R 5 18 R 9 0 R 5 19 R 9 18 R 10 18 R 4 0 R 10 18 R 4 18 R 10 19 R 9 0 R 5 18 R 9 18 R 5 0 R 14 18 R 4 0 R 10 18 R 9 19 R 5 0 R 9 18 R 5 0 R 9 18 R 9 0 R 5 18 R 9 0 R 5 18 R 9 0 R 10 19 R 4 0 R 10 0 R 4 18 R 10 0 R 9 0 R 5 18 R 9 0 R 9 18 R 10 0 R 4 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 19 R 9 0 R 9 0 R 5 0 R 9 18 R 5 0 R 9 0 R 10 0 R 4 18 R 10 0 R 4 0 R 10 0 R 9 0 R 5 18 R 14 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 18 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 19 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 18 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 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4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 10 18 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R D 13276 11480 M 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 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5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 9 0 R 10 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 14 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 9 0 R 5 0 R 9 0 R 5 0 R 9 0 R 10 0 R 4 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 9 0 R 9 0 R 10 0 R 4 0 R 10 0 R 9 0 R 5 0 R 8 0 R D L1 1800 11480 M 15299 0 R D L0 1800 1400 M 15300 0 R D 1800 1400 M 0 56 R D 1177 987 M -15 -15 R 15 -15 R 15 15 R 0 15 R -15 30 R -30 16 R -46 0 R -45 -16 R -31 -30 R -15 -30 R -15 -61 R 0 -91 R 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608 R 187 6 R 187 -435 R 186 364 R 187 -308 R 187 150 R 186 21 R 187 -311 R 186 643 R 186 -52 R 187 -435 R 187 38 R 186 422 R 187 -256 R 187 121 R 186 475 R 180 -546 R D 1800 3129 M 7 10 R 186 -275 R 186 -298 R 187 184 R 187 -125 R 186 180 R 187 -440 R 187 -162 R 186 -128 R 187 591 R 187 -276 R 185 138 R 187 34 R 187 -103 R 186 20 R 187 -187 R 187 154 R 186 138 R 187 -48 R 187 156 R 186 -43 R 187 120 R 186 68 R 187 108 R 186 -116 R 187 41 R 186 69 R 187 661 R 187 -587 R 186 -390 R 187 202 R 187 120 R 186 -160 R 186 74 R 187 364 R 187 -126 R 186 -241 R 187 177 R 186 -153 R 187 -234 R 187 170 R 186 119 R 187 5 R 186 -66 R 187 160 R 186 244 R 187 -42 R 187 -29 R 186 -77 R 187 -134 R 186 -155 R 187 -129 R 187 -46 R 186 452 R 186 60 R 187 -241 R 187 -313 R 186 185 R 187 404 R 187 -434 R 186 -83 R 187 133 R 187 -57 R 186 -9 R 186 67 R 187 -504 R 186 608 R 187 6 R 187 -435 R 186 364 R 187 -308 R 187 150 R 186 21 R 187 -311 R 186 643 R 186 -52 R 187 -435 R 187 38 R 186 422 R 187 -256 R 187 121 R 186 475 R 180 -546 R D 1800 3129 M 7 10 R 186 -275 R 186 -298 R 187 184 R 187 -125 R 186 180 R 187 -440 R 187 -162 R 186 -128 R 187 591 R 187 -276 R 185 138 R 187 34 R 187 -103 R 186 20 R 187 -187 R 187 154 R 186 138 R 187 -48 R 187 156 R 186 -43 R 187 120 R 186 68 R 187 108 R 186 -116 R 187 41 R 186 69 R 187 661 R 187 -587 R 186 -390 R 187 202 R 187 120 R 186 -160 R 186 86 R 187 364 R 187 -132 R 186 -223 R 187 179 R 186 -120 R 187 -211 R 187 205 R 186 153 R 187 56 R 186 -34 R 187 197 R 186 270 R 187 -35 R 187 -32 R 186 -102 R 187 -176 R 186 -204 R 187 -184 R 187 -85 R 186 417 R 186 40 R 187 -268 R 187 -311 R 186 174 R 187 404 R 187 -434 R 186 -83 R 187 133 R 187 -57 R 186 -9 R 186 67 R 187 -504 R 186 608 R 187 6 R 187 -435 R 186 364 R 187 -308 R 187 150 R 186 21 R 187 -311 R 186 643 R 186 -52 R 187 -435 R 187 38 R 186 422 R 187 -256 R 187 121 R 186 475 R 180 -546 R D L1 1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f21a.eps0100644000000000000000000006113210376206774011036 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 13:05:48 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 3534 1830 M 0 186 R D 3002 1281 M 274 0 R D 3397 1402 M 15 -15 R -15 -15 R -15 15 R 0 15 R 15 31 R 15 15 R 46 15 R 61 0 R 45 -15 R 15 -31 R 0 -45 R -15 -30 R -45 -16 R -46 0 R D 3519 1463 M 30 -15 R 15 -31 R 0 -45 R -15 -30 R -30 -16 R 30 -15 R 30 -30 R 15 -31 R 0 -45 R -15 -31 R -15 -15 R -45 -15 R -61 0 R -46 15 R -15 15 R -15 31 R 0 15 R 15 15 R 15 -15 R -15 -15 R D 3564 1296 M 15 -46 R 0 -45 R -15 -31 R -15 -15 R -30 -15 R D 3716 1174 M -15 -15 R 15 -15 R 15 15 R -15 15 R D 3929 1463 M -46 -15 R -30 -46 R -15 -76 R 0 -45 R 15 -76 R 30 -46 R 46 -15 R 30 0 R 46 15 R 30 46 R 15 76 R 0 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7 R 2 7 R 2 7 R 0 7 R F 5800 7406 M 0 -1400 R D 5660 6030 M 281 0 R -141 -243 R -140 243 R F 5791 9859 M 0 7 R -2 7 R -2 7 R -3 6 R -4 6 R -5 6 R -5 5 R -7 4 R -6 3 R -7 2 R -7 2 R -7 0 R -8 0 R -7 -2 R -7 -2 R -6 -3 R -6 -4 R -6 -5 R -4 -6 R -4 -6 R -4 -6 R -2 -7 R -1 -7 R -1 -7 R 1 -8 R 1 -7 R 2 -7 R 4 -6 R 4 -6 R 4 -6 R 6 -4 R 6 -4 R 6 -4 R 7 -2 R 7 -1 R 8 -1 R 7 1 R 7 1 R 7 2 R 6 4 R 7 4 R 5 4 R 5 6 R 4 6 R 3 6 R 2 7 R 2 7 R 0 8 R F 5736 9859 M 0 -1401 R D 5595 8483 M 281 0 R -140 -244 R -141 244 R F L1 2886 6458 M 14248 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f21b.eps0100644000000000000000000006541110376206774011043 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Tue Feb 14 13:05:48 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 4667 1830 M 0 186 R D 4120 1463 M -30 -152 R 30 31 R 46 15 R 45 0 R 46 -15 R 30 -31 R 16 -45 R 0 -31 R -16 -45 R -30 -31 R -46 -15 R -45 0 R -46 15 R -15 15 R -15 31 R 0 15 R 15 15 R 15 -15 R -15 -15 R D 4211 1357 M 31 -15 R 30 -31 R 15 -45 R 0 -31 R -15 -45 R -30 -31 R -31 -15 R D 4120 1463 M 152 0 R D 4120 1448 M 76 0 R 76 15 R D 4470 1463 M -46 -15 R -15 -31 R 0 -45 R 15 -30 R 46 -16 R 60 0 R 46 16 R 15 30 R 0 45 R -15 31 R -46 15 R -60 0 R -31 -15 R -15 -31 R 0 -45 R 15 -30 R 31 -16 R D 4530 1326 M 31 16 R 15 30 R 0 45 R -15 31 R -31 15 R D 4470 1326 M -46 -15 R -15 -15 R -15 -30 R 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510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 12:49:14 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F 7531 4052 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -9 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -14 R 1 -15 R 2 -14 R 5 -14 R 6 -13 R 9 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 0 R 14 0 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 10186 3959 M -1 14 R -3 15 R -4 13 R -7 13 R -8 13 R -10 10 R -10 10 R -13 8 R -13 7 R -13 4 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -10 R -9 -10 R -8 -13 R -7 -13 R -4 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 4 R 13 7 R 13 8 R 10 9 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 15 R F 10121 4399 M -1 14 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 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124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 124 22 R 125 22 R 124 23 R 124 22 R 125 22 R 124 23 R 124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 124 22 R 125 22 R 124 23 R 124 22 R 125 22 R 124 23 R 124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 125 22 R 124 23 R 124 22 R 125 22 R 124 23 R 124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 125 22 R 124 22 R 124 23 R 124 22 R 125 22 R 124 23 R 124 22 R 125 22 R 124 23 R 124 22 R 125 22 R 124 23 R 124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 125 23 R 124 22 R 124 22 R 124 23 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f22b.eps0100644000000000000000000010712210376206774011040 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 12:49:14 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 2886 1830 M 0 186 R D 2476 1463 M -46 -15 R -30 -46 R -15 -76 R 0 -45 R 15 -76 R 30 -46 R 46 -15 R 30 0 R 46 15 R 30 46 R 15 76 R 0 45 R -15 76 R -30 46 R -46 15 R -30 0 R -30 -15 R -16 -15 R -15 -31 R -15 -76 R 0 -45 R 15 -76 R 15 -31 R 16 -15 R 30 -15 R D 2506 1144 M 31 15 R 15 15 R 15 31 R 15 76 R 0 45 R -15 76 R -15 31 R -15 15 R -31 15 R D 2719 1174 M -15 -15 R 15 -15 R 15 15 R -15 15 R D 2932 1463 M -46 -15 R -30 -46 R -15 -76 R 0 -45 R 15 -76 R 30 -46 R 46 -15 R 30 0 R 46 15 R 30 46 R 15 76 R 0 45 R -15 76 R -30 46 R -46 15 R -30 0 R -31 -15 R -15 -15 R -15 -31 R -15 -76 R 0 -45 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R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 31 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 19 30 R 20 30 R 20 30 R 20 30 R 20 30 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f23a.eps0100644000000000000000000013135010376206774011040 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 14:18:33 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 3724 1830 M 0 226 R D 3193 1281 M 273 0 R D 3588 1402 M 15 -15 R -15 -15 R -16 15 R 0 15 R 16 31 R 15 15 R 45 15 R 61 0 R 46 -15 R 15 -31 R 0 -45 R -15 -30 R -46 -16 R -46 0 R D 3709 1463 M 30 -15 R 16 -31 R 0 -45 R -16 -30 R -30 -16 R 30 -15 R 31 -30 R 15 -31 R 0 -45 R -15 -31 R -15 -15 R -46 -15 R -61 0 R -45 15 R -15 15 R -16 31 R 0 15 R 16 15 R 15 -15 R -15 -15 R D 3755 1296 M 15 -46 R 0 -45 R -15 -31 R -16 -15 R -30 -15 R D 3906 1174 M -15 -15 R 15 -15 R 16 15 R -16 15 R D 4119 1463 M -45 -15 R -31 -46 R -15 -76 R 0 -45 R 15 -76 R 31 -46 R 45 -15 R 31 0 R 45 15 R 30 46 R 16 76 R 0 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112 R -19 -112 R D 6043 7850 M -18 -18 R 18 -19 R 19 19 R -19 18 R D 6043 7719 M 0 -261 R D 6062 7719 M 0 -261 R D 5987 7719 M 75 0 R D 5987 7458 M 131 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f23b.eps0100644000000000000000000013130710376206774011043 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/latex/articles/li_vlt %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 14:18:50 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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-18 R 18 -19 R 19 19 R -19 18 R D 6043 7719 M 0 -261 R D 6062 7719 M 0 -261 R D 5987 7719 M 75 0 R D 5987 7458 M 131 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f3.eps0100644000000000000000000014573310376206774010627 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 240 226 %%Title: Graphics produced by IDL %%For: pen@origo, /usr/users/pen/li6.paper/plot.figures %%Creator: IDL Version 6.1 (IRIX mipseb m64) %%CreationDate: Wed Aug 17 12:23:28 2005 %%DocumentData: Clean7bit %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 240 226 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Helvetica 423.333 /Helvetica STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 K 1275 800 M 6800 0 R D 1275 800 M 0 136 R D 1058 609 M -7 -7 R 7 -7 R 7 7 R 0 7 R -7 14 R -14 7 R -21 0 R -21 -7 R -14 -14 R -7 -14 R -7 -28 R 0 -42 R 7 -21 R 14 -14 R 21 -7 R 14 0 R 21 7 R 14 14 R 7 21 R 0 7 R -7 21 R -14 14 R -21 7 R -7 0 R -21 -7 R -14 -14 R -7 -21 R D 1023 630 M -14 -7 R -14 -14 R -7 -14 R -7 -28 R 0 -42 R 7 -21 R 14 -14 R 14 -7 R D 1030 483 M 14 7 R 14 14 R 7 21 R 0 7 R -7 21 R -14 14 R -14 7 R D 1114 630 M 0 -42 R D 1114 602 M 7 14 R 14 14 R 14 0 R 35 -21 R 14 0 R 7 7 R 7 14 R D 1121 616 M 14 7 R 14 0 R 35 -14 R D 1212 630 M 0 -21 R -7 -21 R -28 -35 R -7 -14 R -7 -21 R 0 -35 R D 1205 588 M -35 -35 R -7 -14 R -7 -21 R 0 -35 R D 1296 630 M 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29 R 9 -7 R 9 -8 R 9 5 R 10 6 R 9 17 R 9 26 R 9 -19 R 9 -16 R 9 -31 R 9 -16 R 9 25 R 9 -4 R 9 12 R 10 34 R 9 -24 R 9 -44 R 9 23 R 9 -2 R 9 -21 R 9 21 R 9 2 R 10 9 R 9 10 R 9 -1 R 9 29 R 9 -35 R 9 -36 R 9 57 R 9 44 R 9 -19 R 10 -50 R 9 -29 R 9 3 R 9 1 R 9 21 R 9 -6 R 9 -3 R 9 -3 R 9 -12 R 9 -8 R 9 41 R 10 37 R 9 -7 R 9 -37 R 9 -14 R 9 2 R 9 16 R 9 -5 R 9 13 R 9 9 R 10 14 R 9 36 R 9 -52 R 9 -25 R 9 20 R 9 7 R 9 3 R 9 5 R 10 -47 R 8 9 R 10 29 R 9 2 R 9 -32 R 9 9 R 9 46 R 9 10 R 9 -26 R 9 -2 R 9 -18 R 10 -10 R 9 -28 R 9 33 R 9 45 R 9 -29 R 9 -12 R 9 -11 R 9 2 R 9 19 R 10 -15 R 8 -23 R 10 17 R 9 -21 R 9 2 R 9 35 R 9 5 R 9 -19 R 9 9 R 10 10 R 9 -44 R 9 -17 R 9 28 R 9 -6 R 9 15 R 9 54 R 9 -7 R 9 -33 R 10 -19 R 9 -33 R 9 11 R 9 55 R 9 21 R 9 -36 R 9 -5 R 9 5 R 9 2 R 9 3 R 9 2 R 10 -19 R 9 -23 R 9 31 R 9 -5 R 9 -21 R 9 25 R 9 59 R 9 3 R 9 -53 R 9 -22 R 10 16 R 9 -30 R 9 13 R 9 -4 R 9 -6 R 9 18 R 9 -3 R 10 -24 R 9 22 R 9 11 R 9 18 R 9 -29 R 9 18 R 9 30 R 9 -7 R 9 18 R 9 -3 R 9 -29 R 10 -17 R 9 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9 -23 R 9 1 R 9 44 R 9 5 R 9 -5 R 10 -11 R 9 -42 R 9 20 R 9 31 R 9 32 R 9 27 R 9 -40 R 9 4 R 9 17 R 10 -42 R 9 6 R 9 21 R 9 -23 R 9 -7 R 7 -5 R D 1275 6828 M 8 18 R 9 -20 R 9 6 R 9 27 R 9 -45 R 10 -20 R 9 16 R 9 50 R 9 2 R 9 -34 R 9 24 R 9 7 R 9 -26 R 9 2 R 10 30 R 9 -5 R 9 -29 R 9 -4 R 9 16 R 9 7 R 9 -6 R 9 30 R 9 3 R 9 -39 R 9 0 R 10 1 R 9 0 R 9 -9 R 9 -3 R 9 43 R 9 9 R 9 15 R 9 -35 R 9 6 R 10 74 R 9 -95 R 9 -13 R 9 42 R 9 -26 R 9 -14 R 9 8 R 9 -6 R 10 -5 R 9 25 R 9 68 R 9 -73 R 9 -29 R 9 64 R 9 -38 R 9 -27 R 9 23 R 9 43 R 9 -19 R 10 -46 R 9 2 R 9 31 R 9 10 R 9 -4 R 9 -19 R 9 7 R 9 -6 R 9 6 R 10 25 R 9 -27 R 9 -3 R 9 10 R 9 -7 R 9 -16 R 9 33 R 9 16 R 9 -43 R 10 -15 R 9 28 R 9 -12 R 9 -24 R 9 20 R 9 26 R 9 -6 R 9 -11 R 9 -10 R 9 -6 R 10 23 R 9 2 R 9 -24 R 9 -19 R 9 24 R 9 19 R 9 -9 R 9 -8 R 9 18 R 10 12 R 9 -28 R 9 -14 R 9 19 R 9 -3 R 9 -24 R 9 11 R 9 4 R 9 -15 R 9 7 R 9 23 R 10 -31 R 9 60 R 9 21 R 9 -53 R 9 -11 R 9 10 R 9 23 R 10 -14 R 9 -26 R 9 21 R 9 20 R 9 8 R 9 -3 R 9 -20 R 9 16 R 9 34 R 9 -27 R 9 -52 R 10 -13 R 9 6 R 9 19 R 9 -4 R 9 29 R 9 34 R 9 -27 R 9 -20 R 9 -22 R 10 9 R 9 -6 R 9 -11 R 9 -7 R 9 -1 R 9 12 R 9 -16 R 9 16 R 9 -30 R 9 36 R 10 11 R 9 5 R 9 -20 R 9 34 R 9 9 R 9 -13 R 9 -1 R 9 -12 R 9 -24 R 10 -3 R 9 -7 R 9 -5 R 9 45 R 9 -2 R 9 8 R 9 -13 R 9 -6 R 9 0 R 10 11 R 9 30 R 9 -42 R 9 -5 R 9 38 R 9 -11 R 9 -7 R 9 18 R 9 -32 R 9 6 R 9 31 R 10 15 R 9 -23 R 9 -50 R 9 45 R 9 9 R 9 14 R 9 -31 R 10 -18 R 9 18 R 9 10 R 9 17 R 9 -36 R 9 -4 R 9 16 R 9 0 R 9 -6 R 9 19 R 10 13 R 9 -27 R 9 8 R 9 -9 R 9 7 R 9 -14 R 9 5 R 9 -3 R 9 0 R 9 29 R 9 -6 R 10 9 R 9 0 R 9 -36 R 9 -8 R 9 -9 R 9 1 R 9 2 R 9 0 R 9 3 R 10 9 R 9 14 R 9 -6 R 9 11 R 9 -47 R 9 23 R 9 21 R 10 -3 R 8 -13 R 10 7 R 9 5 R 9 -19 R 9 20 R 9 10 R 9 -30 R 9 0 R 9 33 R 9 25 R 10 5 R 9 -12 R 9 -5 R 9 -8 R 9 -26 R 9 -15 R 9 -6 R 9 20 R 9 11 R 10 7 R 8 -5 R 10 -1 R 9 -17 R 9 -26 R 9 -19 R 9 22 R 9 31 R 9 16 R 9 3 R 10 -7 R 9 -9 R 9 38 R 9 18 R 9 -50 R 9 -28 R 9 12 R 9 21 R 9 -18 R 10 -16 R 9 -9 R 9 23 R 9 -2 R 9 -33 R 9 -1 R 9 -19 R 9 68 R 9 23 R 9 -15 R 9 -12 R 10 17 R 9 -6 R 9 -24 R 9 25 R 9 11 R 9 -9 R 9 -17 R 9 3 R 9 20 R 10 1 R 9 0 R 9 6 R 9 -14 R 9 1 R 9 40 R 9 -7 R 9 -32 R 10 -9 R 9 -6 R 9 -21 R 9 -30 R 9 -44 R 9 -97 R 9 -116 R 9 -138 R 9 -149 R 9 -151 R 10 -158 R 9 -96 R 9 -11 R 9 14 R 9 39 R 9 81 R 9 121 R 9 105 R 9 91 R 9 66 R 10 99 R 9 136 R 9 96 R 9 64 R 9 16 R 9 29 R 9 15 R 9 20 R 9 -9 R 10 7 R 9 -1 R 9 35 R 9 18 R 9 -15 R 9 8 R 9 -22 R 9 -23 R 9 1 R 10 16 R 9 46 R 9 0 R 9 -46 R 9 -35 R 9 19 R 9 23 R 9 -20 R 9 3 R 10 4 R 8 -27 R 10 43 R 9 -19 R 9 -40 R 9 3 R 9 14 R 9 11 R 9 9 R 9 56 R 9 -1 R 10 -10 R 9 -24 R 9 -11 R 9 -15 R 9 -41 R 9 39 R 9 -10 R 9 30 R 10 1 R 9 3 R 9 -2 R 9 -1 R 9 12 R 9 -16 R 9 26 R 9 0 R 9 -39 R 9 17 R 9 13 R 10 5 R 9 -22 R 9 -22 R 9 14 R 9 19 R 9 15 R 9 -15 R 9 9 R 9 -28 R 10 -14 R 9 -8 R 9 40 R 9 12 R 9 -24 R 9 -8 R 9 8 R 9 20 R 9 -11 R 10 -11 R 9 -30 R 9 26 R 9 11 R 9 11 R 9 8 R 9 -9 R 9 -13 R 9 12 R 10 -2 R 9 -12 R 9 -8 R 9 -3 R 9 42 R 9 -1 R 9 -18 R 9 -9 R 9 0 R 10 -14 R 9 18 R 9 -22 R 9 11 R 9 -3 R 9 8 R 9 -19 R 9 23 R 9 6 R 9 3 R 9 3 R 10 2 R 9 -27 R 9 -7 R 9 26 R 9 13 R 9 26 R 9 -5 R 9 -5 R 10 -43 R 9 -22 R 9 18 R 9 26 R 9 -4 R 9 30 R 9 -45 R 9 -28 R 9 18 R 10 -10 R 8 -10 R 10 31 R 9 2 R 9 4 R 9 -2 R 9 -32 R 9 10 R 9 1 R 9 0 R 9 22 R 10 -7 R 9 -7 R 9 1 R 9 -5 R 9 24 R 9 -9 R 9 0 R 9 23 R 9 -21 R 10 -33 R 9 17 R 9 -3 R 9 -48 R 9 40 R 9 41 R 9 -22 R 9 -5 R 9 13 R 10 29 R 9 3 R 9 -27 R 9 -12 R 9 20 R 9 -8 R 9 -6 R 9 9 R 9 -5 R 9 -7 R 10 6 R 9 -4 R 9 -7 R 9 -2 R 9 24 R 9 5 R 9 -2 R 9 -11 R 9 -8 R 9 -11 R 10 -1 R 9 3 R 9 17 R 9 -3 R 9 8 R 9 12 R 9 -7 R 9 44 R 10 37 R 9 -53 R 9 -25 R 9 28 R 9 -18 R 9 -53 R 9 10 R 9 13 R 9 -28 R 10 0 R 9 13 R 9 22 R 9 6 R 9 -2 R 9 -2 R 9 -2 R 9 -16 R 9 19 R 9 -17 R 9 -6 R 10 21 R 9 -20 R 9 -2 R 9 17 R 9 18 R 9 -39 R 9 14 R 9 19 R 9 -12 R 10 -10 R 9 32 R 9 28 R 9 -3 R 9 6 R 9 -24 R 9 -39 R 9 10 R 10 24 R 8 20 R 10 -18 R 9 -11 R 9 1 R 9 -13 R 9 -25 R 9 -15 R 9 19 R 9 16 R 9 -21 R 10 -9 R 9 20 R 9 -10 R 9 0 R 9 30 R 9 6 R 9 -36 R 9 -17 R 9 -18 R 10 1 R 8 15 R 10 45 R 9 -3 R 9 -13 R 9 15 R 9 24 R 9 -4 R 9 17 R 10 -17 R 9 -22 R 9 -11 R 9 1 R 9 2 R 9 3 R 9 -14 R 9 -2 R 9 -10 R 10 30 R 9 -7 R 9 -12 R 9 20 R 9 8 R 9 26 R 9 -39 R 9 -14 R 9 -5 R 9 28 R 9 34 R 10 -14 R 9 5 R 9 28 R 9 -24 R 9 -51 R 9 42 R 9 27 R 9 -37 R 9 7 R 9 8 R 10 -17 R 9 -1 R 9 5 R 9 -2 R 9 -18 R 9 -20 R 9 13 R 10 7 R 9 -24 R 9 -12 R 9 81 R 9 -41 R 9 -1 R 9 5 R 9 -19 R 9 1 R 9 27 R 9 14 R 10 -63 R 9 -3 R 9 16 R 9 -7 R 9 22 R 9 64 R 9 -64 R 9 -34 R 9 39 R 10 -19 R 9 -2 R 9 13 R 9 -5 R 9 6 R 9 0 R 9 -6 R 9 7 R 9 12 R 10 -3 R 9 2 R 9 -14 R 9 26 R 9 38 R 9 -17 R 9 -21 R 9 -9 R 9 -9 R 9 -25 R 10 17 R 9 3 R 9 47 R 9 -6 R 9 -23 R 9 9 R 9 -15 R 9 -35 R 9 8 R 10 22 R 9 26 R 9 30 R 9 -19 R 9 -39 R 9 15 R 9 4 R 9 -27 R 9 3 R 9 52 R 9 -12 R 10 -30 R 9 -17 R 9 24 R 9 9 R 9 -21 R 9 -24 R 9 -3 R 10 25 R 9 25 R 9 -25 R 9 8 R 9 3 R 9 -4 R 9 -12 R 9 -8 R 9 -2 R 9 -33 R 9 -30 R 10 -12 R 9 -22 R 9 -9 R 9 -48 R 9 4 R 9 30 R 9 33 R 9 85 R 9 10 R 10 -16 R 9 -5 R 9 25 R 9 36 R 9 12 R 9 -9 R 9 -12 R 9 5 R 9 -7 R 9 -39 R 10 14 R 9 6 R 9 22 R 9 8 R 9 -31 R 9 -7 R 9 14 R 9 -8 R 9 -3 R 10 11 R 9 -1 R 9 -21 R 9 38 R 9 41 R 9 -40 R 9 -10 R 9 -21 R 9 22 R 10 45 R 9 -28 R 9 -39 R 9 -12 R 9 20 R 9 4 R 9 -18 R 9 20 R 9 6 R 9 -32 R 9 26 R 10 20 R 9 -50 R 9 12 R 9 16 R 9 -16 R 9 25 R 9 -37 R 9 10 R 10 -1 R 9 23 R 9 -13 R 9 18 R 9 -41 R 9 -17 R 9 35 R 9 19 R 9 8 R 10 6 R 9 -33 R 9 -13 R 9 54 R 9 37 R 9 -32 R 9 -25 R 9 6 R 9 15 R 9 -9 R 9 -2 R 10 41 R 9 -46 R 9 -35 R 9 -17 R 9 2 R 9 24 R 9 7 R 9 -6 R 9 -26 R 10 12 R 9 -1 R 9 25 R 9 30 R 9 1 R 7 -21 R D %%PageTrailer end %%PageResources: font Helvetica %%Trailer %%Pages: 1 %%DocumentNeededResources: font Helvetica %%EOF f4.eps0100644000000000000000000131075210376206774010624 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 240 198 %%Title: Graphics produced by IDL %%For: pen@origo, /usr/users/pen/li6.paper/plot.figures %%Creator: IDL Version 6.1 (IRIX mipseb m64) %%CreationDate: Wed Aug 17 12:18:00 2005 %%DocumentData: Clean7bit %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 240 198 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Helvetica 423.333 /Helvetica STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 K 1275 700 M 6800 0 R D 1275 700 M 0 119 R D 1030 446 M 126 0 R D 1219 530 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 1359 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 1422 495 M 0 7 R 7 14 R 7 7 R 14 7 R 28 0 R 14 -7 R 7 -7 R 7 -14 R 0 -14 R -7 -14 R -14 -21 R -70 -70 R 98 0 R D 2125 700 M 0 119 R D 1880 446 M 126 0 R D 2062 495 M 0 7 R 7 14 R 7 7 R 14 7 R 28 0 R 14 -7 R 7 -7 R 7 -14 R 0 -14 R -7 -14 R -14 -21 R -70 -70 R 98 0 R D 2209 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 2335 530 M -70 -98 R 105 0 R D 2335 530 M 0 -147 R D 2975 700 M 0 119 R D 2730 446 M 126 0 R D 2926 502 M 14 7 R 21 21 R 0 -147 R D 3059 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 3206 509 M -7 14 R -21 7 R -14 0 R -21 -7 R -14 -21 R -7 -35 R 0 -35 R 7 -28 R 14 -14 R 21 -7 R 7 0 R 21 7 R 14 14 R 7 21 R 0 7 R -7 21 R -14 14 R -21 7 R -7 0 R -21 -7 R -14 -14 R -7 -21 R D 3825 700 M 0 119 R D 3580 446 M 126 0 R D 3797 530 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 3909 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 4000 530 M -21 -7 R -7 -14 R 0 -14 R 7 -14 R 14 -7 R 28 -7 R 21 -7 R 14 -14 R 7 -14 R 0 -21 R -7 -14 R -7 -7 R -21 -7 R -28 0 R -21 7 R -7 7 R -7 14 R 0 21 R 7 14 R 14 14 R 21 7 R 28 7 R 14 7 R 7 14 R 0 14 R -7 14 R -21 7 R -28 0 R D 4675 700 M 0 119 R D 4556 530 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 4668 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 4766 530 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 5525 700 M 0 119 R D 5406 530 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 5518 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 5609 530 M -21 -7 R -7 -14 R 0 -14 R 7 -14 R 14 -7 R 28 -7 R 21 -7 R 14 -14 R 7 -14 R 0 -21 R -7 -14 R -7 -7 R -21 -7 R -28 0 R -21 7 R -7 7 R -7 14 R 0 21 R 7 14 R 14 14 R 21 7 R 28 7 R 14 7 R 7 14 R 0 14 R -7 14 R -21 7 R -28 0 R D 6375 700 M 0 119 R D 6235 502 M 14 7 R 21 21 R 0 -147 R D 6368 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 6515 509 M -7 14 R -21 7 R -14 0 R -21 -7 R -14 -21 R -7 -35 R 0 -35 R 7 -28 R 14 -14 R 21 -7 R 7 0 R 21 7 R 14 14 R 7 21 R 0 7 R -7 21 R -14 14 R -21 7 R -7 0 R -21 -7 R -14 -14 R -7 -21 R D 7225 700 M 0 119 R D 7071 495 M 0 7 R 7 14 R 7 7 R 14 7 R 28 0 R 14 -7 R 7 -7 R 7 -14 R 0 -14 R -7 -14 R -14 -21 R -70 -70 R 98 0 R D 7218 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 7344 530 M -70 -98 R 105 0 R D 7344 530 M 0 -147 R 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5167 M -1 3 R -1 1 R 0 -8 R 1 1 R 1 3 R F 1279 5143 M 0 3 R -2 2 R -2 2 R 0 -14 R 2 1 R 2 3 R 0 3 R F 1282 5325 M 0 3 R -2 2 R -3 2 R -2 0 R 0 -15 R 2 0 R 3 2 R 2 3 R 0 3 R F 1285 5363 M -1 3 R -1 2 R -3 2 R -3 0 R -2 0 R 0 -15 R 2 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1288 5237 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -2 -2 R 0 -12 R 2 0 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1291 5318 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1293 5388 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1296 5231 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1299 5266 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1302 5294 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1304 5220 M 0 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3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 1352 5293 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1355 5338 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1357 5354 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1360 5308 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1363 5275 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1366 5325 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 1369 5373 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1371 5238 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 1374 5091 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1377 5155 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1380 5282 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1382 5311 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 1385 5281 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 1388 5274 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1391 5234 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1394 5064 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 1396 5185 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 1399 5414 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 1402 5380 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1405 5254 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 1408 5207 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1410 5244 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 1413 5311 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1416 5341 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1419 5304 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1421 5259 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1424 5168 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1427 5274 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1430 5311 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1433 5172 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1435 5188 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1438 5240 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1441 5239 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1444 5238 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1447 5237 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1449 5236 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1452 5235 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1455 5234 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1458 5151 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1460 5180 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1463 5049 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1466 5131 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1469 5198 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1472 5154 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1474 5211 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1477 5230 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 1480 5167 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1483 5218 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1486 5311 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1488 5237 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1491 5146 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 1494 5328 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1497 5311 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1499 5214 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1502 5259 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 1505 5241 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1508 5209 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1511 5214 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1513 5246 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1516 5199 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1519 5135 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1522 5184 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1525 5095 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 1527 5114 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1530 5206 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1533 5080 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1536 5161 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1538 5190 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1541 5235 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 1544 5294 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1547 5264 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1550 5228 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1552 5259 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1555 5309 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1558 5272 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1561 5272 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1564 5269 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1566 5268 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1569 5371 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1572 5332 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1575 5245 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1577 5231 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1580 5221 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1583 5229 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1586 5202 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1589 5207 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1591 5207 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1594 5206 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1597 5188 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1600 5264 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1603 5230 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1605 5140 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1608 5177 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1611 5065 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1614 5101 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1617 5215 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1619 5187 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1622 5213 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1625 5236 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1628 5195 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1630 5159 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 1633 5133 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1636 5170 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1639 5174 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1642 5080 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1644 5167 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1647 5310 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1650 5340 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1653 5345 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 1656 5291 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1658 5246 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 1661 5287 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1664 5190 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1667 5247 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1669 5297 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1672 5215 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1675 5185 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1678 5171 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1681 5159 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1683 5223 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1686 5286 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1689 5176 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 1692 5108 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1695 5173 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1697 5236 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 1700 5247 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1703 5198 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1706 5226 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1708 5283 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1711 5137 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1714 5047 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1717 5138 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1720 5258 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1722 5242 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1725 5212 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1728 5248 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1731 5213 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1734 5208 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1736 5286 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1739 5148 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1742 4980 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1745 5102 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 1747 5125 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1750 5145 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1753 5214 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1756 5239 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1759 5305 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1761 5240 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1764 5101 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1767 5230 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1770 5379 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1773 5377 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1775 5352 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1778 5229 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 1781 5129 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 1784 5185 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1786 5164 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1789 5056 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 1792 5106 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 1795 5137 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1798 5191 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1800 5252 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1803 5115 M 0 2 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 1806 5123 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1809 5239 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1812 5163 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1814 5159 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 1817 5247 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1820 5200 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1823 5006 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1825 5037 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 1828 5151 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1831 5134 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1834 5147 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1837 5119 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1839 5190 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1842 5188 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1845 5187 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 1848 5005 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 1851 5020 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1853 5192 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1856 5251 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1859 5177 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1862 5148 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1864 5187 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1867 5202 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1870 5142 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1873 5169 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 1876 5202 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 1878 5361 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 1881 5349 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 1884 5152 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1887 5149 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1890 5345 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1892 5429 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1895 5221 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1898 5061 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1901 5163 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1903 5308 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 1906 5242 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 1909 5049 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1912 5038 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1915 5238 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1917 5339 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1920 5207 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1923 5095 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1926 5124 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 1929 5095 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1931 5135 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1934 5143 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 1937 5174 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1940 5235 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1942 5159 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 1945 5074 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 1948 5148 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1951 5245 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1954 5182 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 1956 5128 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 1959 5119 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 1962 5148 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 1965 5248 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1968 5255 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1970 5175 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 1973 5139 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 1976 5131 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 1979 5100 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 1981 4951 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1984 4934 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 1987 5036 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1990 5034 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 1993 4992 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 1995 5066 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 1998 5137 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2001 5135 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2004 5170 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2007 5164 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2009 5133 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2012 5094 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2015 4982 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2018 4929 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2021 4951 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2023 5057 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2026 5029 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2029 4859 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2032 4892 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2034 4839 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 2037 5050 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2040 5048 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2043 5046 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2046 5043 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2048 5041 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2051 4856 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2054 4926 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2057 4960 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2060 5089 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2062 5004 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2065 4989 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2068 5176 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2071 5148 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2073 5066 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2076 5031 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2079 5038 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2082 5067 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2085 5037 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2087 4988 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2090 4983 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2093 5104 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2096 5119 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2099 5027 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2101 5026 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2104 5050 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2107 4948 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2110 4962 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2112 4984 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2115 4814 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2118 4845 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2121 4975 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2124 4937 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2126 4883 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2129 4879 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2132 5028 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2135 5018 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2138 5032 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2140 5034 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2143 4844 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2146 4933 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2149 5022 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2151 4894 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 2154 5030 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2157 5185 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2160 5080 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2163 4975 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2165 5012 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2168 5019 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2171 4933 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2174 4963 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2177 5117 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2179 5104 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2182 4942 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2185 5004 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2188 5053 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2190 5069 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2193 4947 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2196 4943 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2199 4942 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2202 4941 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2204 4940 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 2207 4938 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 2 R F 2210 4938 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2213 4937 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2216 4936 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2218 4935 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2221 4934 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2224 4933 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2227 4732 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2229 4826 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2232 4792 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 2235 4787 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2238 4892 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2241 5008 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2243 4982 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2246 4914 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2249 4867 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2252 4801 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2255 4858 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2257 4876 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2260 4838 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2263 4878 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2266 4794 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2268 4813 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2271 4888 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 2274 4845 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2277 4874 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2280 4792 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2282 4905 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 2285 5092 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2288 5072 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2291 5015 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2294 4931 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2296 4938 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2299 4980 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2302 4974 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2305 5039 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2308 5124 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2310 5110 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2313 5038 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 2316 5048 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2319 5037 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2321 4941 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2324 4936 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2327 4934 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2330 4827 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2333 4781 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2335 4878 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2338 4958 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2341 4892 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2344 4888 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2347 4941 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2349 4939 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2352 4944 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2355 4902 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2358 4866 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2360 4959 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2363 4919 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2366 4930 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2369 4965 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2372 4932 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 2374 4988 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2377 5035 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2380 4962 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2383 4831 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2386 4795 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2388 4833 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 2391 4716 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 2394 4739 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2397 4781 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2399 4787 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 2402 4905 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2405 4904 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2408 4903 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2411 4901 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2413 4900 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2416 4898 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2419 4897 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2422 4895 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2425 4893 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2427 4726 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 2430 4890 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2433 4888 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2436 4886 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2438 4947 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2441 5047 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2444 4976 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2447 4873 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2450 4873 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2452 4924 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2455 4826 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2458 4820 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2461 4695 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2464 4753 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2466 4989 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2469 4914 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2472 4782 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2475 4805 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2477 4765 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2480 4787 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2483 4935 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2486 4896 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2489 4852 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2491 4853 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2494 4830 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2497 4863 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2500 4833 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2503 4850 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2505 4892 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2508 4864 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2511 4850 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2514 4814 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2516 4766 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 2519 4750 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 2522 4751 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 2525 4922 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2528 4837 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2530 4709 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2533 4724 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2536 4702 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2539 4767 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2542 4828 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2544 4732 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2547 4718 M 0 2 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2550 4840 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2553 4839 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2555 4756 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2558 4847 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2561 4842 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2564 4712 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2567 4675 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2569 4672 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2572 4723 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2575 4803 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2578 4791 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2581 4695 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2583 4616 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2586 4792 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2589 4972 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2592 4819 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2595 4721 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2597 4660 M 0 2 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2600 4677 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2603 4698 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2606 4695 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2608 4692 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2611 4689 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2614 4686 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2617 4684 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2620 4681 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2622 4678 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2625 4675 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2628 4673 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2631 4670 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2634 4765 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2636 4815 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2639 4640 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 2642 4556 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2645 4606 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2647 4626 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2650 4676 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2653 4714 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2656 4693 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 2659 4686 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2661 4767 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2664 4751 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2667 4651 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2670 4674 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2672 4668 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2675 4633 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 2678 4635 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2681 4588 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2684 4532 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2686 4470 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 2689 4512 M 0 2 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2692 4520 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2695 4485 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2698 4617 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 2700 4616 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2703 4614 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2706 4612 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2709 4610 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2711 4609 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 2714 4607 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 2717 4605 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2720 4603 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2723 4601 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 2725 4600 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2728 4598 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2731 4596 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2734 4555 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2737 4534 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2739 4532 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2742 4585 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2745 4513 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2748 4496 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2751 4563 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2753 4518 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2756 4542 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2759 4478 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2762 4539 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2764 4574 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2767 4497 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 2 R F 2770 4455 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2773 4387 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2776 4421 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2778 4437 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2781 4527 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2784 4676 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2787 4603 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2790 4604 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2792 4706 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2795 4530 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2798 4501 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2801 4644 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2803 4626 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2806 4493 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2809 4456 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2812 4525 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2815 4491 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2817 4399 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2820 4449 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2823 4647 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2826 4778 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2829 4614 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2831 4464 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2834 4642 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2837 4668 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2840 4583 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2842 4587 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 2845 4576 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2848 4544 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2851 4485 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2854 4509 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2856 4655 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2859 4665 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2862 4577 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2865 4582 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2868 4484 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2870 4498 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2873 4648 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2876 4706 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2879 4429 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2881 4306 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2884 4484 M 0 2 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 2887 4481 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2890 4478 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2893 4518 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2895 4462 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2898 4526 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2901 4326 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2904 4404 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2907 4496 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 2909 4396 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2912 4454 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2915 4451 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2918 4448 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2920 4445 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2923 4442 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2926 4439 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2929 4435 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2932 4432 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 2934 4429 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2937 4445 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2940 4359 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 2943 4428 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 2946 4523 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2948 4456 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 2951 4339 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 2954 4356 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 2957 4444 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2959 4461 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 2962 4369 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 2965 4400 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 2968 4441 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2971 4328 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2973 4335 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2976 4429 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 2979 4430 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2982 4458 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 2985 4368 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2987 4324 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 2990 4433 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 2993 4538 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 2996 4526 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 2998 4225 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3001 4127 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 3004 4250 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3007 4264 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3010 4251 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3012 4336 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3015 4457 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3018 4426 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3021 4280 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3024 4259 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3026 4280 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3029 4362 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3032 4311 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3035 4270 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3038 4195 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3040 4176 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3043 4220 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3046 4209 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3049 4179 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3051 4245 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 3054 4320 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3057 4285 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3060 4303 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3063 4334 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3065 4316 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3068 4275 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3071 4084 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3074 4217 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3077 4212 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3079 4207 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3082 4117 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3085 4273 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3088 4252 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3090 4134 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3093 4067 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3096 4128 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3099 4120 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3102 4080 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3104 4158 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3107 4080 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3110 4060 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3113 4080 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3116 4074 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3118 3933 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 3121 3924 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3124 4123 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3127 4118 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3129 4113 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3132 4107 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3135 4102 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3138 4097 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3141 4091 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3143 4086 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3146 4080 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3149 4075 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3152 4070 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3155 4064 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3157 4059 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 3160 3917 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3163 4006 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3166 3992 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3168 3968 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3171 3964 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3174 4056 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3177 4101 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3180 4108 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3182 4144 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3185 4057 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3188 3949 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3191 3918 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3194 4116 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3196 4081 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3199 4135 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3202 4155 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3205 4125 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3207 4027 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3210 3960 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3213 4029 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3216 4047 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3219 3891 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3221 3836 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3224 3955 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 3227 3968 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3230 3957 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3233 3914 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3235 3909 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3238 3903 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3241 4003 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3244 3863 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3246 4012 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3249 4129 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 3252 3877 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3255 3872 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3258 3866 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3260 3861 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3263 3856 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3266 3850 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3269 3845 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3272 3656 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3274 3701 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3277 3702 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3280 3757 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3283 3788 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3285 3848 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3288 3889 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 3291 3793 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3294 3853 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3297 3864 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 3299 3758 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3302 3712 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3305 3702 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3308 3771 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3311 3765 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3313 3760 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3316 3725 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3319 3785 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3322 3776 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3325 3725 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3327 3704 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3330 3716 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3333 3787 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3336 3855 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3338 3797 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3341 3756 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 3344 3780 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3347 3692 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3350 3625 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3352 3471 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3355 3532 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3358 3601 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3361 3452 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3364 3551 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3366 3625 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3369 3707 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3372 3756 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3375 3685 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3377 3654 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3380 3667 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3383 3691 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3386 3649 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3389 3567 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3391 3510 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3394 3407 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3397 3426 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3400 3524 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3402 3636 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3405 3634 M 0 2 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 3408 3489 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3411 3566 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3414 3736 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3416 3637 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3419 3537 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3422 3602 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3425 3567 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3428 3516 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3430 3461 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3433 3345 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3436 3396 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3439 3478 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3441 3419 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3444 3535 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 3447 3656 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3450 3584 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3453 3501 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3455 3516 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3458 3494 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3461 3432 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3464 3437 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3467 3391 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3469 3439 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3472 3460 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3475 3450 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3478 3465 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3481 3372 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3483 3399 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3486 3367 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3489 3284 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3492 3385 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3494 3468 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3497 3464 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3500 3364 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3503 3358 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3506 3485 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3508 3463 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3511 3405 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3514 3436 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3517 3392 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3520 3329 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3522 3321 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3525 3312 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3528 3268 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3531 3320 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3533 3254 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3536 3294 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3539 3273 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3542 3287 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3545 3245 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3547 3181 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3550 3261 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 3553 3233 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3556 3216 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3559 3250 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3561 3181 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3564 3175 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3567 3178 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3570 3120 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3572 3066 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3575 3072 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3578 3261 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3581 3355 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3584 3200 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3586 3142 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3589 3190 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3592 3245 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3595 3049 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3598 2995 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3600 3150 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3603 3011 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3606 2922 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3609 3062 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3611 3053 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3614 3044 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 2 R F 3617 3035 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3620 3026 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3623 3017 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3625 3008 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3628 2999 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3631 2990 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3634 2893 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3637 2941 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3639 2891 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3642 2870 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3645 2823 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3648 2873 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3650 2903 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3653 2924 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3656 2906 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3659 2920 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3662 2896 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3664 2939 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3667 2988 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3670 2882 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3673 2793 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3676 2848 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3678 2862 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3681 2728 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3684 2749 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3687 2806 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3689 2810 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3692 2854 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 3695 2777 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3698 2699 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3701 2637 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3703 2605 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3706 2666 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3709 2673 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3712 2613 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3715 2553 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3717 2676 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3720 2665 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3723 2654 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3726 2643 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3728 2632 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3731 2512 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 3734 2574 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3737 2548 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3740 2623 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3742 2615 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3745 2590 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3748 2668 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3751 2726 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3754 2568 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3756 2514 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3759 2530 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3762 2578 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3765 2523 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3768 2404 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3770 2461 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3773 2449 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3776 2437 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3779 2302 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3781 2375 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 3784 2411 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 2 R F 3787 2466 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3790 2445 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3793 2327 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3795 2357 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3798 2403 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3801 2316 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3804 2306 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3807 2253 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3809 2321 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3812 2408 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3815 2326 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3818 2272 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3820 2268 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3823 2235 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3826 2289 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3829 2292 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3832 2207 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 3834 2134 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3837 2123 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3840 2228 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3843 2178 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3846 2046 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3848 2017 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 3851 2134 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3854 2148 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3857 2067 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3859 2119 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3862 2078 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3865 1972 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3868 1947 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3871 1921 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3873 1992 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3876 1967 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3879 1908 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3882 1987 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3885 2012 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3887 1863 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 3890 1829 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 3893 1883 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3896 1897 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3898 1866 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3901 1813 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3904 1793 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3907 1797 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3910 1783 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 3912 1811 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3915 1799 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 3918 1754 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3921 1737 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3924 1791 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3926 1737 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 3929 1564 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3932 1595 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3935 1730 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3937 1716 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3940 1646 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 3943 1677 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3946 1572 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3949 1500 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3951 1436 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3954 1538 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3957 1555 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3960 1476 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3963 1375 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 3965 1296 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3968 1439 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 3971 1420 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 3974 1402 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 3976 1384 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 3979 1365 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 3982 1169 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 3985 1274 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 3988 1328 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 3990 1352 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 3993 1343 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 3996 1186 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 3999 1186 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 4002 1236 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 4004 1186 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 4007 1256 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 4010 1212 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 4013 1161 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 4015 1152 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 4018 1056 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 4021 973 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 4024 939 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 4027 980 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 4029 1000 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 4032 988 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 4035 966 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 4038 945 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 4041 924 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 4043 902 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 4046 893 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 4049 895 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 4052 773 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 4055 792 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 4057 757 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 4060 758 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 4063 845 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 4066 802 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 4068 747 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 4067 700 M -1 1 R -3 0 R -3 0 R -1 -1 R F 4090 700 M 0 2 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -2 R F 5280 707 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 6 0 R 2 1 R 2 3 R 0 3 R F 5283 743 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5294 702 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -2 R 15 0 R 0 2 R F 5306 813 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5308 845 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5311 855 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5314 957 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5317 1076 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5319 1167 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 5322 1033 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5325 967 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5328 961 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5331 996 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5333 993 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5336 1049 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5339 1007 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5342 1090 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5345 1072 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5347 1036 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 5350 1042 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5353 1019 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5356 971 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5358 994 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5361 976 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5364 993 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5367 1090 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5370 1155 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5372 1098 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5375 1098 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 2 R F 5378 1114 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5381 1143 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5384 1344 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5386 1366 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5389 1418 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5392 1439 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5395 1456 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5397 1441 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5400 1449 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5403 1407 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5406 1509 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5409 1599 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5411 1525 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5414 1522 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5417 1562 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5420 1546 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5423 1625 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5425 1646 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5428 1635 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5431 1626 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5434 1723 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5436 1727 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5439 1717 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 5442 1848 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5445 1855 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 5448 1746 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5450 1717 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5453 1762 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5456 1753 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5459 1684 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5462 1731 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5464 1828 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 5467 1789 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5470 1805 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5473 1842 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5475 1829 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5478 1774 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 5481 1766 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5484 1882 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5487 1897 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5489 1911 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5492 1925 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5495 1939 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5498 1954 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5501 1968 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5503 1982 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5506 1996 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5509 2010 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5512 2024 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5515 1873 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5517 2088 M 0 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 5520 2099 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5523 2107 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5526 2046 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5528 2045 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5531 2125 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 2 R F 5534 2097 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5537 2099 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5540 2153 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5542 2244 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5545 2223 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 5548 2250 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5551 2252 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5554 2355 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5556 2375 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 5559 2223 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5562 2233 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5565 2315 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5567 2283 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5570 2202 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5573 2216 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5576 2284 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5579 2257 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5581 2329 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5584 2488 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 5587 2461 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5590 2398 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5593 2446 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5595 2378 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 5598 2334 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5601 2436 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5604 2527 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5606 2550 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5609 2579 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5612 2481 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5615 2612 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5618 2614 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5620 2505 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5623 2571 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5626 2774 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5629 2614 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5632 2552 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5634 2573 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5637 2499 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5640 2554 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5643 2695 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5645 2657 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5648 2641 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 5651 2667 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5654 2663 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5657 2603 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5659 2530 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5662 2709 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5665 2720 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5668 2731 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5671 2598 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5673 2601 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5676 2682 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5679 2721 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5682 2823 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5684 2844 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5687 2843 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5690 2918 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 5693 2898 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5696 2772 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5698 2773 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5701 2851 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5704 2810 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5707 2855 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5710 2835 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5712 2803 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5715 2809 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 5718 2884 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5721 2893 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5723 2854 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5726 2953 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 2 R F 5729 2844 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5732 2772 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5735 2838 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5737 3071 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5740 3118 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5743 3174 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5746 3219 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5749 3193 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5751 3049 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5754 3030 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 5757 3148 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5760 3163 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5762 3044 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5765 3052 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5768 3060 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5771 3052 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5774 3043 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5776 3087 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 5779 3107 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5782 3110 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5785 3116 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5788 3234 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5790 3179 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5793 3069 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5796 3141 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5799 3153 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5802 3025 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5804 3088 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5807 3156 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5810 3155 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5813 3185 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5815 3229 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5818 3226 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5821 3098 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5824 3194 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5827 3357 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5829 3288 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 5832 3132 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5835 3160 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5838 3218 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5840 3202 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5843 3395 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 5846 3350 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5849 3244 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5852 3262 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5854 3349 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 5857 3254 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5860 3366 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5863 3397 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5866 3420 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5868 3292 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5871 3257 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5874 3242 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5877 3363 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5879 3405 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 5882 3316 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 5885 3371 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5888 3434 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5891 3346 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5893 3337 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 5896 3330 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5899 3450 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5902 3521 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5905 3443 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5907 3465 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5910 3552 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5913 3550 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5916 3413 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5918 3393 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5921 3406 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5924 3387 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 5927 3439 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5930 3470 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5932 3426 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5935 3437 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 5938 3428 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5941 3391 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 5944 3461 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 5946 3677 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5949 3643 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 5952 3386 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5955 3541 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 5958 3548 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5960 3555 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5963 3488 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5966 3588 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 5969 3641 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5971 3617 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 5974 3564 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 5977 3591 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5980 3462 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 5983 3436 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 5985 3596 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 5988 3723 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 5991 3635 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 5994 3603 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 5997 3631 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 5999 3625 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6002 3589 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6005 3581 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6008 3598 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6010 3483 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6013 3645 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6016 3717 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6019 3773 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6022 3801 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6024 3730 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6027 3718 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6030 3720 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6033 3725 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6036 3678 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6038 3724 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6041 3723 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6044 3762 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6047 3833 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6049 3802 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6052 3740 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 2 R F 6055 3748 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6058 3765 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6061 3758 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6063 3836 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6066 3744 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6069 3724 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6072 3873 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6075 3874 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6077 3932 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6080 3886 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6083 3822 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6086 3893 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6088 3992 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6091 3860 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6094 3852 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6097 3854 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6100 3777 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6102 3755 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6105 3776 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 6108 3742 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6111 3804 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6114 3913 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6116 3939 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6119 3787 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6122 3872 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6125 3876 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6127 3880 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6130 3884 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 6133 3888 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 6136 3717 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6139 3880 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6141 3840 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6144 3770 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6147 3769 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6150 3866 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6153 3940 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6155 3836 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 6158 3876 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6161 4001 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6164 4086 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6166 4027 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6169 4022 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 6172 3959 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6175 3905 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6178 4026 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6180 3951 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6183 3977 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6186 4037 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6189 4051 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6192 4022 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6194 4020 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 6197 4087 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6200 4056 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6203 3944 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6205 4005 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6208 3918 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6211 3882 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6214 3968 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6217 3943 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6219 4019 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6222 4122 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6225 4021 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6228 4012 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6231 4069 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6233 4115 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6236 4082 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6239 4158 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6242 4150 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6245 4057 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6247 4091 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6250 4054 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6253 3943 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6256 4022 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6258 4058 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6261 4023 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6264 4000 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6267 4119 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6270 4165 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6272 4145 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6275 4121 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6278 4028 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6281 3938 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6284 4024 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6286 4050 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 6289 4133 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6292 4168 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6295 3977 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6297 3952 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6300 3959 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6303 4054 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 6306 4074 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6309 4244 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6311 4294 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6314 4339 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6317 4292 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6320 4156 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6323 4183 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6325 4243 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 6328 4138 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6331 4147 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6334 4161 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6336 4166 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6339 4075 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6342 4051 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6345 4165 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6348 4326 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6350 4286 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6353 4125 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6356 4196 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6359 4298 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6362 4225 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6364 4276 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6367 4260 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6370 4143 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6373 4250 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6375 4347 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6378 4353 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6381 4292 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6384 4315 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6387 4258 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6389 4275 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6392 4280 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6395 4284 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6398 4162 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6401 4169 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6403 4235 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6406 4301 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6409 4106 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6412 4127 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6414 4315 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6417 4320 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6420 4324 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6423 4328 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6426 4333 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6428 4281 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6431 4390 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6434 4345 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6437 4290 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6440 4366 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6442 4367 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6445 4337 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6448 4289 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6451 4376 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6453 4454 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6456 4359 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 6459 4295 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6462 4357 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6465 4562 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6467 4459 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6470 4273 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6473 4326 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6476 4373 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6479 4393 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6481 4452 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6484 4465 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6487 4386 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6490 4398 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6492 4333 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6495 4308 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6498 4519 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6501 4632 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6504 4608 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6506 4494 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6509 4451 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 6512 4430 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6515 4386 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6518 4475 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6520 4520 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6523 4511 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6526 4504 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6529 4528 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6532 4691 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6534 4730 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6537 4617 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6540 4465 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6543 4410 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6545 4409 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6548 4570 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 2 R F 6551 4620 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6554 4592 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6557 4602 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6559 4576 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6562 4514 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6565 4531 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6568 4475 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6571 4445 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6573 4479 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 6576 4529 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6579 4602 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6582 4591 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6584 4525 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6587 4455 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6590 4376 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6593 4367 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6596 4329 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6598 4394 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6601 4540 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6604 4586 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6607 4576 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6609 4577 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6612 4537 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 6615 4623 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6618 4652 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6621 4629 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6623 4512 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6626 4526 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6629 4576 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6632 4632 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6635 4577 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6637 4566 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6640 4527 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6643 4488 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6646 4469 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6648 4580 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6651 4582 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6654 4584 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6657 4586 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6660 4588 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6662 4508 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6665 4595 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6668 4648 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6671 4689 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6674 4703 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6676 4729 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6679 4745 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6682 4620 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6685 4627 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6688 4588 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6690 4563 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6693 4660 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6696 4677 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6699 4525 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6701 4492 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6704 4578 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6707 4514 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6710 4527 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6713 4706 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6715 4615 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6718 4527 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6721 4449 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6724 4628 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6727 4629 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6729 4631 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6732 4633 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 6735 4634 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6738 4636 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6740 4638 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6743 4639 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6746 4641 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6749 4643 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6752 4644 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6754 4646 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6757 4648 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6760 4649 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6763 4454 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6766 4528 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6768 4619 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6771 4540 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6774 4658 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6777 4660 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6779 4662 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6782 4545 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6785 4639 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6788 4804 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6791 4833 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6793 4836 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6796 4761 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 6799 4687 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6802 4763 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6805 4712 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6807 4529 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 6810 4532 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6813 4582 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6816 4748 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6818 4659 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6821 4655 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6824 4650 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6827 4643 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6830 4735 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6832 4655 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6835 4717 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6838 4769 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6841 4754 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6844 4658 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6846 4698 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6849 4776 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6852 4760 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6855 4731 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6857 4789 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 6860 4696 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 6863 4718 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6866 4793 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6869 4779 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6871 4836 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6874 4845 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6877 4746 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6880 4690 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6883 4705 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6885 4615 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6888 4549 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6891 4612 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6894 4807 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 6896 4926 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6899 4924 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 6902 4848 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6905 4870 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6908 4933 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6910 4771 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6913 4719 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 6916 4828 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6919 4835 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6922 4805 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6924 4726 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6927 4865 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 6930 4901 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 6933 4776 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6935 4776 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6938 4911 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6941 4838 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6944 4695 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6947 4750 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 6949 4811 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6952 4814 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 6955 4816 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6958 4676 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6961 4611 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 6963 4726 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6966 4768 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 6969 4818 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6972 4821 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6975 4812 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6977 4856 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 6980 4817 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 6983 4808 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 6986 4916 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 6988 4991 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 6991 4982 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 6994 4926 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 6997 4972 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7000 4838 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7002 4818 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7005 4900 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7008 4900 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7011 4949 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7014 4917 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7016 4961 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7019 5022 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7022 4895 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7025 4852 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7027 4877 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7030 4779 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7033 4860 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7036 4970 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7039 4843 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7041 4885 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7044 4885 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7047 4979 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7050 4924 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7053 4813 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7055 4804 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 7058 4817 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7061 4892 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7064 4967 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7066 4944 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7069 4942 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7072 4914 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7075 4885 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7078 4876 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7080 4771 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7083 4775 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7086 4876 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7089 4967 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 7092 4804 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7094 4759 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7097 4956 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7100 4893 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7103 4752 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7105 4738 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7108 4985 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7111 5045 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7114 4889 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7117 4812 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7119 4845 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7122 4916 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7125 4934 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7128 4890 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7131 5080 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7133 5166 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7136 5094 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7139 5076 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7142 5021 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7144 4972 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7147 4995 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 7150 4982 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7153 4971 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7156 4859 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 7158 4913 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7161 4945 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7164 5038 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7167 5030 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7170 4958 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7172 4749 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7175 4840 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7178 4963 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7181 4905 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7183 4986 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7186 4945 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 7189 4971 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7192 5027 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7195 4998 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7197 4885 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7200 4922 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7203 5003 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7206 5022 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7209 5086 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7211 5088 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7214 5089 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7217 5006 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7220 5032 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7222 4977 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7225 4975 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7228 5034 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7231 4886 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7234 4916 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7236 4935 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7239 4907 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7242 4874 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7245 4905 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7248 4928 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7250 5031 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7253 5048 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7256 5002 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7259 4998 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7262 4923 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7264 4855 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7267 4895 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7270 4800 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7273 4987 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7275 5030 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7278 4965 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7281 5148 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7284 5170 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7287 5031 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7289 5060 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7292 5093 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7295 5017 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7298 5021 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7301 5152 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7303 5169 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 7306 5130 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7309 5130 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7312 5111 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7314 4907 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7317 4795 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7320 5048 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7323 5214 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7326 5166 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7328 5146 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7331 5109 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7334 5155 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7337 5095 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 7339 4958 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7342 4949 M 0 3 R -2 2 R -3 2 R -2 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 2 1 R 3 1 R 2 3 R 0 3 R F 7345 4979 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -2 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7348 4998 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7351 4983 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7353 4974 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 7356 4984 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7359 4958 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7362 5062 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7365 5094 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7367 5161 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7370 5044 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7373 5026 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7376 5021 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7379 5012 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7381 5135 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7384 5115 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7387 4959 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7390 4976 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7392 5043 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7395 5105 M 0 3 R -2 3 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7398 5063 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7401 5107 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7404 5142 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7406 5182 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7409 5216 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7412 5145 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7415 5107 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7418 5182 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7420 5027 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7423 4932 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7426 4919 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7429 5024 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7431 4863 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7434 4908 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7437 5024 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 7440 5132 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7443 5134 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7445 5117 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7448 5119 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7451 5027 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7454 4891 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7457 5018 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7459 5165 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7462 5075 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7465 5036 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7468 4986 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7470 4942 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7473 4962 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7476 5108 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7479 5188 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7482 5153 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7484 5149 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7487 5112 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7490 4974 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7493 5081 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7496 5230 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7498 5125 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7501 5075 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7504 5105 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7507 5154 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7509 5107 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7512 5182 M 0 3 R -2 2 R -3 2 R -3 0 R -2 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7515 5177 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7518 5136 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7521 5341 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7523 5301 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7526 5116 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7529 5183 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7532 5232 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7535 5236 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7537 5128 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7540 5129 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7543 5078 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7546 5002 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7548 5045 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7551 5176 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7554 5052 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7557 5093 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7560 5014 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7562 5002 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7565 5166 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7568 5168 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7571 5170 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7574 5172 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7576 5174 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7579 5107 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7582 4981 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7585 5111 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7587 5377 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7590 5298 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 7593 5188 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7596 5218 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7599 5183 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7601 5162 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7604 5299 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7607 5245 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7610 5170 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7613 5189 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7615 5163 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7618 5155 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7621 5271 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7624 5103 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7626 5162 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7629 5354 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 7632 5380 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7635 5278 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7638 5227 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7640 5244 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7643 5357 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7646 5325 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7649 5211 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7652 5252 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7654 5306 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7657 5358 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7660 5295 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7663 5223 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7665 5175 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7668 5222 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7671 5312 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7674 5309 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7677 5241 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7679 5093 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7682 5082 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7685 5189 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7688 5296 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7691 5271 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7693 5175 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 7696 5160 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7699 5102 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7702 5454 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7705 5460 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7707 5359 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7710 5290 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 2 R F 7713 5150 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7716 5163 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7718 5244 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7721 5213 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7724 5363 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7727 5361 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7730 5220 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7732 5260 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7735 5262 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7738 5310 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7741 5280 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7744 5290 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7746 5330 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7749 5316 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7752 5270 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7755 5251 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7757 5244 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7760 5247 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7763 5318 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7766 5263 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7769 5140 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7771 5205 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7774 5359 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7777 5177 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7780 5258 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7783 5342 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7785 5381 M 0 3 R -2 2 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 3 R F 7788 5420 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7791 5373 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7794 5197 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7796 5117 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7799 5259 M 0 3 R -2 3 R -3 1 R -3 1 R -2 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 2 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7802 5329 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7805 5358 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7808 5428 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7810 5362 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7813 5259 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7816 5177 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7819 5185 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7822 5315 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7824 5362 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7827 5290 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7830 5347 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7833 5329 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7835 5296 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7838 5307 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7841 5179 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7844 5117 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7847 5123 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7849 5153 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7852 5230 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7855 5330 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7858 5340 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7861 5272 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7863 5185 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7866 5152 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7869 5081 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7872 5258 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 7874 5257 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7877 5256 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 7880 5256 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7883 5255 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7886 5254 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7888 5254 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7891 5101 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7894 5112 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7897 5030 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7900 5236 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7902 5248 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 7905 5275 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7908 5201 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7911 5271 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7913 5331 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7916 5388 M 0 3 R -2 3 R -3 1 R -2 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 2 1 R 3 2 R 2 2 R 0 3 R F 7919 5407 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7922 5296 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7925 5238 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7927 5283 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7930 5198 M 0 3 R -2 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 7933 5205 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7936 5297 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7939 5307 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7941 5280 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7944 5225 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7947 5135 M -1 3 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 2 R 1 3 R F 7950 5275 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7952 5338 M 0 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 3 R F 7955 5252 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7958 5253 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7961 5254 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 7964 5334 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7966 5290 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 7969 5145 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 7972 5211 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7975 5387 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 7978 5285 M -1 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 1 3 R F 7980 5048 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 7983 5072 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 7986 5114 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 7989 5264 M -1 2 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -2 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 7992 5290 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 7994 5274 M 0 3 R -2 2 R -3 2 R -3 1 R -2 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 2 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 7997 5393 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 8000 5343 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 8003 5372 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 8005 5377 M 0 3 R -2 3 R -2 1 R -3 1 R -3 -1 R -3 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 -1 R 3 1 R 2 2 R 2 2 R 0 3 R F 8008 5267 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 2 R 0 3 R F 8011 5183 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 8014 5210 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 8017 5168 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 8019 5232 M 0 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 0 3 R F 8022 5243 M 0 3 R -2 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 2 3 R 0 3 R F 8025 5454 M -1 2 R -1 3 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R -1 -2 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 8028 5515 M -1 3 R -2 2 R -2 2 R -3 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 8031 5460 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 8033 5409 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 3 R 0 2 R F 8036 5256 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 8039 5274 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 8042 5411 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -2 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 2 R F 8044 5427 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 0 3 R F 8047 5448 M 0 3 R -2 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 2 2 R 0 3 R F 8050 5264 M -1 3 R -1 3 R -3 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 3 2 R 1 2 R 1 3 R F 8053 5291 M -1 3 R -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 3 R 1 3 R F 8056 5229 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 1 3 R F 8058 5162 M 0 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -2 R 2 -3 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 3 R 0 2 R F 8061 5310 M 0 3 R -2 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 2 -2 R 3 0 R 3 0 R 3 2 R 2 3 R 0 3 R F 8064 5515 M -1 3 R -1 2 R -3 2 R -3 1 R -3 -1 R -2 -2 R -2 -2 R -1 -3 R 1 -3 R 2 -3 R 2 -1 R 3 -1 R 3 1 R 3 1 R 1 3 R 1 3 R F 8067 5458 M -1 3 R -2 3 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -3 R -1 -3 R 1 -3 R 1 -2 R 3 -2 R 3 0 R 3 0 R 2 2 R 2 2 R 1 3 R F 8070 5423 M -1 3 R -2 2 R -2 2 R -3 0 R -3 0 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 3 1 R 2 1 R 2 3 R 1 3 R F 8072 5382 M 0 3 R -2 3 R -3 2 R -2 0 R -3 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 3 0 R 2 0 R 3 2 R 2 2 R 0 3 R F 8074 5471 M -1 2 R -3 2 R -3 0 R -3 0 R -2 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 2 -2 R 3 0 R 3 0 R 3 2 R 1 1 R F 8074 5456 M -1 1 R -3 1 R -3 -1 R -2 -1 R -2 -3 R -1 -3 R 1 -3 R 2 -2 R 2 -2 R 3 -1 R 3 1 R 1 0 R F 8074 5304 M -1 1 R -3 -1 R -3 -2 R -1 -2 R -1 -3 R 1 -3 R 1 -3 R 3 -1 R 3 -1 R 1 0 R F 8074 5380 M -1 0 R -3 -2 R -2 -3 R 0 -3 R 0 -3 R 2 -2 R 3 -2 R 1 0 R F 8074 5372 M -1 0 R -2 -2 R 0 -3 R 0 -3 R 2 -3 R 1 -1 R F 15 setlinewidth 1275 5346 M 1 0 R 1 -1 R 2 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R D 2072 5131 M 1 -1 R 1 0 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 2 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 2 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R D 2869 4629 M 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 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8 R 1 8 R 1 8 R 1 8 R 2 7 R 1 8 R 1 8 R 1 8 R 1 8 R 1 7 R 1 8 R 1 8 R 1 7 R 1 8 R 1 8 R 1 7 R 1 8 R 1 7 R 1 8 R 1 7 R 2 8 R 1 7 R 1 8 R 1 7 R 1 8 R 1 7 R 1 7 R 1 8 R 1 7 R 1 7 R 1 8 R 1 7 R 1 7 R 1 8 R 1 7 R 1 7 R 1 7 R 2 7 R 1 7 R 1 8 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 2 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 6 R 2 7 R 1 6 R 1 7 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 6 R 1 7 R 2 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 6 R 1 6 R 1 7 R 2 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 2 6 R 1 6 R 1 5 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 5 R 1 6 R 1 6 R 1 6 R 1 5 R 1 6 R 1 6 R 1 6 R 1 5 R 2 6 R 1 6 R 1 5 R 1 6 R 1 5 R 1 6 R 1 6 R 1 5 R 1 6 R 1 5 R 1 6 R 1 5 R 1 6 R 1 5 R 1 6 R 2 5 R 1 6 R 1 5 R 1 6 R 1 5 R 1 5 R 1 6 R 1 5 R 1 6 R 1 5 R 1 5 R 1 6 R 1 5 R 1 5 R 1 5 R 1 6 R 2 5 R 1 5 R 1 5 R 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R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R D 2072 5050 M 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 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1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R D 2869 4487 M 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 2 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 2 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 2 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 2 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 2 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 2 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 2 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 2 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 2 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 2 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 2 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 2 -1 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 2 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 2 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 2 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 2 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 2 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -1 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 2 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -3 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 2 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 1 -3 R 1 -2 R 1 -2 R 1 -2 R 1 -2 R 2 -2 R 1 -2 R 1 -2 R 1 -2 R 1 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9 R 2 9 R 1 8 R 1 9 R 1 9 R 1 8 R 1 9 R 1 9 R 1 8 R 1 9 R 1 9 R 1 8 R 1 9 R 1 8 R 1 9 R 1 8 R 1 8 R 2 9 R 1 8 R 1 9 R 1 8 R 1 8 R 1 9 R 1 8 R 1 8 R 1 8 R 1 8 R 1 9 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 2 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 7 R 1 8 R 1 8 R 2 8 R 1 7 R 1 8 R 1 8 R 1 8 R 1 7 R 1 8 R 1 7 R 1 8 R 1 8 R 1 7 R 1 8 R 1 7 R 1 8 R 1 7 R 1 8 R 1 7 R 2 7 R 1 8 R 1 7 R 1 8 R 1 7 R 1 7 R 1 8 R 1 7 R 1 7 R 1 7 R 1 8 R 1 7 R 1 7 R 1 7 R 1 8 R 2 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 2 7 R 1 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 6 R 1 7 R 1 7 R 2 6 R 1 7 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 6 R 1 7 R 1 6 R 2 7 R 1 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 6 R 1 6 R 1 7 R 2 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 2 6 R 1 6 R 1 6 R 1 6 R 1 6 R 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1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R D 2072 4959 M 1 -1 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 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-1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 2 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 0 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 0 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 2 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R D 2869 4329 M 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 2 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -1 R 1 -2 R 2 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 2 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 1 -1 R 1 -2 R 1 -1 R 1 -1 R 1 -2 R 2 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8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 7 R 1 8 R 1 8 R 1 8 R 1 8 R 1 8 R 1 7 R 1 8 R 1 8 R 1 8 R 1 7 R 2 8 R 1 8 R 1 7 R 1 8 R 1 7 R 1 8 R 1 8 R 1 7 R 1 8 R 1 7 R 1 8 R 1 7 R 1 8 R 1 7 R 1 7 R 2 8 R 1 7 R 1 8 R 1 7 R 1 7 R 1 8 R 1 7 R 1 7 R 1 7 R 1 8 R 1 7 R 1 7 R 1 7 R 1 8 R 1 7 R 1 7 R 2 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 1 7 R 2 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 6 R 1 7 R 1 7 R 1 7 R 1 6 R 2 7 R 1 6 R 1 7 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 7 R 1 6 R 1 6 R 2 7 R 1 6 R 1 7 R 1 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 6 R 1 7 R 1 6 R 1 6 R 1 6 R 2 6 R 1 7 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 2 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 5 R 1 6 R 1 6 R 1 6 R 1 6 R 1 6 R 1 5 R 1 6 R 2 6 R 1 6 R 1 5 R 1 6 R 1 6 R 1 5 R 1 6 R 1 6 R 1 5 R 1 6 R 1 6 R 1 5 R 1 6 R 1 6 R 1 5 R 1 6 R 2 5 R 1 6 R 1 5 R 1 6 R 1 5 R 1 6 R 1 5 R 1 6 R 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14 R 7 14 R D 7586 6053 M -14 -7 R -14 -14 R -7 -14 R -7 -21 R 0 -35 R 7 -21 R 7 -14 R 14 -14 R 14 -7 R D 15 setlinewidth 7012 5906 M 0 -496 R D 6375 5906 M 0 -496 R D 10 setlinewidth 5851 6053 M 0 -147 R D 5858 6053 M 0 -147 R D 5830 6053 M 49 0 R D 5830 5906 M 105 0 R 0 42 R -7 -42 R D 15 setlinewidth 5312 5906 M 0 -496 R D L1 1275 5658 M 6799 0 R D %%PageTrailer end %%PageResources: font Helvetica %%Trailer %%Pages: 1 %%DocumentNeededResources: font Helvetica %%EOF f5a.eps0100644000000000000000000006650610376206774010772 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.local, /Users/martin/conv/output/50x50x82/HD3567 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Thu Oct 20 13:22:25 2005 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL 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All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 4667 1830 M 0 186 R D 4120 1463 M -30 -152 R 30 31 R 46 15 R 45 0 R 46 -15 R 30 -31 R 16 -45 R 0 -31 R -16 -45 R -30 -31 R -46 -15 R -45 0 R -46 15 R -15 15 R -15 31 R 0 15 R 15 15 R 15 -15 R -15 -15 R D 4211 1357 M 31 -15 R 30 -31 R 15 -45 R 0 -31 R -15 -45 R -30 -31 R -31 -15 R D 4120 1463 M 152 0 R D 4120 1448 M 76 0 R 76 15 R D 4470 1463 M -46 -15 R -15 -31 R 0 -45 R 15 -30 R 46 -16 R 60 0 R 46 16 R 15 30 R 0 45 R -15 31 R -46 15 R -60 0 R -31 -15 R -15 -31 R 0 -45 R 15 -30 R 31 -16 R D 4530 1326 M 31 16 R 15 30 R 0 45 R -15 31 R -31 15 R D 4470 1326 M -46 -15 R -15 -15 R -15 -30 R 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3 R -15 1 R -14 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -10 R -10 -10 R -8 -13 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 5 -13 R 6 -14 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 8 12 R 7 14 R 4 13 R 3 14 R 1 15 R F L1 2886 6458 M 14248 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f5b.eps0100644000000000000000000006302510376206774010764 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.local, /Users/martin/conv/output/50x50x82/HD3567 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Thu Oct 20 13:22:25 2005 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore 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10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F 10769 5139 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 3969 6018 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -2 -14 R -1 -15 R 1 -14 R 2 -15 R 5 -13 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 13 R 3 15 R 1 14 R F 14590 5170 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -10 10 R -13 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 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R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 5329 4414 M -1 14 R -3 15 R -5 13 R -6 13 R -8 13 R -10 10 R -11 10 R -12 8 R -13 7 R -14 4 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -10 R -9 -10 R -9 -13 R -6 -13 R -5 -13 R -2 -15 R -1 -14 R 1 -15 R 2 -14 R 5 -13 R 6 -14 R 9 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 14 R 5 13 R 3 14 R 1 15 R F L1 2886 6458 M 14248 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f6a.eps0100644000000000000000000007103010376206774010757 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 240 198 %%Title: Graphics produced by IDL %%For: pen@origo, /usr/users/pen/tracks %%Creator: IDL Version 6.1 (IRIX mipseb m64) %%CreationDate: Wed Aug 17 16:09:10 2005 %%DocumentData: Clean7bit %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 240 198 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Helvetica 423.333 /Helvetica STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 K 1275 700 M 6800 0 R D 1275 700 M 0 178 R D 1058 530 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 1198 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 1345 481 M -7 -21 R -14 -14 R -21 -7 R -7 0 R -21 7 R -14 14 R -7 21 R 0 7 R 7 21 R 14 14 R 21 7 R 7 0 R 21 -7 R 14 -14 R 7 -28 R 0 -35 R -7 -35 R -14 -21 R -21 -7 R -14 0 R -21 7 R -7 14 R D 1436 530 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 2975 700 M 0 178 R D 2758 530 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R 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R 7 -28 R 14 -14 R 21 -7 R 7 0 R 21 7 R 14 14 R 7 21 R 0 7 R -7 21 R -14 14 R -21 7 R -7 0 R -21 -7 R -14 -14 R -7 -21 R D 1275 3080 M 204 0 R D 1166 3143 M -70 0 R -7 -63 R 7 7 R 21 7 R 21 0 R 21 -7 R 14 -14 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 1275 4270 M 204 0 R D 1152 4333 M -70 -98 R 105 0 R D 1152 4333 M 0 -147 R D 1275 5460 M 204 0 R D 1096 5523 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 1275 6650 M 204 0 R D 1089 6614 M 0 7 R 7 14 R 7 7 R 14 7 R 28 0 R 14 -7 R 7 -7 R 7 -14 R 0 -14 R -7 -14 R -14 -21 R -70 -70 R 98 0 R D 1275 1295 M 102 0 R D 1275 2485 M 102 0 R D 1275 3675 M 102 0 R D 1275 4865 M 102 0 R D 1275 6055 M 102 0 R D 721 3573 M 147 0 R D 721 3573 M 147 56 R -147 56 R 147 0 R D 833 3720 M 91 35 R -91 35 R D 8075 700 M 0 5950 R D 8075 700 M -204 0 R D 8075 1890 M -204 0 R D 8075 3080 M -204 0 R D 8075 4270 M -204 0 R D 8075 5460 M -204 0 R D 8075 6650 M 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10 R 30 10 R 34 11 R 31 10 R 30 11 R 38 11 R 37 10 R 34 10 R 34 10 R 34 11 R 31 10 R 34 11 R 30 11 R 28 12 R 27 12 R 34 12 R 30 13 R 31 12 R 31 13 R 27 14 R 27 13 R 27 15 R 27 15 R 28 15 R 27 16 R 24 17 R 23 17 R 21 18 R 27 18 R 20 18 R 24 19 R 21 19 R 23 20 R 21 20 R 17 21 R 20 21 R 21 22 R 27 30 R 17 25 R 27 39 R 20 32 R 17 33 R 21 32 R 17 32 R 17 33 R 17 32 R 17 33 R 17 34 R 13 33 R 14 33 R 14 34 R 13 34 R 14 34 R 13 34 R 11 34 R 13 34 R 14 34 R 13 34 R 11 34 R 13 34 R 10 35 R 11 35 R 13 33 R 10 35 R 11 35 R 10 34 R 13 34 R 11 35 R 10 34 R 10 35 R 14 35 R 10 33 R 10 35 R 14 34 R 10 35 R D 5195 2465 M 10 4 R 4 6 R -4 7 R 0 7 R -6 10 R -14 13 R -20 19 R -21 22 R -27 21 R -20 21 R -24 21 R -27 21 R -24 21 R -24 21 R -24 20 R -24 20 R -20 22 R -24 22 R -24 22 R -23 21 R -24 22 R -21 22 R -23 22 R -24 22 R -21 21 R -23 22 R -24 22 R -21 22 R -20 23 R -20 23 R -24 22 R -21 22 R -20 23 R -20 23 R -21 23 R -20 23 R -21 22 R -17 23 R -20 24 R -20 24 R -17 22 R -17 24 R -17 25 R -21 24 R -17 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R 21 11 R 17 12 R 17 12 R 20 12 R 21 13 R 20 12 R 20 14 R 17 13 R 17 14 R 21 15 R 17 14 R 17 16 R 13 15 R 17 15 R 17 16 R 17 16 R 14 17 R 14 17 R 10 17 R 13 18 R 11 17 R 10 18 R 13 19 R 14 29 R 27 43 R 21 35 R 17 32 R 17 33 R 17 33 R 17 33 R 13 33 R 14 33 R 17 34 R 10 23 R 7 24 R 13 24 R 7 24 R 10 25 R 11 26 R 10 26 R 13 25 R 11 27 R 6 26 R 14 28 R 10 28 R 10 28 R D 4141 3198 M 4 3 R 3 6 R -3 6 R 0 6 R -4 9 R -10 11 R -17 16 R -20 21 R -24 23 R -24 22 R -20 21 R -24 21 R -24 22 R -24 21 R -24 21 R -23 21 R -21 22 R -24 22 R -23 22 R -21 22 R -24 22 R -20 22 R -24 23 R -20 22 R -24 22 R -20 22 R -21 23 R -20 23 R -21 23 R -20 22 R -20 23 R -21 24 R -20 23 R -21 23 R -20 23 R -20 23 R -21 24 R -20 23 R -17 23 R -17 24 R -21 25 R -20 24 R -17 23 R -17 24 R -20 25 R -21 24 R -20 23 R -17 23 R -17 25 R -21 24 R -17 24 R -17 24 R -17 24 R -17 25 R -20 24 R -17 25 R -17 23 R -14 25 R -17 26 R -13 24 R -14 25 R -13 26 R -14 25 R -14 26 R -10 25 R -10 26 R -14 27 R -10 26 R -10 26 R -7 27 R -7 27 R -6 27 R -4 27 R 0 27 R 0 28 R 0 26 R 7 28 R 7 26 R 10 27 R 14 26 R 17 24 R 17 25 R 17 24 R 20 23 R 24 22 R 30 21 R 31 20 R 31 20 R 34 18 R 34 18 R 37 17 R 37 16 R 38 15 R 34 15 R 34 14 R 34 14 R 41 12 R 37 12 R 41 11 R 41 11 R 37 10 R 41 10 R 30 9 R 34 9 R 38 9 R 34 9 R 37 8 R 38 8 R 34 8 R 40 8 R 38 6 R 34 7 R 30 7 R 38 6 R 34 7 R 37 7 R 38 6 R 37 6 R 34 6 R 37 6 R 38 6 R 34 6 R 34 5 R 34 6 R 37 6 R 38 5 R 37 5 R 37 5 R 38 5 R 37 4 R 31 5 R 34 4 R 30 5 R 38 4 R 34 5 R 37 4 R 38 4 R 37 4 R 37 3 R 38 4 R 30 3 R 34 4 R 31 4 R 37 3 R 34 3 R 38 3 R 37 3 R 38 3 R 37 3 R 41 2 R 24 3 R 27 3 R 30 2 R 34 2 R 34 3 R 34 2 R 34 1 R 38 2 R 37 1 R 38 1 R 34 2 R 34 1 R 34 2 R 30 1 R 34 2 R 31 1 R 34 1 R 30 1 R 31 2 R 31 1 R 37 2 R 34 1 R 31 1 R 34 2 R 27 2 R 27 2 R 27 2 R 27 2 R 24 3 R 24 3 R 24 3 R 24 4 R 27 3 R 24 4 R 23 4 R 28 5 R 23 4 R 21 6 R 24 5 R 20 6 R 20 6 R 21 6 R 20 7 R 21 7 R 17 8 R 17 7 R 17 8 R 13 9 R 17 9 R 17 9 R 17 9 R 17 9 R 14 10 R 17 10 R 13 10 R 14 11 R 17 11 R 14 11 R 13 11 R 10 11 R 14 12 R 14 12 R 10 12 R 13 12 R 11 13 R 13 12 R 10 13 R 11 13 R 10 13 R 10 14 R 7 14 R 10 13 R 7 15 R 10 14 R 7 14 R 10 14 R 7 15 R 10 15 R 10 15 R 10 14 R 14 20 R 17 34 R D 5411 6024 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -8 R 14 0 R 21 8 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 5523 5891 M -7 -7 R 7 -8 R 7 8 R -7 7 R D 5670 5975 M -7 -21 R -14 -14 R -21 -7 R -7 0 R -21 7 R -14 14 R -7 21 R 0 7 R 7 21 R 14 14 R 21 7 R 7 0 R 21 -7 R 14 -14 R 7 -28 R 0 -35 R -7 -35 R -14 -21 R -21 -8 R -14 0 R -21 8 R -7 14 R D 5839 6024 M 0 -148 R D 5839 6024 M 56 -148 R 56 148 R 0 -148 R D 6038 5916 M -13 -4 R -13 -9 R -9 -13 R -4 -13 R 0 -13 R 4 -13 R 9 -13 R 13 -9 R 13 -4 R 13 0 R 13 4 R 13 9 R 9 13 R 4 13 R 0 13 R -4 13 R -9 13 R -13 9 R -13 4 R -13 0 R D 6042 5877 M -4 -4 R 0 -5 R 4 -4 R 5 0 R 4 4 R 0 5 R -4 4 R -5 0 R D 6042 5873 M 0 -5 R 5 0 R 0 5 R -5 0 R D 5751 5488 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 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R -9 -13 R -4 -13 R 0 -13 R 4 -13 R 9 -13 R 13 -9 R 13 -4 R 13 0 R 13 4 R 13 9 R 9 13 R 4 13 R 0 13 R -4 13 R -9 13 R -13 8 R -13 5 R -13 0 R D 6722 4390 M -4 -5 R 0 -4 R 4 -4 R 5 0 R 4 4 R 0 4 R -4 5 R -5 0 R D 6722 4385 M 0 -4 R 5 0 R 0 4 R -5 0 R D 6091 2394 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 6203 2261 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 6350 2373 M -7 14 R -21 7 R -14 0 R -21 -7 R -14 -21 R -7 -35 R 0 -35 R 7 -28 R 14 -14 R 21 -7 R 7 0 R 21 7 R 14 14 R 7 21 R 0 7 R -7 21 R -14 14 R -21 7 R -7 0 R -21 -7 R -14 -14 R -7 -21 R D 6519 2394 M 0 -147 R D 6519 2394 M 56 -147 R 56 147 R 0 -147 R D 6718 2287 M -13 -5 R -13 -8 R -9 -13 R -4 -13 R 0 -13 R 4 -13 R 9 -13 R 13 -9 R 13 -4 R 13 0 R 13 4 R 13 9 R 9 13 R 4 13 R 0 13 R -4 13 R -9 13 R -13 8 R -13 5 R -13 0 R D 6722 2248 M -4 -5 R 0 -4 R 4 -4 R 5 0 R 4 4 R 0 4 R -4 5 R -5 0 R D 6722 2243 M 0 -4 R 5 0 R 0 4 R -5 0 R D L1 7844 700 M -21 15 R -23 18 R -28 19 R -27 18 R -24 17 R -27 18 R -27 19 R -24 18 R -27 17 R -24 18 R -27 18 R -27 18 R -24 17 R -27 18 R -24 17 R -27 18 R -27 18 R -24 17 R -24 18 R -27 18 R -27 18 R -24 17 R -27 18 R -24 17 R -24 18 R -27 18 R -24 17 R -27 18 R -24 17 R -27 18 R -24 18 R -24 17 R -24 18 R -27 19 R -24 18 R -23 18 R -24 18 R -27 18 R -24 18 R -24 18 R -24 18 R -24 18 R -27 18 R -24 18 R -23 18 R -21 18 R -24 20 R -23 18 R -24 19 R -24 19 R -20 18 R -24 20 R -24 18 R -24 19 R -20 18 R -24 20 R -24 19 R -24 18 R -20 19 R -20 20 R -24 20 R -21 19 R -20 20 R -24 20 R -20 19 R -21 21 R -20 19 R -20 20 R -24 20 R -21 19 R -20 21 R -20 20 R -21 19 R -20 21 R -21 21 R -20 20 R -17 20 R -17 21 R -20 22 R -17 22 R -21 20 R -17 21 R -17 22 R -17 21 R -13 15 R D 6355 1637 M 0 3 R 10 3 R 3 5 R 0 7 R -7 9 R -10 12 R -20 17 R -24 18 R -24 19 R -20 18 R -24 18 R -27 18 R -24 18 R -24 17 R -24 18 R -23 18 R -24 18 R -27 18 R -24 17 R -24 17 R -24 18 R -20 18 R -24 19 R -24 19 R -24 19 R -23 18 R -24 18 R -24 19 R -24 18 R -20 18 R -24 19 R -24 18 R -24 19 R -23 18 R -24 19 R -17 17 R -24 23 R -27 21 R -24 21 R -20 19 R -21 19 R -20 20 R -24 20 R -24 19 R -20 19 R -21 20 R -20 20 R -20 20 R -21 19 R -17 20 R -20 21 R -21 21 R -20 20 R -20 20 R -17 21 R -21 21 R -20 20 R -17 20 R -21 21 R -17 21 R -20 21 R -17 20 R -20 21 R -14 22 R -17 22 R -17 22 R -17 21 R -14 22 R -17 22 R -17 22 R -17 21 R -17 21 R -17 23 R -13 22 R -17 22 R -17 21 R -14 22 R -13 23 R -14 22 R -14 23 R -13 23 R -14 23 R -10 23 R -10 23 R -14 23 R -10 23 R -10 24 R -14 23 R -10 23 R -10 24 R -10 23 R -11 23 R -6 24 R -11 24 R -6 23 R -7 25 R -10 23 R -7 24 R -7 24 R -7 24 R -7 24 R -6 24 R -4 24 R -3 24 R -4 24 R -3 25 R 0 24 R 0 25 R 0 24 R 0 25 R 3 24 R 4 24 R 7 24 R 6 24 R 11 24 R 10 23 R 10 23 R 10 23 R 14 23 R 10 22 R 17 22 R 14 22 R 17 22 R 17 20 R 20 21 R 20 19 R 21 19 R 24 18 R 23 18 R 24 17 R 24 17 R 24 17 R 27 16 R 27 15 R 27 15 R 24 14 R 27 15 R 24 14 R 31 14 R 27 14 R 27 13 R 31 12 R 27 13 R 34 12 R 27 11 R 31 11 R 30 11 R 28 11 R 27 11 R 30 11 R 28 11 R 30 10 R 31 10 R 30 10 R 34 10 R 31 9 R 31 9 R 30 9 R 31 9 R 30 9 R 31 9 R 31 9 R 27 9 R 30 9 R 31 10 R 31 9 R 30 9 R 31 9 R 27 10 R 34 9 R 31 9 R 30 9 R 27 9 R 28 9 R 27 9 R 27 10 R 24 10 R 27 10 R 24 10 R 27 10 R 24 11 R 24 11 R 30 12 R 27 11 R 28 11 R 23 12 R 28 12 R 23 12 R 21 13 R 24 13 R 20 14 R 17 14 R 20 15 R 21 14 R 17 15 R 17 16 R 20 15 R 17 16 R 21 16 R 20 17 R 20 17 R 17 17 R 17 17 R 17 18 R 14 18 R 14 19 R 13 19 R 14 19 R 13 19 R 11 20 R 13 19 R 14 20 R 10 21 R 14 21 R 10 20 R 10 22 R 10 21 R 14 22 R 10 22 R 14 21 R 6 22 R 11 20 R 10 20 R 10 20 R 14 30 R 13 35 R 24 54 R 17 45 R 14 36 R 13 35 R 14 33 R 13 34 R 11 35 R 13 34 R 10 34 R 11 35 R 13 34 R 10 35 R 14 34 R 10 34 R 14 35 R 10 34 R 10 34 R 10 34 R 14 35 R 10 34 R 10 35 R 14 34 R 10 35 R 10 34 R 14 34 R 10 35 R D 5090 2488 M 3 1 R 4 5 R 3 6 R 0 7 R -7 8 R -10 12 R -14 15 R -23 21 R -21 19 R -24 19 R -23 18 R -24 18 R -21 19 R -20 18 R -24 19 R -20 20 R -24 18 R -20 20 R -21 19 R -24 20 R -20 19 R -20 19 R -24 19 R -21 20 R -20 19 R -24 20 R -20 19 R -21 19 R -20 19 R -20 21 R -21 21 R -20 19 R -17 20 R -21 20 R -20 21 R -20 21 R -17 19 R -21 21 R -20 21 R -17 20 R -21 21 R -17 20 R -17 22 R -20 21 R -17 21 R -17 20 R -17 22 R -20 22 R -17 21 R -17 20 R -17 22 R -21 22 R -17 21 R -13 21 R -17 22 R -17 23 R -17 21 R -14 22 R -17 23 R -14 22 R -17 22 R -13 22 R -17 23 R -14 22 R -17 22 R -13 22 R -14 23 R -14 23 R -17 22 R -13 22 R -10 23 R -14 24 R -14 23 R -13 22 R -10 23 R -14 24 R -10 23 R -10 24 R -11 23 R -10 23 R -10 24 R -10 24 R -7 23 R -10 24 R -7 24 R -7 24 R -7 24 R -6 24 R -4 25 R -3 24 R -4 25 R -3 24 R -3 25 R 0 25 R 3 24 R 3 25 R 4 24 R 3 24 R 7 24 R 10 24 R 7 24 R 14 23 R 10 23 R 17 22 R 13 22 R 21 21 R 17 21 R 20 19 R 24 19 R 24 19 R 24 17 R 23 17 R 28 17 R 23 15 R 28 15 R 27 15 R 27 16 R 27 14 R 31 14 R 27 13 R 31 13 R 30 12 R 31 12 R 30 11 R 31 10 R 31 10 R 30 10 R 27 10 R 31 10 R 31 10 R 30 10 R 34 10 R 31 9 R 30 9 R 34 8 R 31 8 R 34 8 R 27 7 R 27 8 R 31 8 R 34 7 R 31 8 R 34 7 R 30 7 R 34 7 R 34 7 R 31 6 R 34 6 R 27 7 R 27 6 R 31 6 R 34 7 R 30 6 R 34 6 R 34 6 R 34 6 R 31 5 R 34 5 R 34 5 R 24 5 R 24 5 R 27 5 R 30 5 R 28 5 R 30 5 R 31 4 R 34 5 R 30 4 R 34 4 R 34 4 R 31 5 R 31 4 R 30 4 R 31 4 R 27 4 R 27 5 R 31 4 R 27 4 R 27 5 R 27 5 R 24 4 R 24 5 R 31 5 R 27 4 R 27 6 R 31 4 R 27 6 R 27 5 R 27 5 R 27 6 R 24 6 R 24 6 R 27 6 R 24 7 R 24 7 R 27 7 R 24 7 R 27 8 R 24 7 R 20 9 R 21 8 R 20 9 R 20 9 R 21 10 R 17 9 R 17 10 R 20 11 R 17 10 R 17 11 R 17 11 R 14 12 R 17 11 R 17 12 R 20 12 R 17 12 R 14 13 R 17 13 R 17 13 R 13 13 R 11 14 R 13 14 R 10 14 R 14 15 R 10 14 R 10 15 R 14 15 R 10 15 R 10 15 R 11 16 R 10 15 R 10 16 R 10 16 R 10 16 R 11 17 R 6 16 R 11 18 R 30 51 R 21 42 R 17 35 R 17 33 R 13 34 R 17 33 R 14 33 R 17 33 R 13 34 R 14 33 R 14 34 R 13 34 R 14 34 R 10 34 R 14 34 R 13 34 R 14 34 R 10 34 R 14 35 R D 4009 3221 M 0 4 R 3 5 R 0 5 R -3 7 R -7 9 R -7 11 R -17 16 R -20 18 R -24 19 R -21 19 R -23 19 R -21 19 R -24 18 R -20 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30 6 R 28 6 R 30 6 R 34 5 R 34 6 R 34 6 R 34 5 R 34 5 R 31 5 R 34 5 R 34 5 R 30 4 R 28 5 R 30 5 R 31 5 R 34 4 R 34 5 R 34 5 R 34 4 R 34 5 R 34 4 R 34 4 R 27 4 R 31 4 R 30 4 R 34 4 R 31 4 R 34 4 R 34 4 R 34 4 R 34 4 R 34 3 R 30 4 R 28 4 R 30 3 R 31 4 R 30 3 R 34 4 R 34 3 R 34 4 R 34 3 R 34 3 R 34 3 R 28 3 R 27 3 R 30 3 R 31 3 R 31 3 R 30 3 R 34 2 R 34 3 R 34 3 R 34 2 R 34 2 R 24 3 R 27 2 R 27 3 R 28 2 R 30 2 R 31 2 R 30 2 R 34 2 R 31 2 R 34 2 R 34 1 R 31 2 R 30 1 R 31 2 R 30 2 R 31 1 R 27 2 R 31 2 R 27 1 R 27 2 R 24 2 R 24 1 R 27 2 R 27 2 R 27 2 R 28 2 R 23 2 R 28 2 R 27 2 R 24 2 R 23 3 R 24 2 R 24 3 R 24 3 R 20 3 R 24 4 R 20 4 R 24 3 R 24 4 R 24 4 R 20 5 R 24 4 R 17 5 R 20 6 R 17 5 R 17 6 R 17 6 R 14 6 R 17 6 R 14 7 R 17 7 R 13 7 R 14 8 R 13 7 R 14 8 R 10 8 R 14 8 R 17 8 R 13 9 R 14 8 R 14 9 R 13 9 R 10 9 R 14 10 R 14 9 R 10 10 R 10 10 R 14 10 R 10 10 R 7 10 R 10 11 R 7 11 R 10 10 R 10 14 R 31 41 R 23 33 R 21 31 R 20 32 R D L0 1615 1890 M 680 0 R D L1 1615 1533 M 680 0 R D L0 2656 2065 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-6 -30 R 6 -29 R 17 -26 R 25 -16 R 30 -6 R 29 6 R 26 16 R 16 26 R 6 29 R D 4780 4627 M -6 30 R -17 25 R -25 17 R -30 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -30 R 17 -25 R 25 -17 R 30 -6 R 30 6 R 25 17 R 17 25 R 6 30 R D 4900 4603 M -6 30 R -17 25 R -25 17 R -30 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -30 R 17 -25 R 25 -17 R 30 -5 R 30 5 R 25 17 R 17 25 R 6 30 R D 4940 4734 M -6 30 R -17 25 R -25 17 R -30 6 R -29 -6 R -26 -17 R -16 -25 R -6 -30 R 6 -30 R 16 -25 R 26 -17 R 29 -6 R 30 6 R 25 17 R 17 25 R 6 30 R D 4561 4401 M -6 30 R -17 25 R -25 17 R -30 6 R -29 -6 R -26 -17 R -16 -25 R -6 -30 R 6 -30 R 16 -25 R 26 -17 R 29 -6 R 30 6 R 25 17 R 17 25 R 6 30 R D 4855 4353 M -6 30 R -17 25 R -25 17 R -30 6 R -29 -6 R -26 -17 R -16 -25 R -6 -30 R 6 -29 R 16 -26 R 26 -16 R 29 -6 R 30 6 R 25 16 R 17 26 R 6 29 R D 4749 4948 M -6 30 R -16 25 R -26 17 R -29 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -29 R 17 -26 R 25 -16 R 30 -6 R 29 6 R 26 16 R 16 26 R 6 29 R D 4959 4199 M -6 29 R -17 26 R -25 16 R -30 6 R -29 -6 R -26 -16 R -16 -26 R -6 -29 R 6 -30 R 16 -25 R 26 -17 R 29 -6 R 30 6 R 25 17 R 17 25 R 6 30 R D 4566 3842 M -6 29 R -17 26 R -25 16 R -30 6 R -30 -6 R -25 -16 R -17 -26 R -6 -29 R 6 -30 R 17 -25 R 25 -17 R 30 -6 R 30 6 R 25 17 R 17 25 R 6 30 R D 4907 3604 M -6 29 R -17 26 R -25 16 R -30 6 R -29 -6 R -26 -16 R -17 -26 R -5 -29 R 5 -30 R 17 -25 R 26 -17 R 29 -6 R 30 6 R 25 17 R 17 25 R 6 30 R D 4959 3770 M -6 30 R -17 25 R -25 17 R -30 6 R -29 -6 R -26 -17 R -16 -25 R -6 -30 R 6 -30 R 16 -25 R 26 -17 R 29 -6 R 30 6 R 25 17 R 17 25 R 6 30 R D 4543 4151 M -6 30 R -17 25 R -25 17 R -30 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -30 R 17 -25 R 25 -17 R 30 -6 R 30 6 R 25 17 R 17 25 R 6 30 R D 5520 5044 M -6 29 R -17 25 R -25 17 R -30 6 R -29 -6 R -25 -17 R -17 -25 R -6 -29 R 6 -30 R 17 -25 R 25 -17 R 29 -6 R 30 6 R 25 17 R 17 25 R 6 30 R F 4780 4627 M -6 30 R -17 25 R -25 17 R -30 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -30 R 17 -25 R 25 -17 R 30 -6 R 30 6 R 25 17 R 17 25 R 6 30 R F 4900 4603 M -6 30 R -17 25 R -25 17 R -30 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -30 R 17 -25 R 25 -17 R 30 -5 R 30 5 R 25 17 R 17 25 R 6 30 R F 4959 4199 M -6 29 R -17 26 R -25 16 R -30 6 R -29 -6 R -26 -16 R -16 -26 R -6 -29 R 6 -30 R 16 -25 R 26 -17 R 29 -6 R 30 6 R 25 17 R 17 25 R 6 30 R F 4959 3770 M -6 30 R -17 25 R -25 17 R -30 6 R -29 -6 R -26 -17 R -16 -25 R -6 -30 R 6 -30 R 16 -25 R 26 -17 R 29 -6 R 30 6 R 25 17 R 17 25 R 6 30 R F 4543 4151 M -6 30 R -17 25 R -25 17 R -30 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -30 R 17 -25 R 25 -17 R 30 -6 R 30 6 R 25 17 R 17 25 R 6 30 R F %%PageTrailer end %%PageResources: font Helvetica %%Trailer %%Pages: 1 %%DocumentNeededResources: font Helvetica %%EOF f6b.eps0100644000000000000000000006111010376206774010756 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 240 198 %%Title: Graphics produced by IDL %%For: pen@origo, /usr/users/pen/tracks %%Creator: IDL Version 6.1 (IRIX mipseb m64) %%CreationDate: Wed Aug 17 16:09:21 2005 %%DocumentData: Clean7bit %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 240 198 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Helvetica 423.333 /Helvetica STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 K 1275 700 M 6800 0 R D 1275 700 M 0 178 R D 1058 530 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 1198 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 1345 481 M -7 -21 R -14 -14 R -21 -7 R -7 0 R -21 7 R -14 14 R -7 21 R 0 7 R 7 21 R 14 14 R 21 7 R 7 0 R 21 -7 R 14 -14 R 7 -28 R 0 -35 R -7 -35 R -14 -21 R -21 -7 R -14 0 R -21 7 R -7 14 R D 1436 530 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 2975 700 M 0 178 R D 2758 530 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 2898 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 2989 530 M -21 -7 R -7 -14 R 0 -14 R 7 -14 R 14 -7 R 28 -7 R 21 -7 R 14 -14 R 7 -14 R 0 -21 R -7 -14 R -7 -7 R -21 -7 R -28 0 R -21 7 R -7 7 R -7 14 R 0 21 R 7 14 R 14 14 R 21 7 R 28 7 R 14 7 R 7 14 R 0 14 R -7 14 R -21 7 R -28 0 R D 3178 530 M -70 0 R -7 -63 R 7 7 R 21 7 R 21 0 R 21 -7 R 14 -14 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 4675 700 M 0 178 R D 4458 530 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 4598 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 4689 530 M -21 -7 R -7 -14 R 0 -14 R 7 -14 R 14 -7 R 28 -7 R 21 -7 R 14 -14 R 7 -14 R 0 -21 R -7 -14 R -7 -7 R -21 -7 R -28 0 R -21 7 R -7 7 R -7 14 R 0 21 R 7 14 R 14 14 R 21 7 R 28 7 R 14 7 R 7 14 R 0 14 R -7 14 R -21 7 R -28 0 R D 4836 530 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 6375 700 M 0 178 R D 6158 530 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 6298 397 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 6452 530 M -70 -147 R D 6354 530 M 98 0 R D 6578 530 M -70 0 R -7 -63 R 7 7 R 21 7 R 21 0 R 21 -7 R 14 -14 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 1615 700 M 0 89 R D 1955 700 M 0 89 R D 2295 700 M 0 89 R D 2635 700 M 0 89 R D 3315 700 M 0 89 R D 3655 700 M 0 89 R D 3995 700 M 0 89 R D 4335 700 M 0 89 R D 5015 700 M 0 89 R D 5355 700 M 0 89 R D 5695 700 M 0 89 R D 6035 700 M 0 89 R D 6715 700 M 0 89 R D 7055 700 M 0 89 R D 7395 700 M 0 89 R D 7735 700 M 0 89 R D 4331 256 M 0 -147 R D 4416 207 M -14 -7 R -14 -14 R -7 -21 R 0 -14 R 7 -21 R 14 -14 R 14 -7 R 21 0 R 14 7 R 14 14 R 7 21 R 0 14 R -7 21 R -14 14 R -14 7 R -21 0 R D 4598 207 M 0 -119 R -7 -21 R -7 -7 R -14 -7 R -21 0 R -14 7 R D 4598 186 M -14 14 R -14 7 R -21 0 R -14 -7 R -14 -14 R -7 -21 R 0 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R 7 -28 R 14 -14 R 21 -7 R 7 0 R 21 7 R 14 14 R 7 21 R 0 7 R -7 21 R -14 14 R -21 7 R -7 0 R -21 -7 R -14 -14 R -7 -21 R D 1275 3080 M 204 0 R D 1166 3143 M -70 0 R -7 -63 R 7 7 R 21 7 R 21 0 R 21 -7 R 14 -14 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 1275 4270 M 204 0 R D 1152 4333 M -70 -98 R 105 0 R D 1152 4333 M 0 -147 R D 1275 5460 M 204 0 R D 1096 5523 M 77 0 R -42 -56 R 21 0 R 14 -7 R 7 -7 R 7 -21 R 0 -14 R -7 -21 R -14 -14 R -21 -7 R -21 0 R -21 7 R -7 7 R -7 14 R D 1275 6650 M 204 0 R D 1089 6614 M 0 7 R 7 14 R 7 7 R 14 7 R 28 0 R 14 -7 R 7 -7 R 7 -14 R 0 -14 R -7 -14 R -14 -21 R -70 -70 R 98 0 R D 1275 1295 M 102 0 R D 1275 2485 M 102 0 R D 1275 3675 M 102 0 R D 1275 4865 M 102 0 R D 1275 6055 M 102 0 R D 721 3573 M 147 0 R D 721 3573 M 147 56 R -147 56 R 147 0 R D 833 3720 M 91 35 R -91 35 R D 8075 700 M 0 5950 R D 8075 700 M -204 0 R D 8075 1890 M -204 0 R D 8075 3080 M -204 0 R D 8075 4270 M -204 0 R D 8075 5460 M -204 0 R D 8075 6650 M 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R 20 13 R 24 13 R 20 13 R 21 14 R 20 14 R 20 15 R 21 15 R 20 15 R 17 15 R 17 16 R 17 17 R 14 17 R 13 18 R 17 17 R 11 19 R 13 18 R 14 19 R 10 18 R 14 19 R 13 18 R 14 18 R 10 19 R 14 19 R 10 19 R 10 19 R 10 19 R 10 19 R 7 20 R 10 20 R 7 20 R 7 20 R 10 20 R 7 20 R 7 21 R 10 24 R 17 55 R 14 45 R 13 37 R 10 33 R 11 34 R D 5838 2301 M 10 4 R 3 5 R -3 6 R -3 8 R -7 10 R -14 14 R -17 18 R -20 17 R -21 18 R -20 17 R -17 17 R -20 17 R -21 17 R -20 18 R -17 17 R -21 18 R -20 17 R -20 17 R -17 18 R -21 17 R -17 18 R -20 17 R -17 18 R -17 19 R -17 18 R -21 19 R -17 18 R -17 17 R -17 19 R -17 19 R -17 18 R -17 19 R -17 18 R -17 19 R -17 19 R -17 18 R -17 18 R -13 19 R -14 20 R -13 20 R -17 20 R -14 19 R -10 19 R -14 21 R -13 20 R -14 20 R -14 19 R -13 21 R -10 20 R -14 21 R -14 20 R -10 19 R -13 21 R -14 20 R -10 20 R -10 21 R -11 22 R -10 21 R -13 20 R -11 19 R -6 22 R -14 21 R -10 21 R -10 21 R -7 20 R -10 22 R -7 21 R -10 21 R -7 21 R -7 21 R -7 22 R -7 21 R -3 21 R -7 22 R -3 21 R -4 22 R 0 22 R 0 22 R 0 22 R 0 22 R 0 22 R 0 21 R 0 22 R 4 22 R 0 22 R 3 22 R 4 22 R 6 21 R 7 21 R 7 21 R 7 21 R 10 21 R 10 20 R 14 21 R 13 19 R 14 20 R 14 19 R 17 18 R 17 18 R 20 17 R 17 17 R 17 18 R 20 17 R 17 17 R 24 16 R 21 15 R 23 15 R 24 14 R 24 13 R 24 13 R 27 12 R 24 12 R 27 11 R 27 11 R 27 10 R 24 9 R 27 10 R 28 10 R 30 9 R 27 8 R 28 9 R 30 8 R 27 7 R 28 8 R 30 7 R 27 6 R 31 7 R 34 6 R 34 6 R 31 5 R 30 5 R 27 5 R 28 5 R 27 5 R 27 5 R 31 4 R 27 5 R 30 4 R 31 5 R 34 4 R 31 4 R 30 3 R 31 4 R 30 3 R 28 3 R 30 4 R 31 4 R 30 3 R 28 4 R 30 4 R 34 4 R 31 3 R 30 4 R 28 3 R 30 5 R 27 4 R 31 4 R 27 5 R 27 5 R 28 5 R 27 6 R 30 6 R 28 5 R 27 6 R 27 6 R 27 8 R 27 6 R 24 8 R 21 8 R 23 9 R 21 9 R 20 9 R 21 10 R 20 10 R 20 11 R 21 11 R 20 12 R 21 11 R 20 12 R 20 13 R 21 13 R 17 13 R 17 14 R 20 14 R 17 14 R 14 15 R 13 16 R 14 16 R 14 16 R 13 17 R 14 17 R 10 18 R 14 18 R 13 18 R 10 18 R 14 19 R 10 19 R 10 19 R 14 19 R 10 19 R 10 19 R 11 19 R 10 19 R 7 19 R 6 18 R 11 18 R 6 18 R 7 17 R 7 18 R 7 17 R 7 16 R 6 17 R 7 17 R 7 16 R 7 16 R 7 15 R 6 17 R D 4825 3042 M 3 4 R 3 4 R 0 6 R 0 7 R -6 8 R -7 12 R -14 16 R -17 19 R -13 19 R -17 18 R -17 19 R -17 19 R -17 19 R -17 18 R -14 19 R -17 19 R -20 20 R -17 18 R -17 18 R -14 19 R -17 19 R -17 19 R -17 19 R -14 18 R -13 20 R -17 20 R -14 19 R -13 19 R -14 20 R -14 20 R -13 20 R -14 20 R -13 20 R -14 20 R -10 20 R -14 20 R -13 20 R -11 21 R -13 20 R -10 20 R -11 21 R -13 21 R -10 20 R -11 21 R -10 21 R -13 20 R -11 21 R -10 21 R -10 21 R -10 20 R -7 22 R -10 21 R -7 21 R -10 21 R -7 22 R -7 21 R -7 21 R -3 22 R -7 21 R -3 22 R -4 21 R -3 22 R 0 22 R 0 22 R 0 22 R 3 23 R 0 21 R 4 22 R 3 23 R 0 21 R 4 22 R 6 22 R 4 21 R 7 22 R 6 21 R 11 21 R 10 21 R 10 20 R 10 21 R 14 19 R 13 20 R 14 19 R 17 19 R 17 18 R 17 18 R 20 18 R 21 16 R 17 17 R 20 16 R 21 16 R 23 16 R 21 15 R 24 15 R 23 14 R 28 13 R 23 13 R 28 12 R 23 12 R 28 11 R 27 11 R 27 10 R 24 10 R 24 10 R 27 10 R 30 10 R 28 9 R 27 9 R 30 8 R 28 8 R 30 7 R 27 7 R 31 7 R 31 6 R 27 6 R 24 6 R 27 6 R 30 6 R 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7 R 7 21 R 14 14 R 21 7 R 7 0 R 21 -7 R 14 -14 R 7 -28 R 0 -35 R -7 -35 R -14 -21 R -21 -7 R -14 0 R -21 7 R -7 14 R D 6519 5488 M 0 -147 R D 6519 5488 M 56 -147 R 56 147 R 0 -147 R D 6718 5381 M -13 -5 R -13 -8 R -9 -13 R -4 -13 R 0 -13 R 4 -13 R 9 -13 R 13 -9 R 13 -4 R 13 0 R 13 4 R 13 9 R 9 13 R 4 13 R 0 13 R -4 13 R -9 13 R -13 8 R -13 5 R -13 0 R D 6722 5342 M -4 -5 R 0 -4 R 4 -4 R 5 0 R 4 4 R 0 4 R -4 5 R -5 0 R D 6722 5337 M 0 -4 R 5 0 R 0 4 R -5 0 R D 6261 4893 M -21 -7 R -14 -21 R -7 -35 R 0 -21 R 7 -35 R 14 -21 R 21 -7 R 14 0 R 21 7 R 14 21 R 7 35 R 0 21 R -7 35 R -14 21 R -21 7 R -14 0 R D 6373 4760 M -7 -7 R 7 -7 R 7 7 R -7 7 R D 6464 4893 M -21 -7 R -7 -14 R 0 -14 R 7 -14 R 14 -7 R 28 -7 R 21 -7 R 14 -14 R 7 -14 R 0 -21 R -7 -14 R -7 -7 R -21 -7 R -28 0 R -21 7 R -7 7 R -7 14 R 0 21 R 7 14 R 14 14 R 21 7 R 28 7 R 14 7 R 7 14 R 0 14 R -7 14 R -21 7 R -28 0 R D 6689 4893 M 0 -147 R D 6689 4893 M 56 -147 R 56 147 R 0 -147 R D 6888 4786 M -13 -5 R -13 -8 R -9 -13 R -4 -13 R 0 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-6 30 R -17 25 R -25 17 R -29 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -30 R 17 -25 R 25 -17 R 30 -6 R 29 6 R 25 17 R 17 25 R 6 30 R D 5344 3949 M -6 29 R -17 26 R -25 16 R -30 6 R -30 -6 R -25 -16 R -17 -26 R -6 -29 R 6 -30 R 17 -25 R 25 -17 R 30 -6 R 30 6 R 25 17 R 17 25 R 6 30 R F 5731 3270 M -6 30 R -17 25 R -25 17 R -29 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -29 R 17 -26 R 25 -16 R 30 -6 R 29 6 R 25 16 R 17 26 R 6 29 R F 5751 4365 M -6 30 R -17 25 R -25 17 R -29 6 R -30 -6 R -25 -17 R -17 -25 R -6 -30 R 6 -30 R 17 -25 R 25 -17 R 30 -6 R 29 6 R 25 17 R 17 25 R 6 30 R F %%PageTrailer end %%PageResources: font Helvetica %%Trailer %%Pages: 1 %%DocumentNeededResources: font Helvetica %%EOF f7a.eps0100644000000000000000000005725710376206774010777 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.local, /Users/martin/conv/output/50x50x82/HD3567 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Thu Oct 20 13:22:21 2005 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2220 1408 M 15114 0 R D 4109 1408 M 0 198 R D 3689 1125 M -24 -116 R 24 23 R 35 12 R 35 0 R 35 -12 R 23 -23 R 12 -35 R 0 -24 R -12 -35 R -23 -23 R -35 -12 R -35 0 R -35 12 R -12 11 R -12 24 R 0 11 R 12 12 R 12 -12 R -12 -11 R D 3759 1044 M 23 -12 R 24 -23 R 11 -35 R 0 -24 R -11 -35 R -24 -23 R -23 -12 R D 3689 1125 M 117 0 R D 3689 1114 M 58 0 R 59 11 R D 3957 1125 M -35 -11 R -11 -24 R 0 -35 R 11 -23 R 35 -12 R 47 0 R 35 12 R 12 23 R 0 35 R -12 24 R -35 11 R -47 0 R -23 -11 R -12 -24 R 0 -35 R 12 -23 R 23 -12 R D 4004 1020 M 24 12 R 11 23 R 0 35 R -11 24 R -24 11 R D 3957 1020 M -35 -11 R -11 -12 R -12 -23 R 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0 -198 R D 11666 11296 M 0 -198 R D 15445 11296 M 0 -198 R D 2220 11296 M 0 -99 R D 3165 11296 M 0 -99 R D 5054 11296 M 0 -99 R D 5999 11296 M 0 -99 R D 6943 11296 M 0 -99 R D 8832 11296 M 0 -99 R D 9777 11296 M 0 -99 R D 10722 11296 M 0 -99 R D 12611 11296 M 0 -99 R D 13556 11296 M 0 -99 R D 14500 11296 M 0 -99 R D 16389 11296 M 0 -99 R D 17334 11296 M 0 -99 R D 2220 1408 M 0 9888 R D 2220 1408 M 302 0 R D 1256 1513 M 210 0 R D 1618 1653 M -35 -11 R -23 -35 R -12 -59 R 0 -35 R 12 -58 R 23 -35 R 35 -12 R 24 0 R 35 12 R 23 35 R 12 58 R 0 35 R -12 59 R -23 35 R -35 11 R -24 0 R -23 -11 R -12 -12 R -11 -23 R -12 -59 R 0 -35 R 12 -58 R 11 -24 R 12 -11 R 23 -12 R D 1642 1408 M 23 12 R 12 11 R 11 24 R 12 58 R 0 35 R -12 59 R -11 23 R -12 12 R -23 11 R D 1805 1431 M -11 -11 R 11 -12 R 12 12 R -12 11 R D 1910 1607 M 12 -12 R -12 -12 R -11 12 R 0 12 R 11 23 R 12 12 R 35 11 R 47 0 R 35 -11 R 12 -12 R 11 -23 R 0 -24 R -11 -23 R -35 -23 R -59 -24 R -23 -11 R -24 -24 R -11 -35 R 0 -35 R D 2004 1653 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59 R -11 23 R -12 12 R -23 12 R D 1805 6235 M -11 -12 R 11 -12 R 12 12 R -12 12 R D 1969 6457 M -35 -12 R -24 -35 R -11 -59 R 0 -35 R 11 -58 R 24 -35 R 35 -12 R 23 0 R 35 12 R 24 35 R 11 58 R 0 35 R -11 59 R -24 35 R -35 12 R -23 0 R -23 -12 R -12 -12 R -12 -23 R -12 -59 R 0 -35 R 12 -58 R 12 -23 R 12 -12 R 23 -12 R D 1992 6211 M 24 12 R 11 12 R 12 23 R 12 58 R 0 35 R -12 59 R -12 23 R -11 12 R -24 12 R D 2220 8824 M 302 0 R D 1618 8929 M -35 -12 R -23 -35 R -12 -59 R 0 -35 R 12 -58 R 23 -35 R 35 -12 R 24 0 R 35 12 R 23 35 R 12 58 R 0 35 R -12 59 R -23 35 R -35 12 R -24 0 R -23 -12 R -12 -12 R -11 -23 R -12 -59 R 0 -35 R 12 -58 R 11 -23 R 12 -12 R 23 -12 R D 1642 8683 M 23 12 R 12 12 R 11 23 R 12 58 R 0 35 R -12 59 R -11 23 R -12 12 R -23 12 R D 1805 8707 M -11 -12 R 11 -12 R 12 12 R -12 12 R D 1934 8882 M 23 12 R 35 35 R 0 -246 R D 1981 8917 M 0 -234 R D 1934 8683 M 105 0 R D 2220 11296 M 302 0 R D 1618 11295 M -35 -12 R -23 -35 R -12 -58 R 0 -35 R 12 -59 R 23 -35 R 35 -11 R 24 0 R 35 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6638 M 386 -210 R D 643 6720 M 245 0 R D 643 6732 M 245 0 R D 643 6872 M 245 0 R D 643 6884 M 245 0 R D 643 6685 M 0 82 R D 643 6837 M 0 82 R D 760 6732 M 0 140 R D 888 6685 M 0 82 R D 888 6837 M 0 82 R D 596 7047 M 386 0 R D 596 7059 M 386 0 R D 596 6977 M 0 82 R D 982 6977 M 0 82 R D 17334 1408 M 0 9888 R D 17334 1408 M -302 0 R D 17334 3880 M -302 0 R D 17334 6352 M -302 0 R D 17334 8824 M -302 0 R D 17334 11296 M -302 0 R D 17334 1655 M -151 0 R D 17334 1902 M -151 0 R D 17334 2150 M -151 0 R D 17334 2397 M -151 0 R D 17334 2644 M -151 0 R D 17334 2891 M -151 0 R D 17334 3138 M -151 0 R D 17334 3386 M -151 0 R D 17334 3633 M -151 0 R D 17334 4127 M -151 0 R D 17334 4374 M -151 0 R D 17334 4622 M -151 0 R D 17334 4869 M -151 0 R D 17334 5116 M -151 0 R D 17334 5363 M -151 0 R D 17334 5610 M -151 0 R D 17334 5858 M -151 0 R D 17334 6105 M -151 0 R D 17334 6599 M -151 0 R D 17334 6846 M -151 0 R D 17334 7094 M -151 0 R D 17334 7341 M -151 0 R D 17334 7588 M -151 0 R D 17334 7835 M -151 0 R D 17334 8082 M -151 0 R D 17334 8330 M -151 0 R D 17334 8577 M -151 0 R D 17334 9071 M -151 0 R D 17334 9318 M -151 0 R D 17334 9566 M -151 0 R D 17334 9813 M -151 0 R D 17334 10060 M -151 0 R D 17334 10307 M -151 0 R D 17334 10554 M -151 0 R D 17334 10802 M -151 0 R D 17334 11049 M -151 0 R D 8490 9071 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -13 -8 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 13 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R F 7621 6599 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -13 8 R -13 7 R -13 4 R -15 3 R -14 1 R -14 -1 R -15 -3 R -13 -4 R -14 -7 R -12 -8 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 12 -8 R 14 -6 R 13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R F 6790 9566 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 14 2 R 14 5 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 9170 6105 M -1 14 R -3 15 R -4 13 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 13 -4 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 15 R F 6204 7835 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -15 -3 R -13 -4 R -13 -7 R -13 -8 R -10 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 10 -10 R 13 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R F 3332 8577 M -1 14 R -2 15 R -5 13 R -6 13 R -9 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 4 R 13 7 R 12 8 R 11 9 R 9 11 R 9 12 R 6 13 R 5 14 R 2 14 R 1 15 R F 7810 7341 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 11399 7588 M 0 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -14 4 R -14 3 R -15 1 R -14 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -15 R 5 -13 R 6 -13 R 8 -13 R 10 -10 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 10 R 8 13 R 6 13 R 5 13 R 3 15 R 0 14 R F 9945 8082 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -14 0 R -15 0 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F 14328 7341 M -1 14 R -3 15 R -5 13 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 13629 7835 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -13 4 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F 12665 8082 M -1 15 R -2 14 R -5 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 0 R -14 0 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 5 14 R 2 14 R 1 14 R F 7999 8330 M -1 14 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 10 R -12 8 R -13 6 R -13 5 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -5 R -13 -6 R -12 -8 R -11 -10 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -14 R 1 -15 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -5 R 14 -2 R 15 -1 R 14 1 R 15 2 R 13 5 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 15 R F 11456 6846 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 10 R -12 8 R -13 6 R -14 5 R -14 3 R -15 0 R -14 0 R -15 -3 R -13 -5 R -13 -6 R -12 -8 R -11 -10 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R F 12344 8082 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 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m32) %%CreationDate: Thu Oct 20 13:22:22 2005 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2220 1408 M 15114 0 R D 2907 1408 M 0 198 R D 2498 985 M 210 0 R D 2802 1079 M 12 -12 R -12 -12 R -12 12 R 0 12 R 12 23 R 12 12 R 35 11 R 46 0 R 35 -11 R 12 -24 R 0 -35 R -12 -23 R -35 -12 R -35 0 R D 2895 1125 M 24 -11 R 11 -24 R 0 -35 R -11 -23 R -24 -12 R 24 -11 R 23 -24 R 12 -23 R 0 -35 R -12 -24 R -12 -11 R -35 -12 R -46 0 R -35 12 R -12 11 R -12 24 R 0 11 R 12 12 R 12 -12 R -12 -11 R D 2930 997 M 12 -35 R 0 -35 R -12 -24 R -11 -11 R -24 -12 R D 3047 903 M -11 -11 R 11 -12 R 12 12 R -12 11 R D 3211 1125 M -35 -11 R -24 -35 R -11 -59 R 0 -35 R 11 -58 R 24 -35 R 35 -12 R 23 0 R 35 12 R 24 35 R 11 58 R 0 35 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%%BoundingBox: 0 0 510 340 %%Title: Graphics produced by IDL %%For: martin@macmartin.local, /Users/martin/conv/output/50x50x82/HD3567 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Thu Oct 20 13:24:30 2005 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 340 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 2886 1830 M 14248 0 R D 2886 1830 M 0 186 R D 2856 1463 M -46 -15 R -30 -46 R -15 -76 R 0 -45 R 15 -76 R 30 -46 R 46 -15 R 30 0 R 46 15 R 30 46 R 15 76 R 0 45 R -15 76 R -30 46 R -46 15 R -30 0 R -31 -15 R -15 -15 R -15 -31 R -15 -76 R 0 -45 R 15 -76 R 15 -31 R 15 -15 R 31 -15 R D 2886 1144 M 30 15 R 16 15 R 15 31 R 15 76 R 0 45 R -15 76 R -15 31 R -16 15 R -30 15 R D 5261 1830 M 0 186 R D 5154 1402 M 16 -15 R -16 -15 R -15 15 R 0 15 R 15 31 R 16 15 R 45 15 R 61 0 R 46 -15 R 15 -15 R 15 -31 R 0 -30 R -15 -30 R -46 -31 R -76 -30 R -30 -15 R -31 -31 R -15 -45 R 0 -46 R D 5276 1463 M 30 -15 R 16 -15 R 15 -31 R 0 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15 -45 R 30 -31 R 31 -15 R D 10739 868 M 61 0 R D 10785 549 M 61 0 R D 10952 868 M 0 -258 R 15 -46 R 31 -15 R 30 0 R 30 15 R 15 31 R D 10967 868 M 0 -258 R 15 -46 R 16 -15 R D 10906 762 M 122 0 R D 11180 868 M 0 -319 R D 11195 868 M 0 -319 R D 11195 716 M 30 31 R 46 15 R 30 0 R 46 -15 R 15 -31 R 0 -167 R D 11301 762 M 31 -15 R 15 -31 R 0 -167 R D 11134 868 M 61 0 R D 11134 549 M 107 0 R D 11301 549 M 107 0 R D 11742 929 M 0 -501 R D 11757 929 M 0 -501 R D 11742 929 M 106 0 R D 11742 428 M 106 0 R D 11970 762 M 0 -334 R D 11985 762 M 0 -334 R D 11985 716 M 30 31 R 31 15 R 30 0 R 46 -15 R 30 -31 R 15 -45 R 0 -31 R -15 -45 R -30 -31 R -46 -15 R -30 0 R -31 15 R -30 31 R D 12076 762 M 30 -15 R 31 -31 R 15 -45 R 0 -31 R -15 -45 R -31 -31 R -30 -15 R D 11924 762 M 61 0 R D 11924 428 M 106 0 R D 12289 762 M 0 -213 R D 12304 762 M 0 -213 R D 12304 716 M 30 31 R 46 15 R 30 0 R 46 -15 R 15 -31 R 0 -167 R D 12410 762 M 31 -15 R 15 -31 R 0 -167 R D 12471 716 M 30 31 R 46 15 R 30 0 R 46 -15 R 15 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15 76 R 0 46 R -15 76 R -31 45 R -45 15 R -30 0 R -31 -15 R -15 -15 R -15 -30 R -15 -76 R 0 -46 R 15 -76 R 15 -30 R 15 -15 R 31 -16 R D 2590 1830 M 30 16 R 15 15 R 16 30 R 15 76 R 0 46 R -15 76 R -16 30 R -15 15 R -30 15 R D 2886 3681 M 285 0 R D 2514 3757 M 30 15 R 46 45 R 0 -319 R D 2575 3802 M 0 -304 R D 2514 3498 M 137 0 R D 2886 5532 M 285 0 R D 2484 5607 M 15 -15 R -15 -15 R -16 15 R 0 15 R 16 31 R 15 15 R 45 15 R 61 0 R 46 -15 R 15 -15 R 15 -31 R 0 -30 R -15 -30 R -46 -31 R -76 -30 R -30 -15 R -30 -31 R -16 -45 R 0 -46 R D 2605 5668 M 30 -15 R 16 -15 R 15 -31 R 0 -30 R -15 -30 R -46 -31 R -61 -30 R D 2468 5380 M 16 15 R 30 0 R 76 -31 R 45 0 R 31 16 R 15 15 R D 2514 5395 M 76 -46 R 61 0 R 15 15 R 15 31 R 0 30 R D 2886 7383 M 285 0 R D 2484 7458 M 15 -15 R -15 -15 R -16 15 R 0 15 R 16 31 R 15 15 R 45 15 R 61 0 R 46 -15 R 15 -31 R 0 -45 R -15 -30 R -46 -16 R -45 0 R D 2605 7519 M 30 -15 R 16 -31 R 0 -45 R -16 -30 R -30 -16 R 30 -15 R 31 -30 R 15 -31 R 0 -45 R -15 -31 R -15 -15 R 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0 R 30 15 R 15 46 R 0 45 R -15 31 R -30 30 R D 1884 3701 M 15 -31 R 30 -15 R 31 0 R 30 15 R 15 31 R D 1838 4126 M 15 -15 R 15 15 R -15 15 R -15 0 R -30 -30 R -16 -30 R 0 -46 R 16 -46 R 30 -30 R 46 -15 R 30 0 R 46 15 R 30 30 R 15 46 R 0 30 R -15 46 R -30 30 R D 1792 4035 M 16 -30 R 30 -31 R 46 -15 R 30 0 R 46 15 R 30 31 R 15 30 R D 1792 4263 M 213 0 R D 1792 4278 M 213 0 R D 1884 4278 M -46 15 R -30 31 R -16 30 R 0 45 R 16 16 R 15 0 R 15 -16 R -15 -15 R -15 15 R D 1792 4217 M 0 61 R D 2005 4217 M 0 107 R D 1792 4582 M 16 -46 R 30 -30 R 46 -15 R 30 0 R 46 15 R 30 30 R 15 46 R 0 30 R -15 46 R -30 30 R -46 15 R -30 0 R -46 -15 R -30 -30 R -16 -46 R 0 -30 R 16 -31 R 30 -30 R 46 -15 R 30 0 R 46 15 R 30 30 R 15 31 R D 2005 4612 M -15 31 R -30 30 R -46 15 R -30 0 R -46 -15 R -30 -30 R -16 -31 R D 1686 4825 M 258 0 R 46 15 R 15 30 R 0 31 R -15 30 R -30 15 R D 1686 4840 M 258 0 R 46 15 R 15 15 R D 1792 4779 M 0 122 R D 1792 5053 M 168 0 R 30 15 R 15 45 R 0 31 R -15 45 R -30 31 R D 1792 5068 M 168 0 R 30 15 R 15 30 R D 1792 5220 M 213 0 R D 1792 5235 M 213 0 R D 1792 5007 M 0 61 R D 1792 5174 M 0 61 R D 2005 5220 M 0 60 R D 1792 5387 M 213 0 R D 1792 5402 M 213 0 R D 1884 5402 M -46 15 R -30 31 R -16 30 R 0 46 R 16 15 R 15 0 R 15 -15 R -15 -16 R -15 16 R D 1792 5341 M 0 61 R D 2005 5341 M 0 107 R D 1686 5645 M 319 0 R D 1686 5660 M 319 0 R D 1838 5660 M -30 31 R -16 30 R 0 30 R 16 46 R 30 30 R 46 15 R 30 0 R 46 -15 R 30 -30 R 15 -46 R 0 -30 R -15 -30 R -30 -31 R D 1792 5751 M 16 31 R 30 30 R 46 15 R 30 0 R 46 -15 R 30 -30 R 15 -31 R D 1686 5599 M 0 61 R D 1792 5964 M 168 0 R 30 15 R 15 46 R 0 30 R -15 46 R -30 30 R D 1792 5979 M 168 0 R 30 15 R 15 31 R D 1792 6131 M 213 0 R D 1792 6146 M 213 0 R D 1792 5918 M 0 61 R D 1792 6086 M 0 60 R D 2005 6131 M 0 61 R D 1686 6298 M 319 0 R D 1686 6313 M 319 0 R D 1686 6253 M 0 60 R D 2005 6253 M 0 106 R D 1884 6450 M 0 182 R -31 0 R -30 -15 R -15 -15 R -16 -30 R 0 -46 R 16 -46 R 30 -30 R 46 -15 R 30 0 R 46 15 R 30 30 R 15 46 R 0 30 R -15 46 R -30 30 R D 1884 6617 M -46 0 R -30 -15 R D 1792 6526 M 16 -30 R 30 -31 R 46 -15 R 30 0 R 46 15 R 30 31 R 15 30 R D 1792 6754 M 213 0 R D 1792 6769 M 213 0 R D 1838 6769 M -30 30 R -16 46 R 0 30 R 16 46 R 30 15 R 167 0 R D 1792 6875 M 16 31 R 30 15 R 167 0 R D 1792 6708 M 0 61 R D 2005 6708 M 0 107 R D 2005 6875 M 0 107 R D 1838 7240 M 15 -15 R 15 15 R -15 15 R -15 0 R -30 -30 R -16 -31 R 0 -45 R 16 -46 R 30 -30 R 46 -15 R 30 0 R 46 15 R 30 30 R 15 46 R 0 30 R -15 46 R -30 30 R D 1792 7149 M 16 -31 R 30 -30 R 46 -15 R 30 0 R 46 15 R 30 30 R 15 31 R D 1884 7361 M 0 183 R -31 0 R -30 -15 R -15 -16 R -16 -30 R 0 -46 R 16 -45 R 30 -31 R 46 -15 R 30 0 R 46 15 R 30 31 R 15 45 R 0 31 R -15 45 R -30 31 R D 1884 7529 M -46 0 R -30 -16 R D 1792 7437 M 16 -30 R 30 -30 R 46 -16 R 30 0 R 46 16 R 30 30 R 15 30 R D 1625 7893 M 502 0 R D 1625 7908 M 502 0 R D 1625 7893 M 0 106 R D 2127 7893 M 0 106 R D 1686 8121 M 319 0 R D 1686 8136 M 319 0 R D 1792 8288 M 152 -152 R D 1884 8212 M 121 91 R D 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R 14 1 R 15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F 5277 10409 M -1 15 R -3 14 R -5 14 R -6 13 R -8 12 R -10 11 R -11 9 R -12 8 R -13 7 R -13 5 R -15 2 R -14 1 R -15 -1 R -14 -2 R -14 -5 R -13 -7 R -12 -8 R -11 -9 R -9 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 9 -11 R 11 -10 R 12 -8 R 13 -6 R 14 -5 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 12 8 R 11 10 R 10 11 R 8 12 R 6 13 R 5 14 R 3 14 R 1 14 R F 4517 10289 M -1 14 R -3 15 R -5 13 R -6 13 R -8 13 R -10 10 R -11 10 R -12 8 R -13 7 R -13 4 R -15 3 R -14 1 R -15 -1 R -14 -3 R -14 -4 R -13 -7 R -12 -8 R -11 -10 R -9 -10 R -8 -13 R -7 -13 R -4 -13 R -3 -15 R -1 -14 R 1 -15 R 3 -14 R 4 -13 R 7 -14 R 8 -12 R 9 -11 R 11 -9 R 12 -8 R 13 -7 R 14 -4 R 14 -3 R 15 -1 R 14 1 R 15 3 R 13 4 R 13 7 R 12 8 R 11 9 R 10 11 R 8 12 R 6 14 R 5 13 R 3 14 R 1 15 R F 9563 9154 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -9 11 R -11 9 R -12 9 R -13 6 R -14 5 R -14 2 R -15 1 R -14 -1 R -15 -2 R -13 -5 R -13 -6 R -12 -9 R -11 -9 R -10 -11 R -8 -12 R -6 -13 R -5 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 5 -14 R 6 -13 R 8 -12 R 10 -11 R 11 -10 R 12 -8 R 13 -6 R 13 -5 R 15 -3 R 14 -1 R 15 1 R 14 3 R 14 5 R 13 6 R 12 8 R 11 10 R 9 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R F 9670 8758 M -1 15 R -3 14 R -4 14 R -7 13 R -8 12 R -10 11 R -10 9 R -13 8 R -13 7 R -13 5 R -15 2 R -14 1 R -14 -1 R -15 -2 R -13 -5 R -14 -7 R -12 -8 R -10 -9 R -10 -11 R -8 -12 R -7 -13 R -4 -14 R -3 -14 R -1 -15 R 1 -14 R 3 -14 R 4 -14 R 7 -13 R 8 -12 R 10 -11 R 10 -10 R 12 -8 R 14 -6 R 13 -5 R 15 -3 R 14 -1 R 14 1 R 15 3 R 13 5 R 13 6 R 13 8 R 10 10 R 10 11 R 8 12 R 7 13 R 4 14 R 3 14 R 1 14 R F L1 10379 1830 M 0 9254 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f9a.eps0100644000000000000000000013240210376206774010763 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/HD140283 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:07:41 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 2010 4200 M 0 182 R D 5577 4200 M 0 182 R D 9144 4200 M 0 182 R D 12710 4200 M 0 182 R D 16277 4200 M 0 182 R D 2902 4200 M 0 91 R D 3793 4200 M 0 91 R D 4685 4200 M 0 91 R D 6468 4200 M 0 91 R D 7360 4200 M 0 91 R D 8252 4200 M 0 91 R D 10035 4200 M 0 91 R D 10927 4200 M 0 91 R D 11819 4200 M 0 91 R D 13602 4200 M 0 91 R D 14494 4200 M 0 91 R D 15385 4200 M 0 91 R D 1800 13300 M 15300 0 R D 2010 13300 M 0 -182 R D 5577 13300 M 0 -182 R D 9144 13300 M 0 -182 R D 12710 13300 M 0 -182 R D 16277 13300 M 0 -182 R D 2902 13300 M 0 -91 R D 3793 13300 M 0 -91 R D 4685 13300 M 0 -91 R D 6468 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435 4 R 437 8 R 435 -11 R 435 -22 R 437 308 R 435 261 R 435 -84 R 435 -522 R 437 -717 R 436 -317 R 435 399 R 437 633 R 435 229 R 435 39 R 435 -325 R 437 -186 R 435 190 R 435 -51 R 437 -161 R 435 117 R 436 297 R 435 -133 R 437 36 R 435 52 R 435 8 R 437 30 R 435 17 R 435 -140 R 23 -1 R D L2 1800 2909 M 28 7 R 435 -218 R 437 87 R 435 185 R 435 -128 R 437 -60 R 436 -63 R 435 110 R 435 -5 R 437 -22 R 435 -88 R 435 -178 R 437 77 R 435 74 R 435 14 R 435 41 R 437 155 R 436 347 R 435 390 R 437 -59 R 435 -625 R 435 -508 R 435 -417 R 437 2 R 435 425 R 435 100 R 437 -85 R 435 145 R 436 306 R 435 -130 R 437 37 R 435 53 R 435 8 R 437 30 R 435 18 R 435 -140 R 23 -1 R D 10 setlinewidth L1 1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f9b.eps0100644000000000000000000013143310376206774010767 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, /Users/martin/conv/output/1D/HD140283 %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 14:51:51 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 4200 M 15300 0 R D 4341 4200 M 0 182 R D 7596 4200 M 0 182 R D 10851 4200 M 0 182 R D 14107 4200 M 0 182 R D 1899 4200 M 0 91 R D 2713 4200 M 0 91 R D 3527 4200 M 0 91 R D 5155 4200 M 0 91 R D 5968 4200 M 0 91 R D 6782 4200 M 0 91 R D 8410 4200 M 0 91 R D 9224 4200 M 0 91 R D 10038 4200 M 0 91 R D 11665 4200 M 0 91 R D 12479 4200 M 0 91 R D 13293 4200 M 0 91 R D 14921 4200 M 0 91 R D 15735 4200 M 0 91 R D 16548 4200 M 0 91 R D 1800 13300 M 15300 0 R D 4341 13300 M 0 -182 R D 7596 13300 M 0 -182 R D 10851 13300 M 0 -182 R D 14107 13300 M 0 -182 R D 1899 13300 M 0 -91 R D 2713 13300 M 0 -91 R D 3527 13300 M 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253 R 436 876 R 436 483 R 436 -122 R 438 -305 R 184 491 R D 13226 4200 M 33 -48 R 436 -734 R 438 -285 R 436 -516 R 436 33 R 437 200 R 437 -814 R 437 309 R 436 706 R 347 -115 R D 10 setlinewidth L1 1800 2800 M 15299 0 R D %%PageTrailer end %%PageResources: font Times-Roman %%Trailer %%Pages: 1 %%DocumentNeededResources: font Times-Roman %%EOF f9c.eps0100644000000000000000000010121310376206774010761 0ustar rootroot%!PS-Adobe-3.0 EPSF-3.0 %%BoundingBox: 0 0 510 396 %%Title: Graphics produced by IDL %%For: martin@macmartin.anu.edu.au, %% /Users/martin/conv/output/1D/HD140283/figures %%Creator: IDL Version 6.1.1, Mac OS X (darwin ppc m32) %%CreationDate: Wed Feb 15 15:22:08 2006 %%DocumentData: Clean7bit %%Requirements: color %%LanguageLevel: 1 %%PageOrder: Ascend %%Pages: (atend) %%DocumentNeededResources: (atend) %%EndComments %%BeginProlog %+ prolog.ps -- Prolog for IDL generated PostScript files %+ Copyright (c) 1988-2004 Research Systems, Inc. All Rights Reserved. %v 5 /$IDL_DICT 40 dict def $IDL_DICT begin /bdef { bind def } bind def /C {currentpoint newpath moveto} bdef /CP {currentpoint} bdef /D {currentpoint stroke moveto} bdef /F {closepath fill} bdef /K { setgray } bdef /M {moveto} bdef /N {rmoveto} bdef /P {lineto} bdef /R {rlineto} bdef /S {gsave show grestore} bdef /X {currentpoint pop} bdef /Z {gsave currentpoint lineto 20 setlinewidth 1 setlinecap stroke grestore} bdef /L0 {[] 0 setdash} bdef /L1 {[40 100] 0 setdash} bdef /L2 {[200 200] 0 setdash} bdef /L3 {[200 100 50 100] 0 setdash} bdef /L4 {[300 100 50 100 50 100 50 100] 0 setdash} bdef /L5 {[400 200] 0 setdash} bdef /STDFONT { findfont exch scalefont setfont } bdef /ISOFONT { findfont dup length dict begin { 1 index /FID ne {def} {pop pop} ifelse } forall /Encoding ISOLatin1Encoding def currentdict end /idltmpfont exch definefont exch scalefont setfont } bdef /ISOBULLET { gsave /Helvetica findfont exch scalefont setfont (\267) show currentpoint grestore moveto} bdef /MITERLIMIT { 2.5 setmiterlimit } bdef end %%EndProlog %%Page: 0 1 %%PageRequirements: color %%PageResources: (atend) %%PageOrientation: Portrait %%PageBoundingBox: 0 0 510 396 %%BeginPageSetup $IDL_DICT begin 0.0283465 dup scale MITERLIMIT %%IncludeResource: font Times-Roman 423.333 /Times-Roman STDFONT %%EndPageSetup 10 setlinewidth L0 0.000 0.000 0.000 setrgbcolor 1800 1400 M 15300 0 R D 2164 1400 M 0 238 R D 1481 850 M 273 0 R D 1952 1033 M -46 -16 R -30 -45 R -16 -76 R 0 -46 R 16 -76 R 30 -45 R 46 -15 R 30 0 R 46 15 R 30 45 R 15 76 R 0 46 R -15 76 R -30 45 R -46 16 R -30 0 R -31 -16 R -15 -15 R -15 -30 R -15 -76 R 0 -46 R 15 -76 R 15 -30 R 15 -15 R 31 -15 R D 1982 714 M 30 15 R 16 15 R 15 30 R 15 76 R 0 46 R -15 76 R -15 30 R -16 15 R -30 16 R D 2195 744 M -16 -15 R 16 -15 R 15 15 R -15 15 R D 2362 972 M 30 15 R 46 46 R 0 -319 R D 2423 1017 M 0 -303 R D 2362 714 M 136 0 R D 2711 1033 M -45 -16 R -31 -45 R -15 -76 R 0 -46 R 15 -76 R 31 -45 R 45 -15 R 30 0 R 46 15 R 30 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rootroot%\documentclass[12pt,preprint]{aastex} %\documentclass[10pt,preprint2]{aastex} %\usepackage{graphicx, epsf, times} \documentclass{emulateapj} %\usepackage{graphicx, epsf, times} %\documentclass{article} %\usepackage{emulateapj, graphicx, epsf, times} %% manuscript produces a one-column, double-spaced document: %\documentclass[manuscript]{aastex} %% preprint2 produces a double-column, single-spaced document: %\documentclass[preprint2, 10pt]{aastex} \newcommand{\liratio}{$^6$Li/$^7$Li} \newcommand{\liratioinverse}{$^7$Li/$^6$Li} \newcommand{\lisix}{$^6$Li} \newcommand{\liseven}{$^7$Li} \newcommand{\benine}{$^9$Be} \newcommand{\lisixbe}{$^6$Li/Be} \newcommand{\hi}{H\,{\sc i}} \newcommand{\lii}{Li\,{\sc i}} \newcommand{\beii}{Be\,{\sc ii}} \newcommand{\bi}{B\,{\sc i}} \newcommand{\oi}{O\,{\sc i}} \newcommand{\oifor}{[O\,{\sc i}]} \newcommand{\mgi}{Mg\,{\sc i}} \newcommand{\ki}{K\,{\sc i}} \newcommand{\cai}{Ca\,{\sc i}} \newcommand{\fei}{Fe\,{\sc i}} \newcommand{\feii}{Fe\,{\sc ii}} \newcommand{\logh}{log\,$\epsilon_{\rm H}$} \newcommand{\loghe}{log\,$\epsilon_{\rm He}$} \newcommand{\logli}{log\,$\epsilon_{\rm Li}$} \newcommand{\logliseven}{log\,$\epsilon_{\rm ^7Li}$} \newcommand{\loglisix}{log\,$\epsilon_{\rm ^6Li}$} \newcommand{\logbe}{log\,$\epsilon_{\rm Be}$} \newcommand{\logo}{log\,$\epsilon_{\rm O}$} \newcommand{\logfe}{log\,$\epsilon_{\rm Fe}$} \newcommand{\feh}{[Fe/H]} \newcommand{\feih}{[\fei /H]} \newcommand{\feiih}{[\feii /H]} \newcommand{\beh}{[Be/H]} \newcommand{\oh}{[O/H]} \newcommand{\kh}{[K/H]} \newcommand{\cah}{[Ca/H]} \newcommand{\befe}{[Be/Fe]} \newcommand{\bfe}{[B/Fe]} \newcommand{\ofe}{[O/Fe]} \newcommand{\kfe}{[K/Fe]} \newcommand{\cafe}{[Ca/Fe]} \newcommand{\alphafe}{[$\alpha$/Fe]} \newcommand{\fefesun}{Fe/Fe$_\sun$} \newcommand{\oosun}{O/O$_\sun$} \newcommand{\teff}{$T_{\rm eff}$} \newcommand{\logteff}{log\,$T_{\rm eff}$} \newcommand{\logg}{log\,$g$} \newcommand{\micro}{$\xi_{\rm turb}$} \newcommand{\macro}{$\zeta_{\rm macro}$} \newcommand{\vsini}{$v_{\rm rot} \sin i$} \newcommand{\vrot}{\mbox{$v_{\rm rot}$}} \newcommand{\vrad}{$v_{\rm rad}$} \newcommand{\chitwo}{$\chi^2$} \newcommand{\chitwomin}{$\chi^2_{\rm min}$} \newcommand{\chitwored}{$\chi^2_{\rm red}$} \newcommand{\kms}{km\,s$^{-1}$} \newcommand{\mv}{\mbox{$M_V$}} \newcommand{\mstar}{\mbox{$M_*$}} \newcommand{\msun}{\mbox{$M_\sun$}} \newcommand{\mvstar}{\mbox{$M_V {\rm (star)}$}} \newcommand{\mvzams}{\mbox{$M_V {\rm (ZAMS)}$}} \newcommand{\vk}{$(V-K)$} \newcommand{\by}{$(b-y)$} \newcommand{\ha}{H$\alpha$} \newcommand{\hb}{H$\beta$} \newcommand{\marcs}{{\sc marcs}} \newcommand{\gf}{$gf$} \slugcomment{Accepted by ApJ} \shorttitle{Lithium isotopic abundances in metal-poor halo stars} \shortauthors{Asplund et al.} \begin{document} \title{Lithium isotopic abundances in metal-poor halo stars \footnote{Based on observations collected at the European Southern Observatory, Paranal, Chile (observing programs 65.L-0131, 68.D-0091 and 273.D-5043)} } \author{Martin Asplund} \affil{Research School of Astronomy and Astrophysics, Mt. Stromlo Observatory, Cotter Road, Weston, ACT 2611, Australia \email{martin@mso.anu.edu.au} } \author{David L. Lambert} \affil{The W.J. McDonald Observatory, The University of Texas at Austin, Austin, TX 78712-1083, USA} \author{Poul Erik Nissen} \affil{Department of Physics and Astronomy, Aarhus University, DK-8000, Aarhus C, Denmark} \author{Francesca Primas} \affil{European Southern Observatory, Karl-Schwarzschild Str. 2, D-85748 Garching b. M\"unchen, Germany} \and \author{Verne V. Smith} \affil{National Optical Astronomy Observatory, P.O. Box 26732, Tucson, AZ 85726, USA} \begin{abstract} Very high-quality spectra of 24 metal-poor halo dwarfs and subgiants have been acquired with ESO's VLT/UVES for the purpose of determining Li isotopic abundances. The derived 1D, non-LTE \liseven\ abundances from the \lii\ 670.8\,nm line reveal a pronounced dependence on metallicity but with negligible scatter around this trend. Very good agreement is found between the abundances from the \lii\ 670.8\,nm line and the \lii\ 610.4\,nm line. The estimated primordial \liseven\ abundance is $^7{\rm Li/H} = 1.1-1.5 \cdot 10^{-10}$, which is a factor of three to four lower than predicted from standard Big Bang nucleosynthesis with the baryon density inferred from the cosmic microwave background. Interestingly, \lisix\ is detected in nine of our 24 stars at the $\ge 2\sigma$ significance level. Our observations suggest the existence of a \lisix\ plateau at the level of \loglisix\,$\approx 0.8$; however, taking into account predictions for \lisix\ destruction during the pre-main sequence evolution tilts the plateau such that the \lisix\ abundances apparently increase with metallicity. Our most noteworthy result is the detection of \lisix\ in the very metal-poor star LP\,815-43. Such a high \lisix\ abundance during these early Galactic epochs is very difficult to achieve by Galactic cosmic ray spallation and $\alpha$-fusion reactions. It is concluded that both Li isotopes have a pre-Galactic origin. Possible \lisix\ production channels include proto-galactic shocks and late-decaying or annihilating supersymmetric particles during the era of Big Bang nucleosynthesis. The presence of \lisix\ limits the possible degree of stellar \liseven\ depletion and thus sharpens the discrepancy with standard Big Bang nucleosynthesis. \keywords{Stars: abundances -- Stars: atmospheres -- Stars: Population II -- Galaxy: evolution -- Cosmology: early Universe } \end{abstract} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \section{Introduction} \label{s:introduction} Lithium's two stable isotopes -- \lisix\ and \liseven\ -- continue to pose intriguing questions for astrophysicists concerned with understanding the origins of this light element. These questions concern the abundance of lithium in cool interstellar gas and every type of star in which lines of neutral lithium are either detected or are potentially detectable. In this paper, we address by new observations questions about the origin of the lithium seen in the atmospheres of metal-poor stars. In particular, we provide an adequate set of determinations of the isotopic abundance ratio \liratio\ with which to constrain some theoretical ideas on the origins of the rare \lisix\ isotope and of the majority \liseven\ isotope for which the Big Bang is widely identified as the initial and major origin. An observational link of \liseven\ with the Big Bang was promoted first by Spite \& Spite (1982) who showed that the lithium abundance in the warmest metal-poor dwarfs was independent of metallicity for \feh\,$< -1.5$. Their derived abundance of lithium in the dwarfs was given as \logli\,$= 2.05\pm0.15$ on the usual scale where \logh\,$=12.00$. The constant lithium abundance defining what is commonly called `the Spite plateau' suggested that this may be the lithium abundance in pre-Galactic gas provided by the Big Bang. In the succeeding years, many observers have reinvestigated the lithium abundance of the Spite plateau but the lithium (\liseven ) abundance has strayed little from the Spites' original estimate. Here, we also present a new determination of the plateau's lithium abundance as extrapolated to zero metallicity that remains faithful to the 1982 estimate. Early observations showed that the lithium on the plateau was primarily \liseven , as expected from a standard Big Bang: Maurice et al. (1984) set an upper limit \liratio\,$<0.1$ for a couple of stars. The first probable detection of \lisix\ in a very metal-poor star was reported by Smith et al. (1993) for HD\,84937 with \liratio\,$= 0.06\pm0.03$. Confirmation was provided by Hobbs \& Thorburn (1994, 1997), Smith et al. (1998) and subsequently by Cayrel et al. (1999) who obtained \liratio\,$= 0.052\pm0.019$. Smith et al. (1998) observed seven single stars and reported \lisix\ in one additional very metal-poor star (BD\,$+26\arcdeg 3578$, also known as HD\,338529). Cayrel et al. provided a possible detection of \lisix\ in BD\,$+42\arcdeg 2667$ as did Nissen et al. (2000) for G\,271-162. Non-detections gave upper limits variously in the range \liratio\,$<0.03-0.10$. Two questions now face students of the abundances of \lisix\ and \liseven\ in very metal-poor stars. First, predictions of the nucleosynthesis by the Big Bang are tightly constrained because analysis of the anisotropies of the cosmic microwave background determine the one free parameter in a standard cosmological models that sets the abundances (relative to $^1$H) of the products $^2$H, $^3$He, $^4$He, and \liseven . The free parameter is the ratio of baryons to photons $\eta = n_{\rm b}/n_\gamma$ or equivalently the fraction of the critical density $\Omega_b$ provided by baryons: $\Omega_{\rm b} = 3.652 \times 10^7\eta/h^2$ where $h$ is the Hubble constant in units of 100\,\kms\,Mpc$^{-1}$. The recent WMAP-based analysis of the cosmic microwave background implies $\Omega_{\rm b} h^2 = 0.0224 \pm 0.0009$ (Spergel et al. 2003), which in standard Big Bang nucleosynthesis corresponds to an abundance of \logliseven\,$ = 2.65 \pm 0.10$ (Coc et al. 2004; Cuoco et al. 2004; Cyburt 2004). This predicted abundance of \liseven\ is about 0.5 dex or a factor of three larger than the measured abundance of lithium on the Spite plateau. Thus, one key question has become -- How does one bridge the 0.5 dex gap between observation and prediction? The second question arises from the detections of $^6$Li. Our results suggest that there may be a \lisix\ plateau parallel to the Spite plateau for \liseven\ with the implication that the major fraction of the \lisix\ (and presumably some of the \liseven ) may have been synthesised prior to the onset of star formation in the Galaxy. The \lisix\ abundance of the plateau exceeds by a large factor the \lisix\ expected from a standard Big Bang. Thus, our second key question is -- How does one account for the high abundance of \lisix\ in some metal-poor stars? Our principal concern in undertaking the observations reported here was to extend high-precision measurements of \lisix\ to more metal-poor stars and to lower metallicities. The observations and the analysis techniques are described below in Sections \ref{s:observations} and \ref{s:analysis}, respectively. Section \ref{s:parameters} deals with the determination of stellar parameters, abundances, and macroturbulent velocities. The derivation of the Li isotopic abundances from the observed line shapes of the \lii\ 670.8\,nm resonance line is outlined in Section \ref{s:li6708}, while the analysis of the subordinate \lii\ 610.4\,nm line is presented in Section \ref{s:li6104}. In Section \ref{s:evolution}, we take up the two questions just outlined: How can one reconcile the predicted \liseven\ abundance using the WMAP-based $\Omega_{\rm b} h^2$ with the measurement of the abundance for the Spite plateau? How does one account for those \lisix\ abundances that greatly exceed the Big Bang prediction? %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \section{Observations and data reduction} \label{s:observations} \subsection{Selection of Stars} \label{s:sample} Programme stars were selected from the $uvby$-$\beta$ catalogue of Schuster \& Nissen \cite{schuster88} and from the Li abundance survey of very metal-poor stars by Ryan et al. \cite{ryan99}. In order to be able to study the possible evolution of the Li isotopes in the Galactic halo, we aimed at a group of stars covering the metallicity range $-3.0 <$ [Fe/H] $< -1.0$ and situated in the turnoff region of the Hertzsprung-Russell-diagram, where the upper convection zone of the stars is relatively thin so that proton destruction of Li is minimal. Furthermore, the stars had to be brighter than $V \sim 11$ in order to obtain very high resolution spectra with sufficiently high $S/N$. Finally, known double-lined spectroscopic binaries were avoided. \subsection{Spectroscopic Observations} \label{s:spectroscopy} Spectra of 23 stars were obtained with UVES (Dekker et al. 2000) on the ESO VLT 8.2m Kueyen telescope during three observing runs: July 23-25, 2000; February 5-7, 2002, and August 28-31, 2004 (5.5 hours in service mode). About 1/3 of the time during the first two periods was lost due to high humidity. The seeing varied from about $0.5\arcsec$ most of the time in July 2000 to occasionally more than $2\arcsec$ in February 2002. One of the nights in July 2000 was interrupted by ``Target of Opportunity" observations - later compensated by service observations on August 4, 2000. In order to obtain a spectral resolution of about $R \simeq 120\,000$, we used image slicer \#3, which for an entrance aperture of $1.5\arcsec \times 2\arcsec$ produces five slices each $0.3\arcsec$ wide. Thanks to the image slicer, the efficiency of UVES was quite good even during periods with bad seeing. In average conditions a $S/N$ of about 500 per spectral bin (0.00268\,nm at the \lii\ 670.8\,nm line) could be obtained for a $V \sim 11.0$ star in 2 hours. The total integration time was always split into at least three separate exposures so that cosmic rays hits on the CCD could be removed by comparison of the different spectra. The July 2000 and February 2002 spectra were taken in the red arm of UVES with cross disperser \#3 and a central wavelength of 705\,nm. With this non-standard setting, the EEV CCD covers the spectral region 600 - 700\,nm in 15 echelle orders, while the MIT CCD covers the region 710 - 820\,nm in 11 orders. We note that the \lii\ 670.8\,nm line is well centered on the EEV chip and that the orders are separated by more than 140 pixels so that despite of the large width of the orders (about 70 pixels) due to the image slicer, there is ample interorder space for measuring the CCD background including scattered light. Furthermore, the sky spectrum could be monitored through an extension of the entrance slit beyond the position of the image slicer. For further details we refer to Dekker et al. \cite{dekker02}. The service observations in August 2004 were carried out with a standard UVES setting of the red arm (cross disperser \#3, central wavelength 600\,nm). In this setting, the EEV chip covers the 500 - 595\,nm spectral region, and the MIT from 605 to 700\,nm. The primary purpose with this alternative setting was to check an interesting Li isotopic abundance ratio obtained for the very metal-poor star LP\,815-43 based on the July 2000 observations. Further details about the spectroscopic observations are given in Table \ref{t:observations}. In addition to the 23 stars listed here, G\,271-162 is also included in the present paper. Its spectrum was obtained during the commissioning of UVES in October 1999 with the same setting of UVES as in July 2000 and February 2002 but without the use of the image slicer, which was not available at the time. Instead the star was continuously moved along the slit to simulate the effect of the image slicer. This star has already been analyzed by Nissen et al. \cite{nissen00} but is re-analyzed here for comparison purposes. \subsection{Data Reduction} \label{s:reduction} The spectra have been reduced using standard tasks in the IRAF echelle package with the following steps included: {\em i)} bias subtraction, {\em ii)} fitting a 2-dimensional polynomial to the flux in the interorder regions and subtraction of scattered light, {\em iii)} pixel-by-pixel division with a normalized flat field exposed without the image slicer, {\em iv)} tracing and extraction of the echelle orders, {\em v)} corresponding extraction of a thorium calibration spectrum, {\em vi)} wavelength calibration, {\em vii)} rectification of the echelle orders by fitting cubic spline functions with a wavelength scale of about 0.5\,nm to the continuum, {\em viii)} correction for the Doppler shift of the spectral lines. For some stars this procedure was carried out for the individual slicer spectra, which were then combined to one spectrum by applying weights according to the exposure level of the slices. The resulting spectra were compared to spectra obtained by extraction with a long slit covering all five slices. The difference between the two sets of spectra is marginal in terms of $S/N$ and resolution. Hence, the simpler long slit extraction was applied for all stars as our final reduction procedure. Furthermore, we note that the echelle orders are not merged, which means that lines near the edges of the orders, e.g. the oxygen triplet at 777.4\,nm, can be measured in two consecutive orders. The sky background spectrum turned out to be negligible for all stars observed on July 23-25, 2000, August 4, 2000, and February 5-6, 2002. On these dates the Moon was close to first or last quarter. The observations of LP\,815-43 on August 30 - 31, 2004, however, took place during full Moon conditions, and the sky spectrum (corresponding to the extent of the five slices) turned out to be about 1\% of the signal in the spectrum of LP\,815-43. Hence, in this case the sky spectrum was subtracted. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/fig.resolution.eps}} \resizebox{\hsize}{!}{\includegraphics{f1.eps}} \caption{Measured resolving power of UVES based on the FWHM of thorium lines in the echelle order containing the \lii\ 670.8\,nm line. Filled circles: July 2000 (EEV CCD); Open circles: February 2002 (EEV CCD); open squares: August 2004 (MIT CCD). The curves are 3rd order fits to each set of data.} \label{f:resolution} \end{figure} The wavelength calibration is based on 20-40 thorium lines per echelle order. The rms of a third order polynomial transformation between pixel and wavelength is of the order of 0.12\,pm (1.2\,m\AA ). In addition, the Th lines can be used to check the resolution of UVES; the intrinsic width of a typical Th line is negligible compared to the measured width (Hobbs et al. 1999). The profiles of the Th lines are well approximated by Gaussians, but the resolving power as defined from the FWHM of the Th lines ($R = \lambda / \Delta \lambda _{\rm FWHM}$) varies along a given spectral order from about 100\,000 to 130\,000 on the EEV chip. As can be seen in Fig. \ref{f:resolution}, we achieved slightly higher resolving power during our first observing run in July 2000 than in February 2002. The lower resolution for the August 2004 spectra is caused by charge diffusion in the MIT chip, which, as mentioned above, was used in that period. In any case, the large number of Th lines available, enable us to map the variation of the resolving power along an echelle order. Hence, the actual instrumental broadening for a given stellar line is known and can be applied in connection with the spectrum synthesis. In addition to increasing the efficiency, the image slicer in UVES also serves to broaden the spectrum over a larger area of the CCD. This helps to minimize problems in the flat-fielding, i.e., to reduce the amplitude of any residual fringing existing after the flat-fielding. From exposures of bright B-type stars during the July 2000 observations we estimate that the residual fringing is less than about 0.1\,\%. For some unknown reason, the residual fringing turned out to be larger for the February 2002 spectra, reaching an amplitude of about 0.3\,\% on a wavelength scale that could affect the profiles of the spectral lines. Hence, we decided to determine a ``residual fringe function" from the continua of several very metal-poor stars observed in February 2002 taking advantage of the fact that these stars have only a few spectral lines, which are shifted to different positions in the spectra due to large differences in radial velocities. This residual fringe function is well defined and was applied to all spectra observed in February 2002. A similar procedure was applied to the spectra of LP815-43 obtained on August 30-31, 2004; in this case the spectrum of HD\,140283 from August 28, 2004 was used to define the residual fringe function. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/fig.HD140283_july_february.eps}} \resizebox{\hsize}{!}{\includegraphics{f2.eps}} \caption{Comparison of the \lii\ region in the July 2000 spectrum of HD\,140283 with the February 2002 spectrum (shifted by 0.05). The lower panel shows the difference between the two spectra.} \label{f:obsspec_HD140283} \end{figure} As a test of the quality of the spectra and of possible problems with the correction for residual fringing in particular, we compare in Fig. \ref{f:obsspec_HD140283} the \lii\ spectra of HD\,140283 ([Fe/H] = $-2.4$) obtained in July 2000 and Feb. 2002. As seen, there is no significant trend in the residuals, and the rms of the difference is 0.0016 corresponding to a $S/N$ of about 600. This is close to what one would expect for the $S/N$ values of each spectrum given in Table \ref{t:observations}. A similar comparison of the spectra of HD\,140283 from July 2000 and August 2004 does reveal a significant trend in the residuals, but this is mainly due to the lower resolution of the August 2004 spectrum. The $S/N$ of the spectra in the region around the \lii\ 670.8\,nm line ranges from about 400 for some of the very metal-poor stars to more than 1000 for the relatively bright star HD\,140283. All but two of the stars have $S/N>500$. Representative spectra are shown in Fig. \ref{f:obsspec} for a range of metallicities. \subsection{Radial Velocities and Binary Stars} \label{s:radvel} Our conclusions regarding the lithium isotope ratio could be compromised if our targets are binaries. We have searched available databases for evidence suggesting that our program stars are not single. The extensive radial velocity survey of Carney et al. (1994) contains 11 of our 23 stars. One of them, G\,126-062, is reported as a single-lined binary; the orbital solution by Latham et al. (2002) gives a period of 219 days and a radial velocity amplitude of $K = 4.8$\,\kms . In addition, Carney et al. list BD\,$+03\arcdeg0740$ as a suspected binary. Another accurate survey, that of Nordstr\"{o}m et al. (2004) based on radial velocities measured with the Coravel spectrometer, contains eight of our stars but except for G\,126-062 none of them are noted as binaries. Finally, Ryan et al. (1999) have nine of the most metal-poor stars in common with us, but again there is no evidence of radial velocity variations. To supplement these studies we have determined radial velocities for all our stars. The values are based on the measured Doppler shifts of four of the lines that are used in Sect. \ref{s:broadening} to determine the macroturbulent velocity broadening. The following laboratory wavelengths from the NIST database are adopted: \cai\ 612.2217\,nm, \cai\ 616.2173\,nm, \fei\ 623.0726\,nm and \cai\ 643.9075\,nm. In determining the radial velocity one should ideally correct for gravitional redshift and convective blueshift, but as the net effect is expected to be below 0.5\,\kms\ we have not made such a correction. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/fig.6710spectra.eps}} \resizebox{\hsize}{!}{\includegraphics{f3.eps}} \caption{Sample spectra around the \lii\ 670.8\,nm line with the spectra of CD\,$-48\arcdeg2445$ and CD\,$-33\arcdeg3337$ shifted 0.10 and 0.20, respectively. Note, that the region between the \lii\ and the \cai\ lines in the spectrum of CD\,$-33\arcdeg3337$ is affected by several faint lines, which are not identified on the figure.} \label{f:obsspec} \end{figure} The measured radial velocities (corrected to heliocentric values using the IRAF task {\em rvcorrect}) are given in Table \ref{t:observations}. The accuracy of the velocities depends on the stability of UVES because the thorium comparison spectrum was obtained only a few times per night. Comparing the radial velocities for stars observed on different nights we estimate that the precision is $\pm 0.3$\,\kms , i.e. similar or slightly better than the precision obtained in the radial velocity surveys mentioned above. A comparison to the data in these three sources and those in the Li isotope study of Smith et al. (1998) gives the following mean differences (us - them) and rms dispersions of the differences \vspace{1mm} (excluding G\,126-062): \\ Carney et al. (1994): $\Delta v_{\rm r} = +0.6 \pm 0.4$\,\kms\ (10), \\ Nordstr\"{o}m et al. (2004): $\Delta v_{\rm r} = -0.4 \pm 0.6$\,\kms\ (7), \\ Ryan et al. (1999): $\Delta v_{\rm r} = +0.5 \pm 0.3$\,\kms\ (9), \\ \vspace{1mm}Smith et al. (1998): $\Delta v_{\rm r} = -0.4 \pm 0.4$\,\kms\ (7), \\ where the number within parenthesis denotes the number of stars in each comparison. Evidently, there are small systematic differences in the zero point of the radial velocities, but the small rms dispersions are as expected; hence, no additional evidence for binarity is revealed. In particular, we note that BD\,$+03\arcdeg0740$ that was suspected to be a binary by Carney et al. is included in three of the four comparisons and shows no sign of variability. Out of the 23 stars in Table \ref{t:observations}, there are only three (HD\,213657, CD\,$-33\arcdeg3337$ and CD\,$-48\arcdeg2445$) for which our radial velocities could not be compared to other accurate sources. The spectra of these stars show no evidence of lines from a companion; the same is true for the other stars including G\,126-062. Hence, we feel confident that all stellar spectra can be used for determining the Li isotopic ratio. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \section{Analysis: Methods, Models and Input Data} \label{s:analysis} \subsection{Stellar Model Atmospheres} \label{s:model_atmospheres} In the present study, we have made use of both 1D LTE hydrostatic and time-dependent 3D hydrodynamical stellar model atmospheres. One-dimensional model atmospheres with convection treated by the mixing length theory for the particular stellar parameters of our sample have been generated with the \marcs\ code (Gustafsson et al. 1975; Asplund et al. 1997), which includes realistic continuous and line opacities for a wide range of atomic and molecular species. The radiative transfer in the construction of the model atmospheres is treated by opacity sampling. As all our stars are metal-poor, the chemical composition of the models have an over-abundance of the $\alpha$-elements of \alphafe\,$=+0.5$ and a helium abundance of \loghe\,$=10.93$ (Asplund et al. 2005). This He abundance corresponds to a He mass fraction of $Y=0.253$, which is close to the expected value from standard Big Bang nucleosynthesis (e.g. Steigman 2005). For test purposes we have also employed theoretical 1D Kurucz model atmospheres without convective overshoot as computed by Castelli et al. (1997). Those models are based on very much the same approximations and assumptions as our standard \marcs\ models and have been interpolated to the specific stellar parameters of our sample from the available grid of models. A novel feature of our analysis compared with the pioneering works on Li isotopic abundances in metal-poor stars of Andersen et al. (1984), Smith et al. (1993, 1998), Hobbs \& Thorburn (1994, 1997), Nissen et al. (1999), Hobbs et al. (1999) and Cayrel et al. (1999) \footnote{We recognize even earlier observational studies by, for example, Herbig (1964), Feast (1966) and Cohen (1972) who attempted to derive Li isotopic abundances using both the center-of-gravity and profile fitting methods. These works were restricted to Galactic disk stars and yielded no convincing \lisix\ detections.}, is our use also of time-dependent 3D hydrodynamical stellar model atmospheres for the stars for which such 3D models with appropriate stellar parameters exist. The 3D model atmospheres of metal-poor stars are taken from Asplund et al. (1999) and Asplund \& Garc\'{\i}a P\'{e}rez (2001). In short, the models have been constructed by solving the standard hydrodynamical equations of conservation of mass, momentum and energy coupled with a simultaneous solution of the 3D radiative transfer in a representative volume of the stellar atmosphere and near sub-surface layers (e.g. Stein \& Nordlund 1998; Asplund et al. 2000). The 3D models are based on realistic continuous and line opacities and equation-of-state computed for the appropriate \feh\ under the assumption of LTE and opacity binning (Nordlund 1982). At any given time the simulation box is sufficiently large to cover at least ten upflowing regions (granules). The time sequence for each simulation employed is at least one convective turn-over time divided into thirty or more individual snapshots to give statistically significant results for the spatially and temporally averaged line profiles. In contrast to the 1D model atmospheres, no mixing length theory enters for the calculation of the convective energy flux. Instead, the time-dependent hydrodynamical simulation automatically and self-consistently predicts the convection efficiency as a function of depth for the given stellar parameters. \subsection{Spectral Line Formation} \label{s:line_formation} The spectral line formation is treated under the assumption of (strong) LTE making the source function equal to the Planck function: $S_\nu \left(\tau\right) = B_\nu \left[T\left(\tau\right)\right]$, i.e. continuum scattering is treated as an absorption. The lines used in our study are located at wavelengths at which Rayleigh and electron scattering make a negligible contribution to the source function; we have ensured that identical results are obtained with the code used herein and the code {\sc bsyn} from the Uppsala spectrum synthesis package that treats continuum scattering properly within the LTE framework. The radiative transfer is solved with a Fortran implementation of the Feautrier method to which is coupled an IDL routine for the \chitwo -analysis to find the optimum solution in terms of element abundance, wavelength shift, continuum normalization and extra broadening beyond the instrumental broadening (1D: macroturbulence and rotation, 3D: rotation only). The rotational broadening is performed through a disk-integration of the angle-dependent intensity profiles. In the 1D case, microturbulence is prescribed and not part of the \chitwo -optimization while the parameter does not enter the 3D calculations. The same code is able to handle both 1D and 3D geometries with otherwise identical calculations, which is a great advantage when investigating the possible systematic errors when relying on 1D plane-parallel model atmospheres. The background continuous opacities are taken from the \marcs\ project (Gustafsson et al. 1975; Asplund et al. 1997; Gustafsson et al., in preparation). We have verified that identical \liratio\ ratios and absolute Li abundances to within 0.01\,dex would result with the independent spectrum synthesis code {\sc bsyn} which comes as part of the Uppsala package. The resulting velocity field from the predicted convection and waves in the 3D models introduce Doppler shifts, which translate to shifts and asymmetries of spectral lines. These will depend on the line formation depths and the atmospheric conditions (in particular temperature, pressure and velocity) for the individual lines, making the detailed line shapes sensitive probes of the stellar atmospheres. As will become clear in Sect. \ref{s:li6708_3D}, this results in a significant improvement in the ability to reproduce the detailed shapes of spectral lines (e.g. Dravins \& Nordlund 1990; Asplund et al. 2000; Nissen et al. 2000; Allende Prieto et al. 2002). Since the presence of \lisix\ in the stellar atmosphere manifests itself as an asymmetry in the \lii\ 670.8\,nm line in excess of the unresolved fine structure of the \liseven\ line, it is clearly important to have an understanding of other possible mechanisms which can introduce line asymmetries, such as convection. It should be emphasized that no microturbulence or macroturbulence is necessary for the calculation of the line formation in 3D. Our final \liratio\ ratios will be taken from the 1D analysis rather than from the 3D calculations. Partly, this is due to the simple fact that 3D models do not yet exist for all combinations of stellar parameters of our sample. Another reason is that the very steep photospheric temperature gradients in 3D simulations of metal-poor stars are likely conducive to significant departures from LTE, at least for neutral minority species (Asplund et al. 1999). This has already been confirmed by detailed multi-level 3D non-LTE calculations for Li (Asplund et al. 2003; Barklem et al. 2003) which showed significant over-ionization of neutral lithium but the lithium abundance from 3D non-LTE calculations was not greatly different from 1D non-LTE calculations. Likewise, one may expect similarly large 3D non-LTE effects for many of our calibration lines of for example \fei\ and \cai\ used to determine the intrinsic atmospheric line broadening (Asplund et al. 1999; Asplund 2005). Perhaps, more important will be the line asymmetries inherent in predictions for 3D model atmospheres and which will depend somewhat on the thermodynamic conditions (LTE or non-LTE). Under these circumstances, the derived \liratio\ ratios from a 3D LTE analysis may be prone to systematic errors. While the above-mentioned 3D non-LTE studies based on only a couple of snapshots from a simulation are expected to provide a good estimate of the overall Li line {\em strength} and thus the Li abundance, predicting the detailed line {\em shape} requires taking the temporal average of many more snapshots to obtain statistically significant profiles. Unfortunately, performing 3D non-LTE calculations for long time-sequences for a stellar sample our size even for a relatively simple atom like Li is beyond reach of current computers. Therefore, the here presented 3D LTE calculations will mainly serve as a test of the 1D results for the Li isotopic ratios to assess possible systematic errors. \subsection{Atomic Data} \label{s:atomic_data} The basic data for the \lii\ 670.8\,nm resonance line is fortunately very well-known. The wavelengths for the individual hyperfine and isotope components are taken from the highly precise frequency measurements reported by Sansonetti et al. (1995), which are accurate to within 0.01\,pm (0.1\,m\AA ). The $gf$-values for the different \liseven\ and \lisix\ components are based on the calculations by Yan et al. (1998, see also Yan \& Drake 1995) that give $f=0.7467871\pm0.0000010$ and $f=0.7467527\pm0.0000010$ for the \liseven\ and \lisix\ doublets. Recent experimental values are very similar to the theoretical calculations. For example, the radiative lifetime of the $2p$ upper level ($27.11\pm0.06$\,ns) measured by Volz \& Schmoranzer (1996) is very similar to the prediction by Yan et al. ($27.117301\pm0.000036$\,ns). Our adopted wavelengths and $gf$-values are the same as in Hobbs et al. (1999) and Smith et al. (1998). The transition probabilities and wavelengths for the isotope and hyperfine components for the subordinate \lii\ 610.4\,nm were also taken from Sansonetti et al. (1995) and Yan et al. (1998). While not important for the \lii\ lines, we note for completeness that we use the accurate pressure broadening data of Barklem et al. (2000b). The transition probabilities for the lines of other species employed in the present study are taken from a variety of sources, all of which are expected to be accurate and thus not introduce any severe systematic errors. The log\,$gf$-values for the \feii\ lines are from Bi\'{e}mont et al. (1994) while those of the \fei\ lines are from O'Brian et al. (1991). Both of those should be accurate to within $\pm 0.03$\,dex. The corresponding data for the \oi\ triplet at 777\,nm comes from Wiese et al. (1996): log\,$gf = 0.369$, 0.223, and 0.002 The transition probabilities for the \cai\ lines are from Smith \& Raggett (1981) and for the \ki\ line (log$gf = -0.17$) from Reader et al. (1980). Hyperfine and isotope splitting have been taken into account for the \ki\ line although the effects turned out to be negligible. We emphasize that the exact choice of transition probability for our calibration lines used in our determination of the Li isotopic abundances is of no consequence for the determination of the line broadening in the \chitwo -analysis. The excitation potential of the lower level for the lines is taken from the NIST database while the radiative broadening comes from the VALD database. For neutral lines we rely on the pressure broadening from Barklem et al. (2000b) while for \feii\ the classical Uns\"old theory with an enhancement factor of $2.0$ has been adopted; the recent improvements in computing line broadening for \feii\ lines by Barklem \& Aspelund-Johansson (2005) only became available after our analysis was completed. We emphasize that as our \feii\ lines are all weak ($W_\lambda \la 4$\,pm), the exact treatment of the pressure broadening for these lines is of no importance for our purposes. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \section{Stellar Parameters} \label{s:parameters} \subsection{Effective Temperature} \label{s:teff} In a previous paper by Nissen et al. (2002) on oxygen abundances derived from the \oifor\ line in a subset of the same UVES spectra as employed here, the effective temperature was derived from the $b-y$ and $V-K$ colour indices calibrated on the infrared flux method (Alonso et al. 1996). The $1\sigma$ relative error of \teff\ was estimated to be about $\pm 70$\,K with the largest contribution coming from the uncertainty in the interstellar reddening $\Delta (E(b-y)) \simeq \pm 0.01$. Since it is of great importance for our discussion of the total Li abundance in the stars to obtain a higher precision of \teff , we derive here the effective temperature from the profile of the \ha\ line, which is very sensitive to temperature and practically independent of interstellar reddening. The \ha\ line is well centered in one of the echelle orders on the EEV CCD. The main problem in getting an accurate profile is to determine the echelle blaze function of the \ha\ order. The method of fitting cubic spline functions to the continuum, which works well for narrow, well isolated lines like the \lii\ line, cannnot be applied to a broad line like \ha . Hence, we made a special reduction of the \ha\ echelle order taking advantage of the fact that the blaze function varies smoothly and slowly with echelle order. This allows us to determine the blaze function of the \ha\ order by interpolating in the blaze functions of the two adjacent orders. A similar technique has been successfully applied by Barklem et al. (2002) and Korn (2002) for various echelle spectrographs, including UVES. The \ha\ profile is affected by a few metallic lines and several telluric H$_2$O lines, but due to the high resolution of the spectra these narrow absorption lines can easily be removed by interpolating the \ha\ profile over the disturbing lines. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/fig.Halpha_BD03_0740.eps}} \resizebox{\hsize}{!}{\includegraphics{f4.eps}} \caption{Observed \ha\ profile for BD\,$+03\arcdeg0740$ (dots) compared to theoretical profiles calculated for atmospheric models with the gravity and metallicity of the star (\logg\,$ = 4.04$, \feh\,$ = -2.65$) and three values of the effective temperature: \teff = 6170\,K, 6270\,K (best fit), and 6370\,K. The spectral bands used in the definition of the \ha\ index is marked.} \label{f:Halpha_BD03_0740} \end{figure} The observed \ha\ profiles have been compared to theoretical profiles computed for \marcs\ model atmospheres using the Uppsala LTE spectrum synthesis code {\sc bsyn}. Stark broadening is based on calculations of Stehl\'{e} \& Hutcheon (1999) with the model microfield method, and self-broadening of hydrogen from Barklem et al. (2000a) is included. The profiles are computed for models having the same gravity and metallicity as the star but with a range of effective temperatures embracing the value estimated from the colour of the star. An improved \teff\ is then determined from \chitwo -fitting to the observed profile (see Fig. \ref{f:Halpha_BD03_0740}). The region within $\pm 0.6$\,nm from the center is not included in the fit because the core of \ha\ is affected by deviations from LTE (Przybilla \& Butler 2004; Barklem, in preparation). Furthermore, we note that the continuum setting is considered as a free parameter in the fit, because the true continuum is ill-defined due to the limited width of the \ha\ echelle order. As an alternative to the \chitwo -fitting we have also determined \teff\ from an \ha\ index defined as the ratio between the flux in the two regions marked by `C' in Fig. \ref{f:Halpha_BD03_0740} to the flux in the regions marked by `L'. Comparison with model atmosphere calculations of the index then yields \teff . As with the \chitwo -fitting, the derived \teff\ does not depend on the continuum normalization. The two methods to determine \teff\ give consistent results within $\pm 20$\,K. We also note that the \teff\ derived for a given star from spectra observed on different nights is extremely stable with variations being less than $\pm 15$\,K. The calculated \ha\ profile is relatively insensitive to errors in the gravity and the metallicity of the models. Altogether, we estimate that {\em relative} temperatures for our sample of metal-poor turnoff stars are determined with a $1\sigma$ precision of about $\pm 30$\,K. As discussed in Sect. \ref{s:feh}, the good agreement between Fe abundances derived from \fei\ and \feii\ lines, respectively, suggests that this small error estimate is realistic. The {\em absolute} temperature scale is, however, more uncertain than $\pm 30$\,K, as it depends on the theory of hydrogen line broadening among other things. Had instead the older Ali \& Griem (1966) theory of resonance broadening been applied instead of the more complete self-broadening theory of Barklem et al. (2000a), the \teff\ derived would be raised by about 100\,K. In addition, there are uncertainties in the absolute \teff\ values of at least 100\,K arising from the current generation of 1D model atmospheres, which may not capture the effects of convection in a realistic manner. Detailed statistical equilibrium calculations for \hi\ based on available e$^-$+\hi\ and \hi +\hi\ collision cross-sections and 1D model atmospheres reveal no departures from LTE for the wings of \ha\ while the line cores are much better described (Przybilla \& Butler 2004; Barklem, in preparation). For completeness, we note that the adopted He abundance has no effect on the \ha -based \teff : a 0.2\,dex lower He abundance, as perhaps induced by elemental diffusion in the star, would only increase \teff\ by about 8\,K. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/deltaTeffvsTeff.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/deltaTeffvsFeH.eps}} \resizebox{\hsize}{!}{\includegraphics{f5a.eps}} \resizebox{\hsize}{!}{\includegraphics{f5b.eps}} \caption{Difference in \teff\ as estimated from \ha\ and from \by\ and \vk\ photometry calibrated on the infrared flux method as a function of \teff\ ({\em upper panel}) and \feh\ ({\em lower panel}). } \label{f:dteff} \end{figure} The temperatures derived from \ha\ are given in Table \ref{t:parameters}. When compared to the effective temperatures in Nissen et al. (2002, 2004) determined from $b-y$ and $V-K$ calibrated on the infrared flux method, good agreement for the majority of the stars is found: the mean difference is $\Delta T_{\rm eff} = -34 \pm 95$\,K. A few stars show large differences: the \ha -based \teff\ for G\,126-062 is 170\,K higher while for two stars (G\,020-024 and BD\,$-13\arcdeg3442$) the photometric temperatures are higher by about 200\,K. The reason for the latter is probably an overestimate of the reddening for the two stars in Nissen et al. (2002, 2004). Overall the agreement is quite satisfactory, and there are no obvious trends in the temperature differences with \teff\ or \feh , as seen in Fig. \ref{f:dteff}. We are thus unable to find any evidence from \ha\ for the very hot \teff -scale of Melend\'{e}z \& Ram\'{i}rez (2004) and Ram\'{\i}rez \& Melend\'{e}z (2005a,b) based on their reapplication of the infrared flux method. \subsection{Surface Gravity and Absolute Magnitude} \label{s:logg} The surface gravity is determined from the fundamental relation \begin{eqnarray} \log \frac{g}{g_{\sun}} & = & \log \frac{\cal{M}}{\cal{M}_{\sun}} + 4 \log \frac{T_{\rm eff}}{T_{\rm eff,\sun}} + \\ & & 0.4 (M_{bol} - M_{bol,\sun}) \nonumber \end{eqnarray} where $\cal{M}$ is the mass of the star and $M_{bol}$ the absolute bolometric magnitude. The absolute visual magnitude \mv\ is derived from the Hipparcos parallax (ESA 1997), if available, and also from Str\"{o}mgren photometry using the method and calibrations in Nissen et al. (2002, 2004). The only exception from the procedure described by Nissen et al. is that we used the spectroscopic \ha\ index (Sect. \ref{s:teff}) instead of the photometric \hb\ index to derive the interstellar reddening excess. This provides a more precise estimate of $E(b-y)$, and consequently the limit for performing a correction of the Str\"{o}mgren photometry for interstellar absorption and reddening was set at $E(b-y) > 0.010$ instead of $E(b-y) > 0.015$ in Nissen et al. (2002, 2004). If the parallax is available with an accuracy $\Delta \pi / \pi < 0.3$, the mean value of $M_{V,phot}$ and $M_{V,par}$ is adopted for \mv , otherwise $M_{V,phot}$. The bolometric correction is taken from Alonso et al. (1995), and the mass of a star is derived by comparing its position in the \mv -- \logteff\ diagram with evolutionary tracks calculated by VandenBerg et al. (2000). As the determination of \logg\ depends on \teff\ directly and \feh\ indirectly the determination of the stellar parameters has to be iterated. The final values are given in Table \ref{t:parameters} together with values for \feh\ and \oh\ (Sect. \ref{s:feh} and Sect. \ref{s:oh}) and the microturbulence \micro\ (Sect. \ref{s:broadening}). The internal error of the derived value of \logg\ is dominated by the error of \mv , which we have estimated to be $\Delta$\mv\,$ = \pm 0.20$. This corresponds to $\Delta$\logg\,$= \pm 0.08$\,dex. While the VandenBerg et al. (2000) models do not include the effects of diffusion, this translates to the surface gravity possibly being overestimated by at most 0.04\,dex (e.g. Proffitt \& Michaud 1991). We note that this effect is much too small to impact any of our conclusions in what follows. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/fig.HR.li6.lowfeh.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/fig.HR.li6.highfeh.eps}} \resizebox{\hsize}{!}{\includegraphics{f6a.eps}} \resizebox{\hsize}{!}{\includegraphics{f6b.eps}} \caption{HR-diagram for stars with \feh $< -1.7$ ({\em Upper panel}) and for stars with \feh $> -1.7$ ({\em Lower panel}). Filled circles refer to stars with a $\ge 2\sigma$ detection of \lisix , and open circles to stars with no clear detection of \lisix . The displayed evolutionary tracks are from VandenBerg et al. (2000).} \label{f:HR} \end{figure} The upper panel in Fig. \ref{f:HR} shows the \mv -- \logteff\ diagram for stars with \feh $< -1.7$ compared to two sets of evolutionary tracks from VandenBerg et al. (2000) corresponding to \feh = $-2.31$ (the mean metallicity of the stars) and $-2.01$, respectively, and an $\alpha$-element enhancement of \alphafe\ = +0.3. Except HD\,19445 (a main sequence star) and HD\,140283 (a subgiant), the stars are close to the turnoff. Some of the scatter in \teff\ around the turnoff can be attributed to differences in \feh\ with the most metal-poor stars being warmest. The lower panel of Fig. \ref{f:HR} shows the location of the eight stars with \feh $> -1.7$ in the HR-diagram. They have a mean metallicity of \feh = $-1.33$. Again all stars except perhaps HD\,106038 are classified as turnoff stars. As discussed in Sect. \ref{s:trends}, HD\,106038 has a peculiar high Li abundance. \subsection{Metallicity} \label{s:feh} Iron abundances have been determined as described in detail by Nissen et al. (2002) from 13 \feii\ lines, six of which are in our spectra. The remaining seven lines lie in the spectral region 490 - 550\,nm and were measured from UVES spectra with $R \, \simeq 55\,000$ and $S/N \, \simeq 300$ obtained with the primary aim of determining beryllium abundances (Primas et al., in preparation). For the very metal-poor stars BD\,$+09\arcdeg2190$, BD\,$+03\arcdeg0740$ and BD\,$-13\arcdeg3442$ only two of the \feii\ lines (519.76 and 523.46\,nm) could be measured reliably. For these stars, we added the somewhat stronger \feii\ 492.32\,nm line to improve the precision of \feh . For the most metal-poor star in our sample, CD\,$-33\arcdeg1173$, we do not have a spectrum in the 490 - 550\,nm region. Hence, \feh\ could not be determined from \feii\ lines, but was estimated from \fei\ lines taking into account the offset of 0.08 dex between \feh\ from \feii\ and \fei\ lines discussed below. The \feii\ lines were also measured in the solar flux spectrum (Kurucz et. al. 1984), allowing differential iron abundances \feh\ to be determined without knowledge of the exact oscillator strengths of the lines. We note that for an adopted solar iron abundance of \logfe\,$ = 7.50$, the $gf$-values derived from the solar spectrum agree well with those of Bi\'emont et al. (1991) using the {\sc marcs} solar model atmosphere. The Fe abundances for the Sun and our sample of stars were determined from the observed \feii\ line strengths using the Uppsala {\sc eqwidth} program together with 1D \marcs\ model atmospheres having the appropriate stellar parameters. As \teff , \logg\ and \feh\ are interlinked, the determination of \feh\ is an iterative procedure, with the final values listed in Table \ref{t:parameters}. The microturbulence \micro\ used in these calculations was adjusted such that the derived Fe abundances show no trend with line strength. For \feh\,$\la -2.0$, the employed \feii\ lines are weak and, hence, the derived Fe abundances are practically independent of \micro . For those stars, a microturbulence of 1.5\,\kms\ has been adopted. The error in \feh\ induced by the uncertainties in \teff\ is small: $\Delta$\feh\,$\la \pm 0.02$\,dex. Since \feii\ is the dominant ionization stage in the line formation region of these stars, the derived \feii\ based abundance is dependent on \logg : an error in \logg\ of $\pm 0.1$ translates to an error in \feh\ of $\pm 0.035$. Adding in quadrature the error indicated by the line-to-line scatter with those arising from the uncertainties in \teff\ and \logg\ implies a statistical error of $\pm 0.05$\,dex in \feh . The systematic error in \feh\ may be somewhat larger. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/deltaFevsTeff.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/deltaFevsFeH.eps}} \resizebox{\hsize}{!}{\includegraphics{f7a.eps}} \resizebox{\hsize}{!}{\includegraphics{f7b.eps}} \caption{Differences in \feh\ estimated from \feii\ and \fei\ lines as a function of \teff\ ({\em upper panel}) and \feh\ ({\em lower panel}). While there is an offset of about 0.1\,dex, there are no obvious trends with stellar parameters. This difference may signal differential non-LTE effects for \fei\ relative to the Sun or slightly too low adopted \teff\ by about 100\,K.} \label{f:fei_feii} \end{figure} In addition, we have measured Fe abundances based on up to 11 weak \fei\ lines using $gf$-values from O'Brian et al. (1991). As shown in Fig. \ref{f:fei_feii}, the \fei\ lines systematically give \feh\ values slightly lower than those from \feii\ lines. The average difference, \feiih - \feih, is 0.08\,dex with an rms scatter of only 0.041\,dex. The expected scatter arising from the adopted errors, $\Delta$\teff\,$=\pm 30$\,K and $\Delta$\logg\,$=\pm 0.08$\,dex, is 0.046 dex, i.e., not significantly different from the observed scatter. This suggests that the estimated precision of \teff\ and \logg\ is realistic. The difference in the derived Fe abundances from \fei\ and \feii\ lines could reflect departures from LTE, most likely for \fei\ (see discussion in Asplund 2005) or erroneous stellar parameters (e.g., \teff\ too low by about 100\,K). The small abundance differences and the lack of a trend in \feiih -\feih\ with either \teff\ or \feh\ is a strong argument against pronounced departures from LTE for 1D atmospheres, as claimed for example by Th\'evenin \& Idiart (1999). Our \feh\ values are systematically higher by about 0.2\,dex than those of Ryan et al. (1999) for the 11 stars in common. Ryan et al. adopted literature values of \feh\, mainly based on \fei\ lines, with a supporting role played by a calibration of medium resolution spectra. It is likely that this 0.2\,dex difference is largely attributable to the discrepancy between \fei\ and \feii\ lines mentioned above, the lower \teff -scale of Ryan et al. and/or differences in the adopted $gf$-values. Given the remaining uncertainties surrounding \fei\ lines in terms of possible departures from LTE, we believe it is wise to rely on \feii\ lines for the estimate of \feh . \subsection{Oxygen abundance} \label{s:oh} Oxygen may be a preferred alternative to iron in tracking the evolution of the lithium isotopes in the early Galaxy. Oxygen is synthesised primarily in the most massive stars and distributed when those stars explode as Type II supernovae; \liseven\ may also be made in these supernovae by the $\nu$-process (Woosley et al. 1990). Also, when spallation is an effective mode of lithium synthesis, spallation of oxygen nuclei is the dominant mechanism. Iron is also a product of Type II supernovae but in contrast to oxygen its yield is dependent on the mass cut between the stellar remnant (neutron star or black hole) and the ejecta and iron is also a product of Type Ia supernovae. The latter factor is not a major concern here as our stars have a metallicity below that at which Type Ia supernovae are generally considered to begin their contributions. The O abundances for our program stars have been derived from the \oi\ triplet at 777\,nm. Unfortunately, the alternative abundance indicator, the \oifor\ line at 630\,nm, is undetectable for \feh\,$\la -2.5$, even with the very high $S/N$ of our spectra. We have, therefore, opted for using the same diagnostic for the entire sample. The \oi\ triplet typically yields somewhat higher O abundances than the forbidden \oifor\ line at low metallicity (see discussion in Asplund 2005 and references therein). The \oi\ 777.1, 777.4 and 777.5\,nm lines are located towards the edges of two consecutive echelle orders from which the equivalent widths were measured and averaged (weighted by their respective $S/N$). The results for the July 2000 spectra have already been presented in Nissen et al. (2002) to which we now add nine stars from February 2002. From the equivalent widths the 1D LTE O abundances were derived using the stellar parameters listed in Table \ref{t:parameters}; it should be noted that the O abundances for the July 2000 targets differ slightly from those given in Nissen et al. (2002) due to our use of \ha -based \teff\ rather than the photometric values employed in our previous study. We have also computed 1D non-LTE abundance corrections for the \oi\ triplet lines in an identical fashion to the calculations presented in Nissen et al. (2002). These non-LTE corrections are always negative and typically $-0.1...-0.2$\,dex but reach $-0.3$\,dex at the lowest \feh . Our final adopted O abundances given in Table \ref{t:parameters} include these non-LTE corrections. These abundances are referenced relative to the same solar O abundance from a 1D solar model atmosphere as adopted in Nissen et al. (2002), i.e. \logo\,$=8.74$, which is 0.08\,dex higher than the current best estimate based on 3D hydrodynamical model atmospheres (Asplund et al. 2004, 2005). Nissen et al. (2005a) have discussed in some detail the trend and scatter of \ofe\ as a function of \feh\ for our sample. Here we just note that \ofe\ increases from about 0.4~dex at \feh\ = $-1.0$ to 0.6~dex at \feh\ = $-3.0$. The scatter in \ofe\ around a linear fit to the data (\ofe = $-0.11$\,\feh\ + 0.31) is 0.08~dex with a large contribution coming from a relatively low \ofe\ in HD\,160617, a star that is known to belong to the rare class of nitrogen-rich subdwarfs (Bessell \& Norris 1982). \subsection{Spectral Line Broadening} \label{s:broadening} In order to extract the lithium isotopic ratio from the profile of \lii\ 670.8\,nm line, it is paramount to have an accurate understanding of the intrinsic spectral line broadening. This broadening comes in various forms all of which must be taken into account: thermal, pressure, radiative, rotational and Doppler broadening. Thermal broadening can be directly computed from the known temperature structure of the stellar atmosphere while the pressure and radiative broadening are, in principle at least, known atomic properties specific for each transitions. It is well-known that the observed spectral lines are always broader than predicted solely from the thermal and atomic broadening. All stars are expected to rotate, which broadens the line profiles but does not modify the line strength. As our observations are unable to disentangle readily rotational broadening from other atmospheric broadening agents, we adopt in all cases \vsini\,$=0.5$\,\kms\ given the great age of these metal-poor halo stars (for comparison, the Sun has \vrot\,$=1.8$\,\kms\ at the equator). We have confirmed that our derived results are immune to this particular choice of \vsini . In addition, atmospheric velocity fields from convection, wave motion, turbulence and the like introduce Doppler shifts which affect the line profiles. In analyses based on 1D hydrostatic model atmospheres, one normally introduces two free parameters: microturbulence \micro\ and macroturbulence \macro , acting on small and large spatial scales, respectively. Following standard practice we determine \micro\ by ensuring that the derived abundances from \fei\ and \feii\ lines are independent of line strength while \macro\ is estimated from the observed line shapes. The form of \macro\ is assumed to be Gaussian. This choice was made mainly for convenience as the effects of \macro\ can then be easily combined with the line broadening due to the finite instrumental resolution which is also described by a Gaussian distribution. We have performed various tests ensuring that our results in terms of Li isotopic abundances are not affected by the use of a Gaussian \macro\ instead of, for example, a radial-tangential version (e.g. Gray 1992). The lines used for determining \macro\ were \ki\ 769.9\,nm, \cai\ 612.2\,nm, \cai\ 616.2\,nm, \cai\ 643.9\,nm, \fei\ 623.0\,nm, \feii\ 624.7\,nm and \feii\ 645.6\,nm. In some cases we also added the \fei\ 610.2\,nm and \fei\ 613.6\,nm lines when there was a lack of calibration lines of suitable strength compared with the \lii\ line. For the August 2004 observations of LP\,815-43 and HD\,140283, additional lines could be used since the spectra extended further to the blue, enabling the \feii\ 501.8\,nm, \fei\ 523.3\,nm, \fei\ 532.4\,nm, \fei\ 539.7\,nm, \fei\ 538.3\,nm, \fei\ 543.4\,nm, \fei\ 542.4\,nm, \mgi\ 552.8\,nm, \fei\ 561.2\,nm, \cai\ 558.9\,nm and \fei\ 558.7\,nm lines to be covered in exchange for the \ki\ 769.9\,nm line. The \ki\ line was broader than other lines, such as \fei\ 623.0\,nm, of comparable strength in most stars. This may signal significant departures from LTE which have indeed been predicted for this resonance line for metal-poor stars (Ivanova \& Shimanskii 2000; Takeda et al. 2002). Good agreement was found, however, when the \ki\ line had an equivalent width of about 2\,pm, i.e., similar to that of the \lii\ line itself. This is consistent with the finding of Smith et al. (2001) in the case of HD\,84937. We, therefore, decided not to include this line in the final estimates of \macro\ and used it only as a consistency check on the mean value and scatter implied by the other lines. When computing the average broadening parameters from the calibration lines, we have considered only lines with strengths $0.9 \le W_\lambda \le 7.5$\,pm. The calibration lines included in the computation of the mean broadening are of similar line strength to the \lii\ 670.8\,nm line, which should minimize possible systematic differences. This point is important since we have noticed that the derived \macro\ is dependent on the strength of the line, as illustrated in Fig. \ref{f:FWHM} for the case of HD\,106038 (a Li-rich star with a significantly stronger \lii\ 670.8\,nm line than in the typical star of our sample: $W_\lambda = 6.32$\,pm rather than $\approx 2$\,pm). In this particular instance, \macro\ was computed as a mean of the four lines with $W_\lambda = 6\pm1$\,pm, which is expected to give a good estimate of the intrinsic broadening for the \lii\ line. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \section{Li Isotopic Abundances from the \lii\ 670.8\,nm Resonance Line} \label{s:li6708} \subsection{Li Isotopic Abundances} \label{s:li6708_chi2} The presence of \lisix\ alongwith \liseven\ in the stellar atmosphere introduces additional width and asymmetry of the line profile\footnote{We will not consider here the center-of-gravity method which is based on the wavelength shift introduced by the addition of \lisix . The nearby \cai\ 671.7\,nm line has served as a reference line. As discussed by Smith et al. (1998) and Cayrel et al. (1999), the presence of differential line shifts arising from convection (see, for example, Reddy et al. 2002), and the remaining uncertainties in the laboratory wavelength of the \cai\ line render this method very prone to systematic errors.}. As outlined in Sect. \ref{s:broadening}, we first determine \macro\ from a number of \ki , \cai , \fei\ and \feii\ lines. This is achieved by a \chitwo -analysis of the predicted and observed line profiles allowing the element abundance, wavelength zero-point and continuum normalization to vary besides \macro . In most cases, \macro\ could be well determined with a standard deviation of $\Delta$\macro$=\pm0.1-0.2$\,\kms . Larger uncertainties of $\pm 0.3-0.6$\,\kms\ resulted for four stars: G\,126-062, CD\,$-33\arcdeg1173$, HD\,59392 and BD\,$+09\arcdeg2190$. The estimated broadening parameters are listed in Table \ref{t:li_abundances}, while Figs. \ref{f:li6708_HD140283}--\ref{f:li6708_LP815-43} show the resulting profiles for one of these calibration lines (\cai\ 612.2\,nm) for a few stars. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/FWHMvsWlam_HD106038.eps}} \resizebox{\hsize}{!}{\includegraphics{f8.eps}} \caption{Estimated macroturbulence \macro\ (assumed to be described by a Gaussian) from different lines of varying strengths in HD\,106038; in addition the lines were broadened by rotation (assumed to be \vsini\,$=0.5$\,\kms ) and instrumental broadening (measured from Th lines). Note the strong correlation between \macro\ and equivalent width, which emphasizes the importance of having calibration lines of similar strengths as the \lii\ 670.8\,nm line when estimating the intrinsic line broadening. The equivalent width for the Li line in HD\,106038 is denoted by the vertical dotted line.} \label{f:FWHM} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/CaI6122.2_final_HD140283_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_final_HD140283_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI_chi2_final_HD140283.eps}} \resizebox{\hsize}{!}{\includegraphics{f9a.eps}} \resizebox{\hsize}{!}{\includegraphics{f9b.eps}} \resizebox{\hsize}{!}{\includegraphics{f9c.eps}} \caption{{\em Upper panel:} Observed \cai\ 612.2\,nm profile (rhombs) in HD\,140283 together with the best fit theoretical 1D LTE profile (solid line). Also shown are the predictions with the macroturbulence \macro\,$\pm0.5$\,\kms . The Gaussian FWHM is here the combination of \macro\ and the instrumental broadening; the profiles have also been convolved with a stellar rotation velocity of \vrot\,$=0.5$\,\kms . {\em Middle panel:} Computed \lii\ 670.8\,nm profile for three different values for \liratio\ (0.00, 0.05 and 0.10) shown together with the observed line (rhombs). In each case, the Li abundance, wavelength shift and continuum level have been allowed to vary. The location of the various \liseven\ and \lisix\ components are indicated. {\em Lower panel:} Resulting $\Delta$\chitwo\ for the combined Gaussian of the mean \macro\ and instrumental broadening; also shown are the cases for \macro\,$\pm \Delta$\macro . In this star, no significant detection of \lisix\ can be claimed.} \label{f:li6708_HD140283} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/CaI6122.2_final_G013-009_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_final_G013-009_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI_chi2_final_G013-009.eps}} \resizebox{\hsize}{!}{\includegraphics{f10a.eps}} \resizebox{\hsize}{!}{\includegraphics{f10b.eps}} \resizebox{\hsize}{!}{\includegraphics{f10c.eps}} \caption{Same as Fig. \ref{f:li6708_HD140283} but for G\,013-009. In this star, the \chitwo -analysis indicate a $>2\sigma$ detection of \lisix\ at the level of \liratio\,$=0.05$. } \label{f:li6708_G013-009} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/CaI6122.2_final_G020-024_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_final_G020-024_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI_chi2_final_G020-024.eps}} \resizebox{\hsize}{!}{\includegraphics{f11a.eps}} \resizebox{\hsize}{!}{\includegraphics{f11b.eps}} \resizebox{\hsize}{!}{\includegraphics{f11c.eps}} \caption{Same as Fig. \ref{f:li6708_HD140283} but for G\,020-024. In this star, the \chitwo -analysis indicate a $4\sigma$ detection of \lisix\ at the level of \liratio\,$=0.07$. } \label{f:li6708_G020-024} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/CaI6122.2_august-sky_no6162_LP815-43_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_august-sky_no6162_LP815-43_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI_chi2_august-sky_no6162_LP815-43.eps}} \resizebox{\hsize}{!}{\includegraphics{f12a.eps}} \resizebox{\hsize}{!}{\includegraphics{f12b.eps}} \resizebox{\hsize}{!}{\includegraphics{f12c.eps}} \caption{Same as Fig. \ref{f:li6708_HD140283} but for LP\,815-43. In this star, the \chitwo -analysis indicate a $2\sigma$ detection of \lisix\ at the level of \liratio\,$=0.05$. The observed spectrum shown here is the one from August 2004.} \label{f:li6708_LP815-43} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/Li6Li7vsTeff.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/Li6Li7vsFeH.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/Li6Li7_histogram.eps}} \resizebox{\hsize}{!}{\includegraphics{f13a.eps}} \resizebox{\hsize}{!}{\includegraphics{f13b.eps}} \resizebox{\hsize}{!}{\includegraphics{f13c.eps}} \caption{Derived \liratio\ as a function of \teff\ ({\em Upper panel}) and \feh\ ({\em Middle panel}). The stars considered to have a significant detection ($\ge 2\sigma$) of \lisix\ are shown as solid circles while non-detections are plotted as open circles. Note that the non-detections do not cluster around \liratio\,$=0.00$ but rather at $\approx 0.01$. This is also illustrated as a histogram ({\em Lower panel}). The observed distribution is clearly not representative of a Gaussian centered at \liratio\,$=0.00$.} \label{f:li6708_summary} \end{figure} Equipped with the estimate of the macroturbulence \macro\ for each star, the adopted \vsini\ (0.5\,\kms ) and the measured instrumental broadening at 670.8\,nm from Th lines, synthetic profiles of the \lii\ 670.8\,nm line for different Li isotopic ratios were generated for the program stars using the stellar parameters listed in Table \ref{t:parameters}. Calculations were done for \liratio\ between $-0.10$ and $0.10$ by step of $0.01$. Negative \liratio\ ratios, of course, do not exist in reality but were included in order to obtain estimates as accurate as possible for stars with very small or vanishing \lisix\ content. These were produced by allowing the \lisix\ components of the \lii\ 670.8\,nm line to be in emission rather than in absorption as is the case for positive \liratio\ ratios. At the low metallicity of the program stars, one does not need to worry about potential blends from various atomic and molecular lines that can perturb the Li feature at solar metallicity (Nissen et al. 1999; Israelian et al. 2001, 2003; Reddy et al. 2002) and we thus computed the theoretical profile taking into account only the various components of the Li line. Test calculations revealed that this was fully justifiable for the target stars. The comparison between the theoretical and observed profiles was quantified using a \chitwo -analysis similar to that used in most recent investigations of \liratio\ in late-type stars (e.g. Smith et al. 1998; Nissen et al. 1999, 2000; Israelian et al. 2001, 2003; Reddy et al. 2002; Aoki et al. 2004). The \chitwo\ was computed according to \chitwo\,$=\sum \left(O_{\rm i}-S_{\rm i}\right)^2/\sigma^2$, where $O_{\rm i}$ and $S_{\rm i}$ denote the observed and synthetic flux at wavelength point $i$, respectively, and $\sigma = \left(S/N\right)^{-1}$ as estimated in three nearby continuum windows. Typically 26 wavelength points were considered across the Li line to estimate \chitwo . For each \liratio , the total Li abundance, the wavelength zeropoint of the observed spectrum and the continuum level were allowed to vary in order to optimize the fit and thus minimize \chitwo . The most probable value for \liratio\ was obtained by cubic spline interpolation of the resulting \chitwo\ values, from which the minimum \chitwomin\ could be determined. The $1\sigma$, $2\sigma$ and $3\sigma$ confidence limits of the determinations correspond to $\Delta \chi^2 = \chi^2 - \chi^2_{\rm min} = 1, 4$ and 9, respectively. These uncertainties are determined by the noise of the spectra, which as mentioned above are better than $S/N > 500$ for all but two stars that have 400 and 470, respectively. The reduced $\chi^2_{\rm r}$ is in all cases close to one with the variations between stars as expected from statistical fluctuations. In addition, the \chitwo -analysis was repeated for each star with different adopted macroturbulence parameters, $\zeta_{\rm macro} \pm \Delta \zeta_{\rm macro}$, where $\Delta \zeta_{\rm macro}$ was given by the standard deviation from the various Ca and Fe lines. Examples of the observed and predicted \lii\ line profiles and the corresponding \chitwo\ values can be found in Figs. \ref{f:li6708_HD140283}--\ref{f:li6708_LP815-43} for a few stars. The resulting \liratio\ ratios and \liseven\ abundances are listed in Table \ref{t:li_abundances}. The errors in the derived \liratio\ ratios are quantified by taking the uncertainties from the finite $S/N$ as well as the adopted \macro\ and stellar parameters in quadrature. In essentially all cases, the first source dominates the error budget in spite of the extremely high $S/N$ achieved in these observations, but for a couple of stars with poorly determined \macro\ such as CD\,$-33\arcdeg$1173 the second uncertainty drives the final error. The errors arising from the uncertainties in the stellar parameters are in all cases very minor, as discussed in detail in Sect. \ref{s:li6708_parameters}. We note that our error estimates are slightly more conservative than previous studies of the Li isotopic ratios in metal-poor stars, which, for example, often have relied on only one or two calibration lines to determine the line broadening. As seen in Table \ref{t:li_abundances}, nine of the 24 stars fulfill our criteria of a $\ge 2\sigma$ result to be considered a significant \lisix\ detection: HD\,102200, HD\,106038, HD\,160617, G\,013-009, G\,020-024, CD\,$-30\arcdeg$18140, CD\,$-33\arcdeg$3337, CD\,$-48\arcdeg$2445 and LP\,815-43. This should be contrasted with the previous single confirmed detection of \lisix\ in HD\,84937 (Smith et al. 1993, 1998; Hobbs \& Thorburn 1997; Cayrel et al. 1999). The stars with detected \lisix\ are all very near the turn-off for their respective metallicities (Fig. \ref{f:HR}), in accordance with the suggestion of Smith et al. (1993, 1998). In addition, we find a large number of borderline cases at the $1-2\sigma$ level that we do not consider significant enough to claim a positive detection. In fact, there is a tendency for the non-detections to cluster at \liratio\,$\approx 0.01$, as illustrated in Fig. \ref{f:li6708_summary}. This could be taken as a warning sign that our analysis contains an unidentified systematic error that bias the derived isotopic ratio towards too high values. We have therefore carried out tests in an attempt to identify such a problem, which are described in detail in the following subsections. In summary, no serious problem that could affect our analysis has been uncovered: no differences are found when taking into account possible ISM absorption in the Li line (Sect. \ref{s:li6708_lp815}), adopting an alternative \chitwo -analysis (Sect. \ref{s:li6708_chi2_cayrel}), changing the stellar parameters within reasonable bounds (Sect. \ref{s:li6708_parameters}), employing a different suite of 1D model atmospheres (Sect. \ref{s:li6708_kurucz}) or using 3D hydrodynamical model atmospheres (Sect. \ref{s:li6708_3D}). Furthermore, we independently obtain the same results as some previous investigations when relying on their observations (Sect. \ref{s:li6708_literature}). Finally, our confidence in the derived results is boosted by the analysis of HD\,19445, which was included in our program to provide a consistency check (see, also, Smith et al. 1993). Since this star is a relatively cool (\teff\,$=5980$) metal-poor dwarf (\logg\,$=4.42$), standard models of stellar evolution predict that \lisix\ should be thoroughly destroyed on the star attaining the main sequence (see discussion in Sect. \ref{s:depletion}). Indeed, an analysis identical to that for all of our other stars indicate no presence of \lisix : \liratio\,$=0.002\pm0.008$. We conclude that the Li isotopic ratios presented in Table \ref{t:li_abundances} are reliable. We claim significant \lisix\ detections only in the above-mentioned nine stars, but we can not rule out the possibility that the majority of turn-off halo stars in fact have \liratio\,$\approx 0.01$ (Fig. \ref{f:li6708_summary}). To confirm an isotopic ratio as low as 0.01 for an individual star is extremely challenging (c.f. our analysis of HD\,140283 with $S/N \approx 1000$), but confirmation should be attemptable in at least a statistical sense for a sample like ours but with even higher $S/N$ spectra and additional calibration lines to nail down the line broadening accurately. The Li abundances derived from the profile fitting of the \lii\ 670.8\,nm line have been obtained under the assumption of LTE. We have applied the non-LTE abundance corrections computed by Carlsson et al. (1994) interpolated to the stellar parameters of our sample to the LTE Li abundances. These non-LTE calculations are particularly appropriate as they have been performed using similar \marcs\ model atmospheres as employed here. The resulting non-LTE \liseven\ abundances are given in Table \ref{t:li_abundances}. The non-LTE abundance corrections are in all cases very small ($\Delta$\logli$\la 0.02$\,dex) and generally negative. The scatter in Li abundances is not significantly modified by the application of these non-LTE corrections. \subsection{Is the High \liratio\ in LP\,815-43 Real?} \label{s:li6708_lp815} Due its low \feh , LP\,815-43 will feature prominently in the discussions in Sect. \ref{s:evolution}. It is natural to inquire whether its high \lisix\ abundance determined from our \chitwo -analysis is real. We note that both the spectrum of LP\,815-43 obtained in July 2000 and that acquired in August 2004 imply a detection of \lisix\ at the $2\sigma$ level or more. The former indicated \liratio\,$=0.078\pm0.033$ based on an observed spectrum with $S/N=540$ but with only three \cai\ lines to estimate the intrinsic line broadening. This result prompted us to request additional observing time for this star to improve the $S/N$ and include more calibration lines. The combined spectrum from two nights in August 2004 has $S/N=630$ as well as covering as many as 10 calibration lines of the right strength which importantly beat down the uncertainty in the macroturbulence to $0.19$\,\kms . The resulting isotopic ratio is slightly less but still implies a significant detection by our criteria: \liratio\,$=0.046\pm0.022$. The result from the July 2000 spectrum is fully consistent with this improved value taking the uncertainties into account. The individual spectra obtained on August 30 and 31, 2004, have $S/N = 420$ and 490, respectively. Both of these imply \liratio\,$\approx 0.03-0.04$ but each allows only a $1\sigma$-detection due to the reduced $S/N$. Finally, we note that had we adopted the better determined macroturbulence value from the August 2004 spectrum for the analysis of the July 2000 spectrum, the derived \liratio\ would have increased to $0.089\pm0.027$, i.e. a $3\sigma$-detection. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_obs_LP815-43_1.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_obs_LP815-43_2.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_obs_LP815-43_3.eps}} \resizebox{\hsize}{!}{\includegraphics{f14a.eps}} \resizebox{\hsize}{!}{\includegraphics{f14b.eps}} \resizebox{\hsize}{!}{\includegraphics{f14c.eps}} \caption{Enlargement of the August 2004 spectrum of LP\,815-43 around the \lii\ 670.8\,nm line. Note that the spike at 670.655 is a cosmic ray hit. Also shown with a dashed line is the predicted contribution of \lisix\ to the \lii\ 670.78\,nm line for \liratio\,$=+0.05$.} \label{f:LiI6708_obs_LP815-43} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_obs_LP815-43_random0.50.eps}} \resizebox{\hsize}{!}{\includegraphics{f15.eps}} \caption{Histogram of the measured equivalent widths over a 0.08\,nm window in the continuum near the \lii\ 670.8\,nm line for the August 2004 spectrum of LP\,815-43 (solid line). Also shown is the same distribution for pure random noise with the same $S/N$ (630) as the observed spectrum (dotted line). The dashed line shows the distribution of equivalent widths for the random noise spectrum with an added sinusoidal component of amplitude 0.05\% (see text for details). The similarity with the observed distribution suggests the presence of residual fringing at the 0.05\% level for this star while fringing at the 0.1\% level can be ruled out (not shown).} \label{f:LiI6708_obs_LP815-43_histogram} \end{figure} As described in Sect. \ref{s:reduction}, there may be residual fringing in the reduced spectrum at the level of $<0.1$\% of the continuum level with a typical wavelength scale of 0.1-0.2\,nm. If it is as high as $0.1$\% and one of those depressions falls on top of the Li line, it could mean that the \liratio\ has been overestimated. An ad-hoc adjustment of the local continuum level by this amount would change \liratio\ for LP815-43 to only a $1\sigma$ detection and thus not significant by our standards (of course if instead of a depression there is a peak in the residual fringing it would increase \liratio\ by the corresponding amount). This illustrates clearly the challenges posed by this method to determine the Li isotopic ratio in metal-poor turn-off stars. An enlargement of the observed August 2004 spectrum is shown in Fig. \ref{f:LiI6708_obs_LP815-43}. While there may be hints of a residual fringing at some wavelengths, there are no traces thereof in other parts of the spectrum near the Li line. We have tried to quantify the amount of fringing by computing the equivalent width directly integrated over a 0.08\,nm window (the width of the Li line) along the echelle order with the Li line. The wavelength variation of these equivalent width measurements is slightly more pronounced than expected from pure random noise with the same $S/N$, suggesting the presence of fringing with a quasi-regular wavelength dependence. Adding a sinusoidal component with an amplitude of 0.05\% and wavelength scale of about 0.17\,nm to such pure random noise produces a similar equivalent width distribution to that observed in August 2004, as shown in Fig. \ref{f:LiI6708_obs_LP815-43_histogram}; fringing as large as 0.1\% can clearly be ruled out. A similar exercise for the July 2000 spectrum suggests residual fringing with an amplitude of 0.08\%. It can also be noted that the expected \lisix\ contribution to the equivalent width (0.1\,pm for \liratio\,$=+0.046$) is very unlikely to be produced purely by chance as the observed equivalent width distribution of the nearby continuum have a typical uncertainty of 0.03\,pm, consistent with our claimed $2\sigma$ detection for this star. We stress that the presence of fringing at the 0.05\% level does not automatically imply that our derived \liratio\ for this star is overestimated as it also requires that a fringing depression rather than a peak falls on top of the Li line, something we are not able to evaluate the likelihood of. The fact that independent observations acquired in 2000 and 2004 both yield a significant presence of \lisix\ in the star increases our confidence that our \lisix\ detection in this star is real. We nevertheless strongly encourage further observations of this star to confirm our conclusions. A further concern in the analysis of LP\,815-43 is that lithium interstellar (ISM) absorption line may mimic the presence of \lisix\ considering that the \ki\ 769.8\,nm is clearly distorted by a {\em blue-shifted} ($-2.07$\,\kms ) ISM line. Welty \& Hobbs (2001) found in their survey of ISM absorption that $N$(\lii )/$N$(\ki )\,$= 0.0054$. Together with the difference in $gf$-values of the two resonance lines, the ISM \lii\ profile should be about 100 times weaker than the corresponding ISM \ki\ line. The ISM \ki\ line has a line depth of about 8\% and an equivalent width of 0.97\,pm. The ISM \lii\ line should, therefore, have an equivalent width of less than 0.01\,pm (0.1\,m\AA ). It is, therefore, unlikely that an ISM lithium line will have a significant influence on the derived \liratio . To quantify the above estimates, we first subtracted from the \ki\ 769.8\,nm profile the expected stellar \ki\ line as predicted using an K abundance similar to the other four stars with similar \feh\ and \macro\ and \vrad\ from the \cai\ and \fei\ lines. We then fitted a Gaussian to this ISM \ki\ profile, which was subsequently converted to a corresponding ISM \lii\ profile while taking into account the hyperfine structure of the Li line and the difference in overall line strength. The difference in line width of the Gaussians due to different thermal broadening of Li and K was also included. After subtraction of this blue-shifted ISM profile, we again performed a \chitwo -analysis of the remaining stellar \lii\ line. As expected from the above estimates, the resulting \liratio\ was indistinguishable from the previous value. We conclude that our derived high \liratio\ is not an artifact of ISM Li absorption. \subsection{Estimating Uncertainties Using Monte Carlo Calculations} \label{s:monte_carlo} As an independent means of estimating the uncertainties attached to our Li isotopic abundance analysis, we have carried out extensive Monte Carlo simulations for HD\,140283. A theoretical profile of the \lii\ 670.8\,nm line with an adopted \liratio\,$=0.02$ was treated as an observed line, to which noise corresponding to various $S/N$ values (400, 500, 600, 700, 800, 900 and 1000) were added. All line profiles were convolved with a Gaussian of width 5\,\kms\ and projected stellar rotational velocity of 0.5\,\kms\ prior to introducing the effects of finite $S/N$. These artificial observed lines had the same wavelength sampling as our UVES spectra. We then performed a \chitwo -analysis of these profiles in an identical fashion as for our real observations with the exception that the line broadening parameters were assumed to be known beforehand. For each $S/N$, 100 realisations of the noisy synthetic profile were generated and exposed to the \chitwo -analysis. The scatter in the estimated \liratio\ gives an estimate of the accuracy with which the isotopic ratio can be determined for a given $S/N$. To these uncertainties should still be added the possible errors arising from uncertainties in the line broadening, continuum placement and stellar parameters. The estimated \liratio\ deviated from the input value with a standard deviation of 0.010, 0.007, 0.005 and 0.004 for $S/N = 400$, 600, 800 and 1000, respectively. These estimates are consistent with the \chitwo\ results using the true observed profile for this star when ignoring the uncertainty stemming from the estimated errors in the adopted macroturbulence and stellar parameters. We conclude that the error estimates in Sect. \ref{s:li6708_chi2} are indeed realistic. \subsection{Effects of Choice of a \chitwo\ Analysis} \label{s:li6708_chi2_cayrel} In their analysis of the Li isotopic ratio in HD\,84937, Cayrel et al. (1999) adopted a slightly different technique than the one employed by us. Rather than determining the intrinsic line broadening due to macroturbulence and rotation from lines of other species, they introduced this as an additional free parameter in the \chitwo -analysis of the \lii\ 670.8\,nm line. Only after the analysis did they confirm that the derived broadening parameter was consistent with values estimated from the \cai\ 616.2 and 671.7\,nm lines. The \liratio\ ratio Cayrel et al. obtained for this star ($0.052\pm0.019$ at $1\sigma$) is in agreement with the value ($0.06\pm0.03$ at $1\sigma$) of Smith et al. (1998) from an independent observational data set. Smith et al. used the same approach as us but with fewer calibration lines. We have investigated how our conclusions would be modified by employing Cayrel et al.'s approach for our full sample. Our results are reasonably unchanged by adopting this alternative approach. Only in six of our 24 stars is the derived \liratio\ ratio changed by more than $\pm 0.02$. Of our nine detections at the $\ga 2\sigma$ level, seven (HD\,102200, HD\,106038, HD\,160617, G\,020-024, CD\,$-30\arcdeg18140$, CD\,$-33\arcdeg3373$, LP\,815-43) are still detections under the same criterion. While G\,013-009 and CD\,$-48\arcdeg2445$ would no longer be significant detections, three other stars would in this framework be classified as $\ga 2\sigma$ detections: HD\,213657, HD\,298986 and BD\,$+03\arcdeg0740$, which otherwise were only $1\sigma$ results. BD\,$+03\arcdeg0740$ (\feh\,$=-2.65$) is noteworthy given its low \feh . We believe that Cayrel et al.'s method is inferior to ours as it does not make full use of the information content in the observed spectra. Due to the limited wavelength coverage of their spectra, Cayrel et al. had access to only two calibration lines (\cai\ 616.2 and 671.7\,nm) which in HD\,84937 are of quite different strength compared with the Li line. Under those circumstances it may be justified to allow also the broadening parameters to vary in the \chitwo -analysis of the \lii\ 670.8\,nm profile when the $S/N$ is very high as in their spectrum. One of the great advantages of the VLT/UVES is the wide wavelength coverage that provides several lines for estimating the intrinsic line broadening. We also note that the uncertainties in the estimated \liratio\ ratios are in general larger when Cayrel et al.'s method is used in place of our standard analyis presented in Sect. \ref{s:li6708_chi2}, in some cases significantly so (e.g. BD\,$-13\arcdeg3442$: \liratio$=0.001\pm0.028$ and $0.042\pm0.050$, respectively), while in no case was the uncertainty reduced. We conclude that the method of Cayrel et al. is less appropriate than the one employed in the present study. Nevertheless, our results would have been quite similar had we adopted this approach. \subsection{Effects of Choice of Stellar Parameters} \label{s:li6708_parameters} As described in Sect. \ref{s:parameters}, the estimated uncertainties in the adopted stellar parameters in absolute terms are $\Delta$\teff$=\pm100$\,K, $\Delta$\logg$=\pm0.2$, $\Delta$\feh$=\pm0.2$ and $\Delta$\micro$=\pm0.2$\,\kms . We have repeated our Li isotopic abundance determinations for all stars using \marcs\ model atmospheres with modified stellar parameters by deriving new line broadening parameters and then repeating the \chitwo -analysis of the \lii\ 670.8\,nm profile. The resulting \liratio\ ratios when changing the stellar parameters by $+100$\,K, $+0.2$\,dex and $+0.5$\,\kms , respectively, are given in Table \ref{t:li_parameters}. Clearly, the \liratio\ ratios are basically immune to the uncertainties at this level in the stellar parameters: the slightly different line broadening parameters derived from the calibration lines also apply to the \lii\ line, leaving \liratio\ essentially intact. Very rarely is $\Delta$\liratio\ as large as 0.003 with the difference being $\le 0.001$ in the majority of cases. This finding is in line with those reported previously by Smith et al. (1993, 1998). While the effects of the uncertainties in \logg , \feh\ and \micro\ are negligible for the derived \liseven\ and \lisix\ absolute abundances ($\Delta$\logli$<\pm 0.01$\,dex for our estimated stellar parameter uncertainties), this is not true when changing \teff . Our calculations reveal that \logli\ increases with about 0.073\,dex for $\Delta$\teff$=+100$\,K, necessarily quite similar to the estimate by Ryan et al. (1999). \subsection{Effects of Choice of Suite of 1D Model Atmospheres} \label{s:li6708_kurucz} The tendency for our derived \liratio\ ratios to be slightly but positively offset from zero, may raise concern that our analysis suffer from an unidentified systematic error. One possibility could be our use of \marcs\ model atmospheres, since Nissen et al. (1999) found a {\em smaller} isotopic ratio (0.033 instead of 0.041) for the disk star HD\,68284 when switching from a \marcs\ to a Kurucz model atmosphere with identical stellar parameters. To investigate whether the choice of suite of 1D model atmospheres has any effect on the derived Li isotopic abundances, we have repeated the analysis for all stars using Kurucz model atmospheres without convective overshoot and for the same stellar parameters, as computed by Castelli et al. (1997). The resulting \liratio\ ratios are presented in Table \ref{t:li_parameters} together with the corresponding values with \marcs\ model atmospheres. The changes to the isotopic ratios resulting from substitution of the Kurucz for the \marcs\ models are, as anticipated, negligible: $\Delta$\liratio$\le \pm 0.001$ and in no case larger than 0.003. Furthermore, the small differences can be both positive and negative. Similarly, the effect of the Kurucz models on the absolute Li abundances is marginal\footnote{Differences in absolute Li abundances approaching 0.1\,dex would have been found had we resorted to the convective overshoot models of Kurucz (1993) instead of using the models with this option switched off (Ryan et al. 1996). These overshoot models are, however, significantly less successful in reproducing observed stellar flux distributions and their shallower temperature gradients find no support in our detailed 3D hydrodynamical simulations of stellar atmospheres with surface convection. We conclude that the overshoot models are less appropriate for abundance analyses of halo stars.}. The average difference compared with the \marcs\ based results is $\Delta$\logli$ = 0.015\pm0.018$\,dex with the maximum difference being 0.048 for HD\,102200. For completeness, we note that the above test is based on the assumption that the stellar parameters of the model atmospheres need no adjustments when switching to a different suite of model atmospheres. Given the almost identical behaviour of our \lii , \ki, \cai , \fei\ and \feii\ lines in the two cases, we expect insignificant differences for both the photometric calibrations or the \ha\ line profile fitting. In summary, our conclusions about the lithium isotopic ratio are immune and the lithium abundance insensitive to the particular brand of theoretical 1D, hydrostatic, LTE model atmospheres employed in the analysis. \subsection{Effects of 3D Hydrodynamical Model Atmospheres} \label{s:li6708_3D} In addition to the tests described above, we have also performed a similar \chitwo -analysis using the time-dependent 3D hydrodynamical model atmospheres described in Sect. \ref{s:model_atmospheres} under the assumption of LTE. Since such 3D models still only exist for relatively few stellar parameter combinations, only some of our target stars could be exposed to a 3D analysis. The 3D models assigned to the various stars were based on similarity in stellar parameters; we note therefore that the here presented 3D results are obtained with somewhat different stellar parameters than adopted for the 1D calculations described in Sect. \ref{s:li6708_chi2}. As explained in Sect. \ref{s:line_formation}, the main advantages with a 3D approach is that neither micro- nor macroturbulence enter the analysis and that the intrinsic line asymmetries arising from convective motions follow directly from the 3D line formation calculations. The projected stellar rotation velocity \vsini\ must however be determined from other lines. Thus, in the \chitwo -analysis, \vsini\ replaces \macro\ as a free variable; the Gaussian instrumental broadening measured for each line is known from Th lines. The results for the stars for which a 3D analysis has been carried out are given in Table \ref{t:li6_3D}, while Fig. \ref{f:ca6162_3D_1} and Fig. \ref{f:ca6162_3D_2} show examples of the achieved profile fits for the \cai\,616.21 lines for a few of the stars. It is noteworthy that the 3D analysis yields a substantial improvement in the agreement with the observed profiles of Ca and Fe lines, as also previously reported by Nissen et al. (2000). In almost all cases, the resulting \chitwo\ for the calibration lines are smaller than for the corresponding 1D cases; the only exceptions are for the \ki\,769.89, \feii\,624.76 and/or \feii\,645.64\,nm lines for a few of the stars. The derived \vsini\ values are between 0.1 and 3.8\,\kms . The typical uncertainties in \vsini\ are 0.3\,\kms\ but in some cases can be as large as $\approx 1$\,\kms . Very little is known about the observed rotation properties of metal-poor halo stars but due to their high age one would expect them to rotate slowly (the Sun has $v_{\rm rot}=1.8$\,\kms ). It is therefore quite possible that the estimated rotational velocities towards the higher end are overestimated. For example, Smith et al. (1998) suggest \vsini\,$<2-3$\,\kms\ for a typical metal-poor turn-off star. It can, however, not be ruled out at present that some of these stars actually have \vsini\,$\approx 3$\,\kms . Part of the explanation for some of the high estimated \vsini\ values is that the adopted stellar parameters for the 3D models are inappropriate for some of the stars: if a too low \teff\ or too high \logg\ are used then the convective motions and thus the Doppler line broadening will be too small, requiring large \vsini\ to compensate when fitting the observed spectral lines. Furthermore, we remind the reader that LTE has been assumed for these 3D line formation calculations while the steep temperature gradients in low metallicity 3D models can be expected to result in significant non-LTE effects (Asplund et al. 1999; Asplund 2005). We suspect that this may be the explanation for the slight correlation between \vsini\ and \feh\ in our sample, although we note that \vsini\ is particularly uncertain for the two stars with \feh\,$\approx -1$ (HD\,3567 and G\,075-031) because of the quite strong calibration lines employed. We therefore urge these \vsini\ values not to be taken too literally at this stage. In fact, it is encouraging that the resulting rotational velocities are at least reasonable given that there are no broadening mechanisms like micro- and macroturbulence as in 1D that can be tuned. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/CaI6162.1_3D+1D_HD140283_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/CaI6162.1_3D+1D_HD160617_res.eps}} \resizebox{\hsize}{!}{\includegraphics{f16a.eps}} \resizebox{\hsize}{!}{\includegraphics{f16b.eps}} \caption{\cai\ 616.21\,nm line in HD\,140283 ({\em upper panel}) and HD\,160617 ({\em lower panel}). The solid lines correspond to the best fitting 3D profiles from a \chitwo\-analysis while the dashed lines are for the 1D profiles; the rhombs are the observed profiles. Also shown are the residuals between observed and predicted line profiles.} \label{f:ca6162_3D_1} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/CaI6162.1_3D+1D_G020-024_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/CaI6162.1_3D+1D_G075-031_res.eps}} \resizebox{\hsize}{!}{\includegraphics{f17a.eps}} \resizebox{\hsize}{!}{\includegraphics{f17b.eps}} \caption{Same as Fig. \ref{f:ca6162_3D_1} but for G\,020-024 ({\em upper panel}) and G\,075-031 ({\em lower panel}).} \label{f:ca6162_3D_2} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_3D_G020-024_res.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6707.8_3D_LP815-43_res.eps}} \resizebox{\hsize}{!}{\includegraphics{f18a.eps}} \resizebox{\hsize}{!}{\includegraphics{f18b.eps}} \caption{\lii\ 670.78\,nm line in G\,020-024 ({\em upper panel}) and LP815-43 ({\em lower panel}) based on a 3D LTE analysis. The best fitting line profiles as judged by a \chitwo\-analysis for \liratio\,$=+0.00, +0.05$ and $+0.10$ are shown.} \label{f:li6708_3D} \end{figure} Interestingly, in general the 3D LTE calculations do not improve the agreement with the \lii\,670.78\,nm line as judged by the \chitwo -statistics. For more than half of the stars, the 3D analysis yield slightly higher minimum \chitwo-values than in 1D. The most likely explanation in our opinion for this contrasting behaviour compared with the Ca and Fe lines is that LTE is a particularly poor assumption for the \lii\ line in metal-poor stars; pronounced over-ionization of \lii\ is predicted from 3D non-LTE calculations due the steep temperature gradients of the 3D model atmospheres (Asplund et al. 2003; Barklem et al. 2003). An inspection of Table \ref{t:li6_3D} reveal that the 1D \liratio\ ratios appear to be similar or lower than the ratios derived from 3D LTE calculations. Only in three stars are the 3D results noticeably smaller than for the corresponding 1D case. The smaller \liratio\ ratios in HD\,3567 and G\,075-031 are likely a reflection of the relatively high \feh\ of these two stars, which renders the calibration lines used to determine \vsini\ quite strong (equivalent widths up to 12\,pm); in the case of the Sun, the impressive agreement between predicted and observed line profiles found for weak lines break down for such strong lines (Asplund et al. 2000). The difference between 3D and 1D for LP\,815-43 is of particular interest given the prominent status this star will have when later discussing the implications of our \lisix\ survey. In 3D, the derived isotopic ratio is \liratio\,$=0.036\pm0.021$ to be compared with the 1D value of \liratio\,$=0.046\pm0.022$ (both results are for the August 2004 observations). Taking these 3D LTE calculations at face value, LP\,815-43 would no longer be considered a significant \lisix\ detection, although it would not be far from making the $2\sigma$ criteria. Considering the expected severe 3D non-LTE effects on the \lii\ line in metal-poor stars that are not accounted for here, the 1D results are to be preferred. Indeed, one would expect also the calibration lines used to estimate \vsini\ to be vulnerable to departures from LTE, in particular minority species like \cai\ and \fei\ (Asplund 2005). Carrying out detailed 3D non-LTE calculations for both the calibration lines and the \lii\ line for the necessary many simulation snapshots is unfortunately extremely computationally demanding. We will therefore have to postpone investigating this remaining issue to a future date. The preliminary 3D LTE analysis carried out here, however, has not uncovered any significant systematic errors that would suggest that our 1D-based Li isotopic ratios are overestimated in general. \subsection{Comparison with Previous Studies} \label{s:li6708_literature} A number of our targets have been investigated for their Li isotopic abundances in previous studies. Our non-detection of \lisix\ is consistent with the upper limits reported for HD\,19445, HD\,140283 and BD\,$+03\arcdeg0740$ by Smith et al. (1993, 1998) and Hobbs \& Thorburn (1994, 1997). Our derived value for G\,271-162 (\liratio\,$=0.019\pm0.012$) does not constitute a detection of \lisix\ but is very close to Nissen et al.'s (2000) result of \liratio\,$=0.02\pm0.01$ based on the same VLT/UVES commissioning spectra, in particular as we have here adopted a slightly more conservative estimate of the uncertainties. More noteworthy is the result that we do not confirm the \lisix\ detection for HD\,338529 (also known as BD\,$+26\arcdeg3578$) by Smith et al. (1998) who found \liratio\,$=0.05\pm0.03$. Our value of $0.010\pm0.013$ is based on a higher quality spectrum ($S/N \simeq 520$ vs 420) but the main difference can be traced to the adopted line broadening parameters. Smith et al. combined the effects of instrumental broadening and macroturbulence by convolving the synthetic spectra with a Gaussian profile, but used only the \cai\ 671.78\,nm line to determine the width of this Gaussian; however, this line is quite weak in HD\,338529 having a line depth of only 3\% at $R = 110,000$. As a result, Smith et al. could not constrain the macroturbulent velocity parameter for this star very well (this can be seen in their Figure 6 for HD\,338529, where the \chitwo\ as a function of macroturbulent velocity is very shallow). Our higher broadening parameter is significantly better determined as it is based on four \cai\ and \fei\ lines, all in very good agreement. We would also have found a significant \liratio\ ratio had we adopted the same macroturbulence as Smith et al. (1998). In addition, for two of our stars with significant \lisix\ detections, Smith et al. could only obtain upper limits: $\le 0.06$ and $\le 0.05$ ($2\sigma$) for HD\,102200 and HD\,160617, respectively. Again, the main difference appears to be the adopted macroturbulence parameter, which in our case is smaller than their value. Also, our spectra for these stars have significantly higher $S/N$. The differences in \liratio\ between us and Smith et al. for HD\,338529 certainly serve as a warning when trying to interpret the results in terms of Li isotopic abundances for this extremely challenging method. It is clearly paramount to have exceptionally high $S/N$ as well as well-determined intrinsic broadening parameters based on a multitude of spectral lines with similar strength as the \lii\ 670.8\,nm line. While we have tried to accomplish both of these factors and believe that we have set a new standard in this respect, we urge the reader to exercise some caution when using our quoted Li isotopic abundances. Deliyannis \& Ryan (2000) reported a firm detection of \lisix\ in the subgiant HD\,140283: \liratio\,$=0.040 \pm 0.015$. No details of this analysis have as yet appeared in the literature. We are, therefore, not able to identify reasons for the discrepancy with our non-detection of \liratio\,$=0.008 \pm 0.006$. Our result for HD\,140283 is, however, consistent with the upper limit of \liratio\,$<0.018$ estimated recently by Aoki et al. (2004) based on a Subaru/HDS spectrum of the quality of our VLT/UVES spectrum. Wako Aoki has kindly made available their Subaru spectrum of HD\,140283 for an independent analysis by us. As we did not have access to their measured instrumental profile, we performed the analysis adopting a combined Gaussian for the instrumental and macroturbulence broadening, a case also considered by Aoki et al. Our result of \liratio\,$=0.003$ is in perfect agreement with their corresponding result of 0.002 when using their choice of calibration lines. We note that when we perform an analysis in the same way as for our own sample (i.e. using the same calibration lines and taking into account uncertainties in line broadening, $S/N$ and stellar parameters), we find \liratio\,$=0.006\pm0.004$, which is in excellent agreement with the UVES result. When expanding the set of calibration lines to include in total 14 lines between 500 and 650\,nm from the Subaru spectrum, the $1\sigma$ error doubles: \liratio\,$=0.007\pm0.009$. The exact results and uncertainties thus depend (slightly) on the particular choice of lines to estimate the line broadening, which must be borne in mind when comparing different \liratio -analyses. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \section{Li Abundances from the \lii\ 610.4\,nm Subordinate Line} \label{s:li6104} \subsection{Analysis} \label{s:li6104.anal} The exceptionally high quality of our UVES spectra allows Li abundances to be derived from the subordinate \lii\ 610.36\,nm line, which in these halo stars has an equivalent width of just $0.1-0.2$\,pm ($1-2$\,m\AA ). We have performed a similar \chitwo -analysis of a wavelength region around 610.4\,nm, taking into account the hyperfine and isotope splitting for the Li line and neighboring lines of \fei , \feii\ and \cai . The adopted Fe and Ca abundances were those implied by the other considered Fe and Ca lines. While no attempt was undertaken to optimize the agreement between observations and predictions for these Fe and Ca lines by adjusting the $gf$-values or elemental abundances, we emphasize that this had no impact on the derived Li abundances as the neighboring lines are quite well described and sufficiently far away from the Li feature not to cause any problems. Fig. \ref{f:li6104_spec1} and Fig. \ref{f:li6104_spec2} compare the synthesized profiles for different Li abundances with the observed spectra for a few stars. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6104_HD19445.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6104_HD140283.eps}} \resizebox{\hsize}{!}{\includegraphics{f19a.eps}} \resizebox{\hsize}{!}{\includegraphics{f19b.eps}} \caption{Observed and theoretical \lii\ 610.4\,nm profiles for HD\,19445 (upper panel) and HD\,140283 (lower panel). The four theoretical 1D LTE profiles are computed with no Li, \logli\,$=2.0$, 2.2 and 2.4, respectively, with the stellar parameters listed in Table \ref{t:parameters}. For each star, the residuals between the synthesis and observations are also shown.} \label{f:li6104_spec1} \end{figure} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6104_LP815-43.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6104_BD+09_2190.eps}} \resizebox{\hsize}{!}{\includegraphics{f20a.eps}} \resizebox{\hsize}{!}{\includegraphics{f20b.eps}} \caption{Same as for Fig. \ref{f:li6104_spec1} but for LP\,815-43 (upper panel) and BD\,$+09\arcdeg 2190$ (lower panel). No significant detection of the \lii\ 610.4\,nm line is made in the latter star according to a \chitwo -test, although there is a possible feature at the correct wavelength that would correspond to \logli\,$\approx 2.0$. } \label{f:li6104_spec2} \end{figure} The derived Li abundances from the subordinate \lii\ 610.4\,nm line are listed in Table \ref{t:li_abundances}. The line is unambiguously detected in 22 of the 24 program stars with the two exceptions being the very metal-poor stars BD\,$+03\arcdeg 0740$ and BD\,$+09\arcdeg 2190$. Also for those two stars there is a tantalizing suggestion of a feature at the correct wavelength, although the \chitwo -analysis does not indicate a significant detection. As a consequence, we only give $3\sigma$ upper limits to the Li abundance in these two stars. The derived 1D LTE Li abundances from the \lii\ 610.4\,nm line have been corrected for departures from LTE using the detailed 1D statistical equilibrium calculations of Carlsson et al. (1994). The non-LTE abundance corrections for the subordinate line are positive and slightly larger than for the resonance lines: typically $\Delta$\logli$\simeq +0.05$\,dex. The maximum non-LTE effect occurs for the metal-poor subgiant HD\,140283 ($+0.09$\,dex). \subsection{Comparison with Results from the Li Resonance Line} \label{s:li6104vsli6708} Figure \ref{f:li6104vsli6708} compares the derived Li abundances from the weak subordinate \lii\ 610.4\,nm line with those from the stronger \lii\ 670.8\,nm resonance line. The agreement is very encouraging with a mean difference of only $0.05\pm0.05$\,dex for the 22 stars with measured Li abundances. For all practical purposes, the two lines return the same lithium abundance for a given star. The differences show no obvious trends with metallicity or effective temperature. The upper limits for the Li abundances from the subordinate line in BD\,$+03\arcdeg 0740$ and BD\,$+09\arcdeg 2190$ are very close to the abundances from the resonance line. It is unlikely that the explanation for this minor abundance difference can be found in erroneous $gf$-values for either of the two lines. One (remote) possibility is that the adopted \teff\ values are underestimated; a $\approx 150$\,K higher \teff -scale would erase the mean difference. Another explanation could be inappropriate non-LTE abundance corrections for the 1D models. Use of 3D models with non-LTE line formation might erase the differences (Asplund et al. 2003). A study aimed at investigating the 3D non-LTE line formation for a wider range of stellar parameters as well as revisiting the 1D non-LTE abundance corrections in light of recent improvements in collisional data (Belyaev \& Barklem 2003; Barklem et al. 2003) would be worthwhile. \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6104_abudiffvsTeff.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LiI6104_abudiffvsFeH.eps}} \resizebox{\hsize}{!}{\includegraphics{f21a.eps}} \resizebox{\hsize}{!}{\includegraphics{f21b.eps}} \caption{Differences in the 1D non-LTE abundances from the \lii\ 610.4\,nm and 670.8\,nm lines as a function of \teff\ ({\em upper panel}) and \feh\ ({\em lower panel}).} \label{f:li6104vsli6708} \end{figure} The \lii\ 610.4\,nm line was first detected in the halo star HD\,140283 by Bonifacio \& Molaro (1998). They also found very good agreement in the abundances inferred from the two Li lines. Likewise, Ford et al. (2002) derived the same abundances from the 610.4 and 670.8\,nm lines for this star using a very high quality spectrum obtained with Subaru/HDS (the same spectrum as used by Aoki et al. (2004) to derive an upper limit to \liratio\ in this star as discussed above). However, for the other seven stars for which Ford et al. (2002) claimed a detection of the subordinate line, the derived Li abundances are $0.2-0.5$\,dex higher than suggested by the resonance line. This is in sharp contrast with our findings. While we are not in a position to unequivocally identify the reasons for the very different conclusions of Ford et al., we suspect that the key is the quality of the observations. The $S/N$ ratios of the spectra of Ford et al. are between 200 and 300 around the 610.4\,nm line, which may still not be sufficient to detect this very weak line in metal-poor turn-off stars (note that this line is about 50\% stronger in a subgiant like HD\,140283 with \teff\,$\approx 5700$\,K than in a turn-off star with \teff\,$\approx 6200$\,K for the same Li abundance). Under these circumstances it is easy to overestimate the line strength due to noise and thus derive too high abundances. In comparison, our spectra have $S/N \approx 500$ or better in the relevant wavelength region. Finally, we note that our resolving power is about twice as large as obtained by Ford et al. (110\,000 vs 50\,000). %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \section{Origin and Evolution of Lithium} \label{s:evolution} \subsection{Lithium Abundance Trends and Scatter} \label{s:trends} Since our sample is relatively small and does not extend to extremely low metallicities, our discussion of the lithium abundances will be relatively brief. Furthermore, our results for the total lithium abundance are in broad agreement with many published analyses. The principal novelty from our study is an estimate of the isotopic ratio for stars on the Spite plateau. Our data may be used to quantify the trend of the lithium abundance with metallicity (here, Fe/H or O/H), to extrapolate the trend to zero metallicity, and to determine the scatter in lithium abundance about the mean trend. In applying our data, we have excluded G\,271-162 since no accurate H$\alpha$-based \teff\ could be derived from this star (see Sec. \ref{s:teff}). IIn addition, the Li-rich star HD\,106038 has been excluded because it has strong overabundances in Si, Ni, Y and Ba (Nissen \& Schuster 1997), and a very high Be abundance relative to other halo stars of similar \feh\ (Primas et al., in preparation). This peculiar abundance pattern suggests that the star has undergone a highly unusual nucleosynthesis enrichment, possibly due to mass transfer, which justifies its exclusion here. Such Li-rich stars as HD\,106038 appear to be extremely rare. Perhaps the only known other example is the subgiant BD\,$+23\arcdeg 3912$ with [Fe/H] $=-1.5$ and \logli\ $= 2.6$ (King et al. 1996). In addition, our sample deliberately excluded any of the rare Li-deficient halo dwarfs. The nature of these stars is currently under debate (cf. Ryan et al. 2002; Frebel et al. 2005; Aoki et al. 2006; Charbonnel \& Primas 2005). Our assumption is that these stars have also undergone a very special event, a binary merger perhaps (Ryan \& Elliott 2005). \begin{figure}[t!] %\resizebox{\hsize}{!}{\includegraphics{figures/logLivsFeH.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/LivsFe.eps}} \resizebox{\hsize}{!}{\includegraphics{f22a.eps}} \resizebox{\hsize}{!}{\includegraphics{f22b.eps}} %\epsscale{0.6} %\plotone{f22a.eps} %\plotone{f22b.eps} \caption{Non-LTE \liseven\ abundances (1D) from the \lii\ 670.8\,nm line as a function of metallicity; as for Fig. \ref{f:li6708_summary} solid circles here denote stars for which \lisix\ appears to have been detected while open circles are non-detections. In the upper panel logarithmic abundances are shown (\logli\ vs \feh ) while in the lower panel linear abundances ($^7$Li/H vs \fefesun ) are used, which are more appropriate when extrapolating to the primordial composition. The solid lines denote the best linear fits to the data when excluding G\,271-162 (no \ha -based \teff ) and HD\,106038 (abnormally high Li abundance and other peculiar abundances, see text). In the lower panel, the dashed line corresponds to the linear fit when only including the stars with \feh\,$<-2.2$ (G\,271-162 again excluded). The horizontal solid line in the upper panel shows the predicted primordial Li abundance from Big Bang nucleosynthesis and the baryon density inferred from WMAP (Spergel et al. 2003) together with the corresponding $\pm 1\sigma$ uncertainties as dotted lines. } \label{f:li_feh} \end{figure} From the abundances listed in Table \ref{t:li_abundances}, the mean \liseven\ abundance of the remaining 22 stars is \logliseven\,$=2.21 \pm 0.07$. As shown in Fig. \ref{f:li_feh}, there is, however, a pronounced trend with metallicity, which resembles the correlation with \feh\ found in some previous Li studies (e.g. Thorburn 1994; Norris et al. 1994; Ryan et al. 1996, 1999; Bonifacio et al. 2003, 2006). A univariate linear least-square-fit taking into account the estimated uncertainties in \feh\ and the Li abundances (excluding HD\,106038 and G\,271-162 for the above reasons) implies \begin{equation} \log \epsilon_{\rm ^7Li} = \left( 2.409\pm0.020\right) + \left(0.103\pm0.010\right) \cdot [{\rm Fe/H}]. \end{equation} \noindent The observed slope is very similar in value to that presented by Ryan et al. (1999): $0.103\pm0.010$ vs $0.118\pm0.023$ for Ryan et al. The scatter around our fit is only $\sigma_{\rm obs} = 0.033$\,dex. None of the remaining 22 stars is identified as an outlier by statistical tests. Repeating the exercise using \oh\ instead of \feh\ as the independent variable yields \begin{equation} \log \epsilon_{\rm ^7Li} = \left( 2.372\pm0.017\right) + \left(0.115\pm0.011\right) \cdot [{\rm O/H}]. \end{equation} \noindent Here the non-LTE abundances from the \oi\ 777\,nm triplet have been used to estimate [O/H]. Again, the scatter is very small: $\sigma_{\rm obs} = 0.034$\,dex. In Sect. \ref{s:teff} we estimated the relative precision in our adopted \teff -values to be about 30\,K, which would introduce an uncertainty in Li abundance of 0.022\,dex. Adding also the minor uncertainties from the $S/N$ and the other stellar parameters gives a total expected random error of 0.026\,dex. This expectation is only slightly less than the observed scatter of $\sigma_{\rm obs} = 0.033$\,dex around the linear fit. The indication is that the star-to-star scatter in lithium abundances at a given [Fe/H] is very small, say 0.02\,dex or less. (If the temperature error were increased to 40\,K, the expected scatter in the abundances would match the observed scatter.) The observed scatter around the linear fit to our data is very similar to that found by Ryan et al., who achieved similarly high precision in \teff\ ($\sigma_{\rm T} \approx 30$\,K) but utilised lower quality spectra ($S/N \approx 100-150$ and $R \approx 50 000$). They found $\sigma_{\rm obs} = 0.031$\,dex after rejecting one star, BD\,$+09\arcdeg$2190, as an outlier; we note that with the equivalent width measured from our $S/N \approx 650$ spectrum, it would no longer be considered an outlier. A different and especially a larger sample of stars may shed new light on the intrinsic scatter in the lithium abundances. For example, Nissen et al. (2005b) find that the otherwise almost identical stars G\,64-12 and G\,64-37 differ in their Li abundances by about 0.16\,dex. Their reported observed scatter is 0.041\,dex when including G\,64-12 but 0.035\,dex when excluding it. No doubt, any intrinsic scatter must be very small: $\la 0.04$\,dex. The near-common belief has been that the primordial lithium abundance is obtainable by extrapolation of the observed abundances to zero metallicity. One supposes that extrapolation should be performed using Fe/H (or an alternative such as O/H) and not the logarithmic [Fe/H] (or [O/H]). As seen in Fig. \ref{f:li_feh}, on such a linear scale the most metal-poor stars seem to indicate a steeper slope than the less metal-poor stars, but there is no known explanation for the apparent change of slope close to the origin Fe/Fe$_{\rm sun}$ = 0. Somewhat different results are, therefore, obtained depending on which stars are included. When including only the nine stars with \feh\,$<-2.2$ (as usual, excluding G\,271-162), the estimated primordial \liseven\ abundance is $^7{\rm Li/H} \approx 1.1 \cdot 10^{-10}$ or \logli\ $\approx 2.04$. Taking all 22 stars into account results in an increase to $^7{\rm Li/H} \approx 1.4 \cdot 10^{-10}$ of \logli\ $\approx 2.15$. Very similar results are obtained using extrapolation to \oosun\,$=0$. If the presence of \lisix\ at the level of that now observed for LP\,815-43 is a general feature among the most metal-poor stars and it is produced in spallation or $\alpha$-fusion reactions, the \liseven\ abundances would have a minor non-Big Bang contribution which would reduce the estimated primordial \liseven\ abundance further by about 0.05\,dex (Smith et al. 1998; Ryan et al. 1999; 2000). Our estimates of the primordial abundance do not differ significantly from the majority of published determinations, although they may be somewhat on the low side of previous estimates (e.g., Spite \& Spite 1982; Thorburn 1994; Ryan et al. 1996, 1999; Bonifacio \& Molaro 1997; Bonifacio et al. 2003, 2006). Our estimate of the primordial abundance is based on 1D model atmospheres and includes a correction for non-LTE effects. Presently available calculations (Asplund et al. 2003; Barklem et al. 2003; also Sec. \ref{s:li6708_3D}) suggest that only a minor revision will be needed when the abundance analyses are redone using 3D models with inclusion of non-LTE effects. It has been claimed by Melend\'{e}z \& Ram\'{i}rez (2004) that their new calibration of the infrared flux method (IRFM) of effective temperature determinations (Ram\'{\i}rez \& Melend\'{e}z 2005a,b) raises substantially the lithium abundances derived from metal-poor dwarf stars. This new \teff -scale is significantly hotter at low metallicity than our \ha -based \teff -scale. It is also hotter than the IRFM calibration of Alonso et al. (1996), even though the photometric measurements required by the IRFM of the two studies agree well for the stars in common. For stars with \feh\,$<-3$, such as G\,64-12, G\,64-37 and LP\,831-70, the new temperatures are 240, 460 and 320\,K, respectively, higher than those estimated using the Alonso et al. \vk\ calibration. Ram\'{\i}rez \& Melend\'{e}z argue that the strikingly different behaviour for the colour calibrations at low \feh\ is due to the shortage of low metallicity stars in Alonso et al.'s sample. A detailed scrutiny of Ram\'{\i}rez \& Melend\'{e}z' \teff -scale is beyond the scope of the present investigation. Nevertheless, it is pertinent to estimate the impact of the scale on our results. For the most metal-poor stars in our sample (\feh\,$<-2.6$), the \teff -values of Melend\'{e}z \& Ram\'{i}rez (2004) are on average $182\pm72$\,K higher than ours based on \ha , which increases the mean 1D non-LTE \liseven\ abundance for those particular stars from \logliseven\,$=2.10$ to 2.23. Independently of the new \teff\ scale, there are reasons why Melend\'{e}z \& Ram\'{i}rez (2004) arrive at the significantly higher mean \liseven\ abundance of \logliseven\,$=2.37\pm0.06$ compared with our estimate: their use of convective overshoot model atmospheres ($\approx +0.1$\,dex), their neglect of non-LTE corrections ($\approx +0.02$\,dex) and their use of Kurucz models rather than \marcs\ model atmospheres ($\approx +0.02$\,dex). The remaining difference with our primordial \liseven\ abundance estimate stems from the extrapolation to Fe/Fe$_{\rm sun}$ = 0 in the presence of our derived slope with metallicity. Observational evidence does not favor the convective overshoot option as introduced in the Kurucz (1993) model atmospheres (e.g. Castelli et al. 1997) nor does this approach find any support in 3D hydrodynamical simulation of surface convection in metal-poor stars (Asplund et al. 1999). Non-LTE abundance corrections, while small, should be taken into account. We suggest therefore that Melend\'{e}z \& Ram\'{i}rez' estimate of the primordial \liseven\ abundance should be revised downward by at least 0.12\,dex regardless of whether or not their \teff -scale is preferable to the one employed here. We note that our \ha -based temperatures are in excellent agreement on average with the well-established IRFM \vk\ and \by\ calibrations of Alonso et al. (1996), which seems to give little room for such large increases in \teff\ as advocated by Melend\'{e}z \& Ram\'{i}rez (2004), In addition, accounting for 3D effects should push the \ha -based \teff -values downwards. More work is needed to settle the \teff -scale of metal-poor stars, Recently Bonifacio et al. (2006) have attempted to push the abundance determinations to yet lower \feh . In general their results agree well with ours. Their mean 1D non-LTE Li abundance for 17 stars (excluding a subgiant and a spectroscopic binary) is \logli\,$=2.17 \pm 0.09$; they argue that the expected uncertainty is about 0.08\,dex from the \teff -errors and quality of the spectra (median $S/N =180$), leaving little or no room for intrinsic scatter, in particular when considering the possibility of a trend in their Li abundances with metallicity. Due to the small range in \feh\ of their sample, this correlation may or may not be statistically significant by itself but when including also our results a consistent picture emerges. We note that their \ha-based \teff-scale should be very similar to ours but that their \feh\ are likely underestimated by $0.1-0.2$\,dex due to their use of \fei\ lines (Sect. \ref{s:feh}); unfortunately the two samples have no stars in common, which prevents a direct comparison of the parameters and Li abundances. Interestingly, the combination of the two samples suggest a steeper slope for \feh\,$\la -2.3$ than for higher metallicity. Whether this effect is real or spurious due to the analysis methods (1D model atmospheres, \teff-scale etc) is an open question for the future. An alternative interpretation is that the intrinsic scatter increases significantly for \feh\,$\la -2.3$. Our major new result concerns the measurements of the lithium isotopic ratio and the apparent appearance of the analogue for \lisix\ of the Spite plateau (Fig. \ref{f:li6708_summary}). It is impossible to determine if the observed plateau is tilted, as the Spite plateau is; as shown in Sect. \ref{s:depletion}, when accounting for \lisix\ depletion during the pre-main sequence evolution the observed \lisix\ abundances apparently increase towards higher metallicity. There may be a real scatter associated with this \lisix\ plateau. The average observed abundance from eight stars with a positive \lisix\ detection (HD\,106038 is not included) is \loglisix\,$ = 0.82$, i.e. without accounting for any \lisix\ depletion. Taking the mean \liratio\ of all stars but HD\,106038 (unusually high Li abundance) and HD\,19445 (expected to have no \lisix ) together with the mean \liseven\ abundance of the same stars would instead imply \loglisix\,$=0.54$. To both of these estimates should be added the expected \lisix\ depletion which is $\ge 0.3$\,dex during the pre-main sequence during which \liseven\ remains largely intact, as discussed in Sect. \ref{s:depletion}. If, in addition, some \liseven\ has been destroyed as well this would increase the \lisix\ depletion further. \subsection{The Lithium Problems} \label{s:liproblems} Since Spite \& Spite's (1982) seminal paper, the lithium abundance of metal-poor warm dwarfs has been widely equated with the abundance provided by the Big Bang. The predicted abundance from a standard Big Bang is dependent on one free parameter, namely, the baryon density. Now, the free parameter is determined independently of any inferred primordial abundances from the WMAP-observations of the anisotropies of the cosmic microwave background: $^7{\rm Li/H} = 4.4\pm1.0 \cdot 10^{-10}$ or \logliseven\,$=2.65\pm0.1$ (Coc et al. 2004; Cuoco et al. 2004; Cyburt 2004). As different calculations yield slightly different results even when adopting exactly the same baryon density, we have taken an average of the cited results. These same calculations show that very little \lisix\ is synthesised, say \liratio\ $\sim 10^{-5}$. While the predictions from standard Big Bang nucleosynthesis are in good agreement with the mean deuterium abundance from the six available damped Ly-$\alpha$ systems (e.g. Steigman 2005 and references therein), they are in substantial conflict with the observations for Li. The \liseven\ problem is now well established: the inferred primordial \liseven\ abundance is about 0.5 dex less than the prediction. As will become clear from the discussion in Sect. \ref{s:spallation}, our survey has in addition identified a \lisix\ problem: the observed high \lisix\ abundance at very low \feh\ can not be explained by neither standard Big Bang nucleosynthesis nor apparently by Galactic cosmic ray spallation and $\alpha$-fusion reactions. Possible resolutions of these problems were reviewed by Lambert (2004). It should also be noted that the problem of reconciling the inferred and predicted \liseven\ abundance is not entirely decoupled from the goal of achieving an understanding of the synthesis of \lisix . Possible modes of \lisix\ synthesis imply simultaneous synthesis of \liseven\ but this aggravates the severity of the \liseven\ problem. In turn, the presence of \lisix\ constrains the possible explanations invoked for the \liseven\ problem. The solution to the \liseven\ problem may lie in one or more of the following areas: \smallskip \noindent {\em Systematic errors in the abundance analysis:} The introduction of an abundance analysis based on 3D model atmospheres and non-LTE line formation for the lithium resonance and subordinate lines has not resulted in a significant upward revision of the lithium abundance obtained from 1D atmospheres and LTE or non-LTE line formation. The derived lithium abundance is dependent on the adopted \teff -scale but this cannot accommodate the higher temperatures necessary to bring inferred and predicted abundance into agreement (see Sec. \ref{s:teff} and \ref{s:trends}). Although the last word has not been said on the representation of the physics of the stellar atmospheres and the formation of the lithium lines, it would be extremely surprising were systematic errors in these areas be shown to resolve the lithium problem. \smallskip \noindent {\em Present-day abundances do not reflect the primordial Li abundance:} Dilution and destruction of lithium in metal-poor stars are discussed in the following section (Sec. \ref{s:depletion}). \smallskip \noindent {\em Erroneous nuclear reaction rates:} Nuclear reactions included in the customary networks have been well studied and uncertainties in the reaction rates at the relevant temperatures for Big Bang nucleosynthesis cannot be held responsible for the lithium problem. Coc et al.'s (2004) suggestion that addition to the network of a previously neglected reaction -- $^7$Be($^2$D, p)2 $^4$He -- might possibly reduce the predicted \liseven\ abundance is not substantiated by a cross-section measurement (Angulo et al. 2005). ($^7$Be decays to $^7$Li following Big Bang nucleosynthesis.) Based on the measured solar neutrino flux, Cyburt et al. (2004) have been able to show that employed nuclear data for the $^3$He($\alpha,\gamma$)$^7$Be reaction can not be in error by a large factor as to modify the predicted $^7$Li abundances significantly. \smallskip \noindent {\em Non-standard Big Bang nucleosynthesis:} Comments on the synthesis of the lithium isotopes by non-standard Big Bang models are included in our discussion of the synthesis of \lisix\ in Sec. \ref{s:spallation}. \subsection{Lithium Destruction and Dilution in Halo Stars} \label{s:depletion} Identification of the primordial lithium abundance from the Spite plateau with the abundance provided by the Big Bang rests on the assumption that the lithium abundance of the atmosphere of a star on the plateau has been unchanged since the star was formed from gas having the lithium abundance provided by the Big Bang. Perhaps, the most promising solution to the lithium problem represents a failure of this assumption. Solutions have consequences for the correction of observed \lisix\ abundances to the \lisix\ abundance of the gas from which a star formed. In standard stellar models, the expected depletion of \liseven\ for metal-poor turn-off stars is negligible, i.e., less than 0.02\,dex (Deliyannis et al. 1990; Pinsonneault et al. 1992). A larger depletion, $\ge 0.3$\,dex, is predicted for \lisix\ with most of this occuring during the pre-main sequence phase when \lisix\ is destroyed by protons at the base of the star's deep convective envelope (e.g. Richard et al. 2005). The cross-section for destruction of \lisix\ is about 60 times greater than for \liseven . Destruction of \lisix\ is predicted to increase sharply with decreasing stellar mass for main sequence stars below the turn-off. Evidently, depletion (destruction) of \liseven\ is according to standard models not the answer to the lithium problem but is a factor to be considered when we turn to examine synthesis of \lisix . The search for a solution to the lithium problem then turns to investigation of non-standard models of stellar evolution (Lambert 2004). Physical processes neglected by standard models but incorporated into non-standard models in connection with halo stars in recent years include rotationally-induced mixing (e.g. Vauclair 1988; Chaboyer \& Demarque 1994; Pinsonneault et al. 1999, 2002; Piau 2005), diffusion\footnote{The term diffusion normally includes the effects of gravitational settling, thermal diffusion and radiative acceleration.} (e.g. Michaud et al. 1984; Salaris \& Weiss 2001; Richard et al. 2002; 2005) and internal gravity waves (e.g. Talon \& Charbonnel 2004; Charbonnel \& Talon 2005), sometimes working in tandem with other mechanisms such as mass loss (e.g. Vauclair \& Charbonnel 1995) and turbulent mixing. In most cases, the predictive power of these processes is restricted by their need to introduce one or more free parameters. We comment briefly on two non-standard models drawn from the suite of proposals: rotationally-induced mixing and diffusive separation. An obvious requirement of successful non-standard models is that they provide a depletion of surface lithium by about 0.5\,dex over the 10-13 Gyr life of the observed stars (we take it as given that the stars began life with the WMAP-inferred predicted lithium abundance.) Surely, a more demanding requirement (and a certain clue to the dominant process) is that this depletion be achieved uniformly over the observed sample of stars spanning a range in mass, metallicity, age, and rotational angular momentum: the depletion sought is about 0.5\,dex with a star-to-star scatter of not more than about 0.03\,dex. Our present interest is in identifying non-standard models that may solve the lithium problem and in obtaining an estimate of the correction to be applied to a \lisix\ abundance to obtain the star's original \lisix\ abundance. A description of lithium destruction from rotationally-induced mixing depends on processes and initial conditions that are as yet poorly known, including the initial distribution of angular momentum in the star, the transport of angular momentum through the star and its loss from the surface, and attendant mixing of the interior material. To make progress requires calibrations using observations of rotational velocities and lithium abundances for stars, e.g., the Sun and stars belonging to open clusters. Calibrations have not involved metal-poor dwarfs. A probable result of rotational effects on lithium depletion is a spread in the final lithium abundance for a sample of stars differing only in their rotational characteristics. One expects lithium depletion to be most severe for the stars initially rotating rapidly and least severe to vanishingly small for the slowest rotators. Then, the observed (small) spread in lithium abundances on the Spite plateau is, in principle, an indicator of rotationally-induced depletion of lithium. Conversion of the observed spread to an indicator of depletion depends on the description of rotational-induced mixing and the attendant calibrations. The recipe and calibrations (Sun, open clusters) invoked by Pinsonneault et al. (1999) show that the depletion of \liseven\ ($D_7$ in dex) was related to the dispersion ($\sigma$ in dex) where $\sigma/D_7 \simeq 0.4$ and, hence, the required depletion by 0.5 implies $\sigma$ = 0.2, a value far in excess of the observed upper limit. The depletions of \liseven\ and \lisix\ were predicted to be correlated: $D_7/D_6 \simeq 0.4$ yielding $D_6 \approx 1.2$ dex. Given that the observed \loglisix\ $\simeq 0.8$ for the stars with detected \lisix , the initial abundance would have been \loglisix\ $\simeq 2.0$, the value that has historically been identified with the Spite plateau for \liseven\, and, more importantly, a value that implies most or all of the \liseven\ came from synthesis by cosmic rays and not from the Big Bang! Pinsonneault et al. (2002) argue that the Li data of Ryan et al. (1999), who like us measured $\sigma_{\rm obs} = 0.03$\,dex, imply a most-likely \liseven\ depletion of $0.13$\,dex although destruction factors as high as 0.3\,dex were not ruled out. The corresponding \lisix\ destruction is then $\ge 0.3$\,dex, and \loglisix\ $\ge 1.1$ for our stars with \lisix\ detections. In summary, rotationally-induced mixing as presented in the models of Pinsonneault et al. appears not to be the solution to the \liseven\ problem. Stars on the Spite plateau have a thin convective envelope of uniform composition. Atomic diffusion occurs in the radiative zone below the convective envelope. The base of the latter mixes with and attains the composition of the top of the radiative zone. Diffusion is a slow process but is predicted to be effective in the halo dwarfs because of their great age and their thin convective envelopes. The diffusive velocity decreases with increasing density. Since the stars at the turn-off have the thinnest envelopes, the effects of diffusion on surface composition are likely to be more severe for these stars than for stars further down the main sequence. Lithium is predicted to diffuse inwards in the radiative zone and the surface abundance to decrease. Inward diffusion of lithium can result in its destruction by protons. Model calculations including diffusion suggest that the lithium abundance for stars on the Spite plateau can be reduced to the observed level from a starting value corresponding to the WMAP-based prediction (Salaris \& Weiss 2001; Richard et al. 2002; Richard et al. 2005). The earliest calculations (Michaud et al. 1984), as well as recent ones (Salaris \& Weiss 2001), predicted lower lithium abundances for stars at the hot end of the plateau, in contradiction to the observations. Richard and colleagues invoke `turbulent diffusion' with a recipe that restores uniform lithium abundance to the plateau; this extra turbulence could for example be induced by stellar rotation, which would limit the diffusion but not necessarily mix Li to sufficiently high temperatures where it is burnt by nuclear reactions as in the models by Pinsonneault et al. (1999, 2002) and others described above. Richard et al. (2002, 2005 and private communication) have presented detailed calculations of the combined effects of diffusion and a parameterized recipe for turbulent diffusion. The predicted \liseven\ and \lisix\ depletion factors for our program stars based on their calculations are given in Table \ref{t:depletion}. We note that the pre-main sequence depletion factors are likely more uncertain than the main sequence and post-main sequence counterparts (Proffitt \& Michaud 1989). Furthermore, we note that the predictions are presently available only for a very limited number of metallicities, and thus many depletion estimates in Table \ref{t:depletion} are based on extrapolations, which likely introduce further uncertainties, in particular towards higher \feh . For the disk stars HD\,68284 and HD\,130551, in which \lisix\ has been detected (Nissen et al. 1999), we estimate the pre-main sequence \lisix\ depletion to be about 1 dex; these two stars have nearly identical mass and \feh , which explains their similarity in depletion in spite of their \teff\ differences. The following results are pertinent to our discussion. One, there is a recipe for the turbulent diffusion (the so-called T6.25 model) that reduces the Big Bang lithium abundance by $0.4-0.5$\,dex for turn-off stars to the observed value and preserves a largely flat plateau (Richard et al. 2005). Two, simulations suggest that stars of different ages and metallicities may have lithium quite uniformly depleted, but a quantitative comparison with the small scatter reported by us and others was not made. Third, \lisix\ is partly destroyed during the pre-main sequence evolution even without any accompanying \liseven\ destruction; due to the lower \teff\ in general for our higher \feh\ stars, the observed \lisix\ plateau becomes tilted when accounting for this depletion (Fig. \ref{f:li6vsfeh}). Fourth, any substantial \liseven\ destruction is accompanied by an even larger \lisix\ depletion; for example, the T6.25 model which provides a 0.4 dex depletion of \liseven\ predicts 1.6 dex depletion for \lisix\ in LP\,815-43, in addition to about $0.3$\,dex \lisix\ destruction during the pre-main sequence phase. It then follows that the stars with \lisix\ detections began with \logliseven\ $= 2.6$ and \loglisix\ $ \approx 2.6$ too -- not a combination that can be said to reconcile observations with the Big Bang predictions. The choice of a model that provides a smaller \liseven\ depletion also gives a smaller \lisix\ depletion; for example, the T6.09 model reduces \liseven\ by about 0.25 dex (lithium problem is lessened but not eliminated) and \lisix\ by about 0.6 dex including the pre-main sequence destruction (the initial abundance was \loglisix\ $\approx 1.4$). The question is whether alternative recipes for turbulent diffusion can resolve the \liseven\ problem without requiring very high initial \lisix\ abundances. Although no quantitative predictions yet exist for Population II stars, a further promising candidate for Li depletion is internal gravity waves, which lead to angular momentum transport and thus mixing (e.g. Garc\'{\i}a Lop\'{e}z \& Spruit 1991; Talon \& Charbonnel 2004; Charbonnel \& Talon 2005). Recent calculations including these effects successfully reproduce both the quasi-flat solar rotation profile and the degree of Li depletion in disk open clusters as a function of age (Charbonnel \& Talon 2005). We are eagerly awaiting similar modelling for metal-poor stars with predictions for the \liseven\ and \lisix\ depletions, in particular whether large Li depletions can be achieved while still retaining the small observed abundance scatter. Our commentary on rotationally-induced mixing and diffusion shows that plausible (rotationally-induced mixing) and seemingly inevitable (diffusion) processes may solve the \liseven\ problem, but the observers' challenge to fit the Spite plateau's shallow slope with respect to \teff\ and \feh\ and its smoothness are as yet unmet. These potential solutions to the \liseven\ problem indicate that the observed \lisix\ abundance is almost certainly a lower bound to the initial \lisix\ abundance. Some solutions lead to very high initial \lisix\ abundances that, if correct, imply that our understanding of the pre-galactic and Big Bang nucleosynthesis is poor indeed. \subsection{Lithium Production in the Early Universe} \label{s:spallation} \begin{figure} %\resizebox{\hsize}{!}{\includegraphics{figures/Li6vsFeH.eps}} %\resizebox{\hsize}{!}{\includegraphics{figures/Li6vsFeH_depletion.eps}} \resizebox{\hsize}{!}{\includegraphics{f23a.eps}} \resizebox{\hsize}{!}{\includegraphics{f23b.eps}} %\epsscale{0.5} %\plottwo{f23a.eps}{f23b.eps} \caption{{\em Upper panel:} Observed logarithmic abundances of \liseven\ (open triangles) and \lisix\ (solid circles) as a function of \feh\ for our program stars; $3\sigma$ upper limits to the \lisix\ abundances are denoted with arrows. Also shown as open circles are the \lisix\ detections in the halo turn-off star HD\,84937 (Smith et al. 1993, 1998; Cayrel et al. 1999) and in the two Galactic disk stars HD\,68284 and HD\,130551 (Nissen et al. 1999). The large circle correspond to the solar system meteoritic \lisix\ abundance (Asplund et al. 2005), while the horizontal solid line is the predicted \liseven\ abundance from Big Bang nucleosynthesis and the baryon density as determined by WMAP (Spergel et al. 2003; Coc et al. 2004; Cuoco et al. 2004; Cyburt 2004). The (lower) solid, dashed, (lower) dotted and dash-dotted lines correspond to the models for cosmic ray \lisix\ production by Prantzos (2006), Ramaty et al. (2000), Fields \& Olive (1999) and Vangioni-Flam et al. (2000), respectively; see text for details. The higher dotted line shows the \liseven\ abundance assuming the Fields \& Olive model with a \liratioinverse\ production ratio of 1:1.5 and a primordial abundance of \logliseven\,$=2.1$. {\em Lower panel:} Same as in the upper panel but taking into account the predicted pre-main sequence \lisix\ depletion from Richard et al. (2002, 2005; and 2005, private communication) to the observed \lisix\ abundances; these are the minimum values corresponding to negligible \liseven\ depletion (see Sect. \ref{s:depletion} for details).} \label{f:li6vsfeh} \end{figure} The observed \lisix\ abundance is several orders of magnitude larger than that predicted from the standard Big Bang. On the assumption that the standard Big Bang sequence is the correct representation of the primordial fireball, synthesis of \lisix\ is attributed to collisions in the intergalactic or interstellar medium between high-energy particles (cosmic rays) and ambient nuclei. The two leading processes are the $\alpha +\alpha$ fusion reactions and spallation reactions involving protons (also, $\alpha$s) and $^{16}$O (also $^{12}$C and $^{14}$N) nuclei. Both processes also produce \liseven\ with \liratioinverse\,$\sim 1$ to 2 (Mercer et al. 2001). Only the spallation reactions produce $^9$Be, $^{10}$B, and $^{11}$B. In the classical, or direct, Galactic cosmic ray spallation scenario as formulated by Reeves et al. (1970) and Meneguzzi et al. (1971), the accelerated particles are the protons etc hitting ambient interstellar CNO nuclei. As a consequence, this reaction is secondary in nature: \beh\,$\propto$\oh\,$^2$. In inverse spallation the collisions instead occur through fast CNO nuclei and interstellar protons and $\alpha$-particles. Since the CNO nuclei are both produced and accelerated by supernovae, the resulting spallation yields will be essentially independent of the metallicity, a primary process: \beh\,$\propto$\oh . One possible way of achieving this is through superbubbles (Higdon et al. 1998; Parizot \& Drury 1999 but see Prantzos 2005, 2006 for a critique of this scenario): a sequence of supernovae in rapid concession in a cluster or OB association accelerates nuclear-process enriched material. Establishing the behaviour of [O/Fe] with metallicity is clearly important for estimating the spallation production rate but unfortunately no unanimous verdict have appeared to date in this regard (e.g. Israelian et al. 1998, 2001; Boesgaard et al. 1999; Asplund \& Garc\'{\i}a P\'{e}rez 2001; Nissen et al. 2002; Fulbright \& Johnson 2003; Garc\'{\i}a P\'{e}rez et al. 2006). Since spallation reactions are thought to be the sole process by which Be is synthesised and the Be abundance is obtainable for stars on the Spite plateau (Boesgaard et al. 1999; Primas et al., in preparation), the efficiency of a proposed scenario invoking spallation may be rather well calibrated using observed Be abundances. The simultaneous production from the $\alpha + \alpha$ fusion reactions is not simply calibratable. The observed \lisixbe\ ratio shows that the \lisix\ must be produced primarily from the fusion reactions at low metallicities with Be necessarily from spallation; the meteoritic \lisixbe\ ratio ($\approx 6$) is a representative measure of the production ratios for spallation but the ratio is $\approx 40$ for HD\,84937 (Smith et al. 1998) and may reach $\approx 150$ for LP\,815-43 (Primas et al., in preparation). The initial \lisixbe\ ratios were likely even greater due to \lisix\ depletion, underscoring the need for $\alpha + \alpha$ fusion reactions. A large number of Galactic chemical evolution models including spallation and $\alpha$-fusion reactions have been presented in recent years and compared with observed Li, Be and B isotopic abundances (e.g. Yoshii et al. 1997; Fields \& Olive 1999; Parizot 2000; Vangioni-Flam et al. 2000; Ramaty et al. 2000; Suzuki \& Yoshii 2001; Alibes et al. 2002; Prantzos 2005, 2006). Four representative predictions are presented in Fig. \ref{f:li6vsfeh}: the model by Fields \& Olive (1999) is based on direct cosmic ray spallation but with a very steep [O/Fe] trend (Israelian et al. 1998; Boesgaard et al. 1999); the model by Ramaty et al. (2000) is for inverse spallation with special consideration of the energetics of the light element production; the Vangioni-Flam et al. (2000) model is for inverse spallation in superbubbles with an assumed low energy ($\la 30$\,MeV/nucleon) cosmic ray component (Meneguzzi \& Reeves 1975); and the calculations by Prantzos (2006) assume that the cosmic ray composition does not vary with time and that the light isotopes are produced as primaries, i.e. like in the inverse spallation models. These calculations fit about equally well the observed run of the Be abundance with the Fe abundance, although Ramaty et al. (2000) argue that the Fields \& Olive Be production is significantly overestimated through the adoption of unrealistic Fe yields . A fair fit to the observed \lisix\ abundance in HD\,84937 (previously the sole data point for this isotope) when ignoring the inevitable pre-main sequence destruction is achieved for the Fields \& Olive and Vangioni-Flam et al. models but it requires some assumptions to maximise \lisix\ production. There are other problems and difficulties with the calculations: for example, the efficiency assumed for cosmic ray acceleration may be unrealistic given the available kinetic energy from supernovae, which may rule out the low energy cosmic ray scenario (Ramaty et al. 2000; Suzuki \& Yoshii 2001; Prantzos 2005, 2006). Furthermore, several of the spallation models presented here invoke a [O/Fe] trend that is significantly higher than observed by Nissen et al. (2002) and us (Sect. \ref{s:oh}); note that in addition our adopted solar O abundance is $0.1-0.2$\,dex lower than assumed by Fields \& Olive and Ramaty et al. As a consequence, their predicted \lisix\ abundances should be shifted downwards by $\approx 0.3$\,dex for [Fe/H]\,$\le-2$. Finally, the subsequent downward revision by a factor of two of the measured cross-section for $^{6}$Li production by $\alpha$-fusion (Mercer et al. 2001) will further push the predictions to lower yields for all but the Prantzos model. Now that additional \lisix\ detections are available with the high \lisix\ abundance in LP\,815-43 in particular, it is clear that the model calculations do not reproduce the \lisix\ measurements and the apparent observed \lisix\ plateau. Of the here presented models, the one by Prantzos (2006, shown as a solid line in Fig. \ref{f:li6vsfeh}) is likely the most realistic as it requires the least number of assumptions in terms of maximising the production efficiency and is based on the most recent reaction cross-sections. Still we note that it makes the as yet unproven assumption that the cosmic ray composition stays constant with time and thus may well overestimate the \lisix\ production. The discrepancy between models and observations at low \feh\ is further aggravated when accounting for the pre-main sequence \lisix\ depletion of $\ge 0.3$\,dex (Table \ref{t:depletion}), as seen in Fig. \ref{f:li6vsfeh}; invoking any significant amount of \liseven\ depletion would make the situation worse still (Sect. \ref{s:depletion}). The inclusion of \lisix\ pre-main sequence depletion tilts the \lisix\ observations to follow roughly the metallicity-dependence of the models, albeit at a higher \lisix\ abundance; we recall here that the pre-main sequence depletion calculations are rather uncertain and that most of the \lisix\ depletion may in fact take place during the main sequence. At face value, it seems like a remarkable coincidence that the \lisix\ production from cosmic ray spallation and Li-depletion can result in a nearly flat \lisix\ abundance plateau as observed. However, we do note that we are only able to detect \liratio\ ratios of $\ga 0.02$ for observational reasons and thus would not be able to identify the stars in which the depletion is much larger than the corresponding production. A means to boost the light element production over direct and indirect cosmic ray spallation in the interstellar medium has recently been put forward by Nakamura et al. (2006, see also Fields et al. 1996 and Nakamura \& Shigeyama 2004). They speculate that the fast CNO-rich ejecta of very energetic ($\approx 10^{52}~{\rm erg}=10^{45}~{\rm J}$) supernovae having lost all but a small fraction of their H- and He-rich envelopes can interact directly with the circumstellar material without shock acceleration of cosmic rays. Such SNe Ic events may produce significant amounts of primary \lisix\ and \benine\ under suitable conditions. Nakamura et al. (2006) have identified a parameter space that seem to explain the high \lisix /O ratio we observe in LP\,815-43 but it requires some fine-tuning in regards the explosion energy and the amount of available He in the ejecta. It remains to be seen whether real supernovae fulfill these requirements. An additional and alternative scenario places lithium synthesis by $\alpha+\alpha$ fusion reactions during the formation of the Galaxy within the framework of hierarchical structure formation (Suzuki \& Inoue 2002, 2004). Infalling and merging subgalactic clumps would have produced shocks that could have accelerated the $\alpha$-particles at early epochs. Due to our incomplete understanding of the details of galaxy formation, models for the accompanying \lisix\ production by necessity include several free parameters. To achieve the observed high \lisix\ abundances at \feh\,$\le -2.3$ requires strong structure formation shocks to have been in place very early on ($\approx 0.1$\,Gyr after Big Bang) but vanished relatively shortly thereafter ($\approx 0.1$\,Gyr). An argument against this scenario is that mergers in $\Lambda$CDM continue to the present day with only a relatively small dark matter halo present at early times, which would appear to make it difficult for the necessary strong shocks to have formed during the required time interval (Prantzos 2006). Rollinde et al (2005, see also Montmerle 1977) have presented a similar scenario of pre-Galactic production of \lisix\ (and \liseven ) due to an ad-hoc early burst of cosmological cosmic rays, possibly due to Population III stars. The energetics of such a production were not investigated. Prantzos (2006) also speculate that accretion to a supermassive black hole such as the one believed to exist currently in the Galactic center could generate sufficient energy to accelerate the necessary cosmic rays. This scenario requires some extreme assumptions about the time of its formation and its efficiency in converting accretion energy to particle acceleration to produce sufficient \lisix\ at \feh\,$\approx -2.7$. The final potential site for \lisix\ synthesis is the Big Bang. In a standard Big Bang much too little \lisix\ is produced to explain our observations. An extension of the standard model for particle physics such as supersymmetry predicts the existence of various exotic particles, including the gravitino, axion and the neutralino; the first two of these particles are predicted to be unstable but the neutralino is likely stable. The decay and the annihilation during or shortly after the era of Big Bang nucleosynthesis can alter the resulting light element abundances, provided the masses and life-times of these putative particles are right (e.g. Dimopoulos et al. 1988; Jedamzik 2000, 2004a,b, 2005; Kawasaki et al. 2004; Ichikawa et al. 2004). The annihilation of the neutralino can release sufficient energy to produce \lisix\ by non-thermal reactions like $^3$H($\alpha$,n)\lisix\ and $^3$He($\alpha$,p)\lisix\ (Jedamzik 2004a). The amount of \lisix\ produced depends on the mass of the neutralino and the exact annihilation channels but can reach the levels observed in some of our very metal-poor stars; this scenario does not, however, resolve the \liseven\ dilemma described above. Another option to produce \lisix\ is through the decay of particles like the gravitino and axion. While the electromagnetic decay routes of such particles result in $^3$He/D ratios inconsistent with observations (Ellis et al. 2005), the injection of energetic nucleons through the hadronic decay about $10^3$\,s after Big Bang can lead to substantial \lisix\ production without spoiling the agreement with D and the He isotopes. Indeed, for the right combination of particle properties, a simultaneous production of \lisix\ and destruction of \liseven\ appears achievable and may explain both the observed \lisix\ plateau and the low \liseven\ abundances in comparison with standard Big Bang nucleosynthesis (Jedamzik 2004b, 2005). Thus, both of the Li problems can conceivably be solved at the same time. While these idea are very attractive, they rests on as yet unproven and speculative physics. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \section{Concluding Remarks} \label{s:conclusions} Remarkable as it may have seemed in 1982 following the discovery of the Spite plateau and the near-universal association of the plateau's lithium abundance with primordial nucleosynthesis, the debate over that association has not been stilled. Two key recent factors heating the debate have been the measurement of the Big Bang's photon-to-baryon ratio ($\eta$) using the WMAP measurements of the anisotropies in the cosmic microwave background and the detections, here and previously, of the lighter isotope $^6$Li. A standard model of the Big Bang with the WMAP estimate of $\eta$ predicts a lithium ($^7$Li) abundance greater by about 0.5 dex than the value generally attributed to the Spite plateau, and a $^6$Li abundance several orders of magnitude below the value reported here. These two discrepancies resist simple resolution, as should be clear from the discussion in Section 7. One supposes that resolution of the discrepancies may be found in one or more of the following three areas: \smallskip \noindent {\em 1. Composition of the gas from which stars on the Spite plateau formed} \noindent Ignoring the possibility that the $^6$Li was synthesised after the formation of the star, a conjecture is that $^6$Li was synthesised either in a non-standard Big Bang (e.g., hadronic decays of exotic particles resulting in post-processing the $^7$Li from a standard Big Bang) or through $\alpha - \alpha$ fusion reactions in the proto-Galaxy (e.g. hierarchical structure formation shocks and/or supermassive black holes). Introduction of a non-standard Big Bang may lower the predicted $^7$Li abundance and increase the predicted $^6$Li abundance. Qualitatively, these changes resolve both discrepancies provided that points 2 and 3 below do not come into play. Addition of lithium synthesis from fusion reactions in pre-Galactic gas, as the sole additional site over a standard Big Bang, may remove the $^6$Li discrepancy but may aggravate the discrepancy between the predicted $^7$Li abundance and the observed abundance, unless one adopts the heresy that the WMAP estimate of $\eta$ should be replaced by the lower value that results in the minimum synthesis of $^7$Li. (The nuclear reaction network appears to be free of significant uncertainties.) \smallskip \noindent {\em 2. Relationship between the stars' initial composition set 10 -- 13 Gyr ago and the present composition of their stellar atmospheres} \noindent There is tension on this point between those who stress the significance of the observed very small scatter of the lithium abundances along the Spite plateau and those who identify physical processes that ought to change the atmospheric compositions of plateau residents (Section 7.4). The very small scatter would seem to imply that the change in surface lithium abundance has been itself slight. Yet, some argue that reduction of the lithium abundance through diffusion, perhaps supplemented by rotationally-induced mixing and other processes, must occur but can result in a small star-to-star scatter of lithium abundances. The presence of $^6$Li, as we noted, complicates interpretations that rely on depletion/destruction of $^7$Li to reduce the WMAP-based Big Bang $^7$Li abundance to the observed value for the Spite plateau; very high to extraordinarily high initial $^6$Li abundances may be implied. There are clearly open questions for pursuit by observers. Diffusion does not exclusively act on lithium. Relative abundances of abundant elements are changed but these elements are not subject to destruction as lithium is. Alterations of the abundances are lessened and then removed as stars evolve from the main sequence to subgiants and then to giants. Careful comparisons of stars along this sequence might confirm that diffusion was operable in their main sequence progenitors. At present, abundance data from dwarfs and giants have given seemingly consistent results for composition as a function of metallicity, i.e., the same run of [X/Fe] versus [Fe/H] (e.g. Gratton et al. 2001). \smallskip \noindent {\em 3. Measurement of the present $^6$Li and $^7$Li abundances} \noindent Systematic errors are now unlikely to be uncovered that will lift the Spite plateau's lithium abundance by the 0.5 dex to match the Big Bang WMAP-based abundance (Section 7.1). The adjustments (e.g, the necessary increase of effective temperatures by about 700\,K) unless specific to lithium would result in large changes to abundances of other elements. Presently, there is generally good agreement between the compositions of metal-poor dwarfs and giants of the same metallicity and this agreement would be compromised unless adjustments were also made to the abundance analyses of giants with their very different atmospheric structures. The simplest conceivable adjustment -- raising the effective temperatures by 700 K -- introduces more problems than the one it solves. Absence of systematic errors affecting the determinaton of the $^6$Li/$^7$Li ratio cannot be so strongly dismissed: the presence of $^6$Li is deduced from a slight additional asymmetry to the intrinsically asymmetric $^7$Li line. The various tests outlined in Sect. \ref{s:li6708} give confidence that $^6$Li has indeed been detected. This confidence should be tested by observations of additional stars like HD\,19445 for which pre-main sequence destruction of $^6$Li is so great that this isotope should be undetectable. Obviously, additional \lisix\ observations at very low \feh\ would be extremely valuable, including a confirmation of our detection in LP\,815-43. The confidence commonly and frequently expressed after 1982 that primordial lithium had been discovered and measured and could be matched with a prediction from a standard Big Bang is today weakened. There remains a belief that much of the lithium is traceable to primordial nucleosynthesis but quantitative agreement between prediction and observation of the $^6$Li and $^7$Li abundances in stars on the Spite plateau is proving elusive. Observers will suppose that well designed additional spectroscopic analyses of metal-poor stars will provide some of the clues necessary to determining the primordial abundance of the two lithium isotopes. Theoreticians may combine these clues with other evidence and probe deeper into primordial nucleosynthesis. Interest in the lithium of the Spite plateau is greater than in 1982, even as the lack of concordance between predictions of the standard Big Bang and measured lithium abundances has been demonstrated. %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \acknowledgements This paper has benefitted from helpful assistance, illuminating discussions and penetrating questions from numerous colleagues, including Paul Barklem, Lars Bergstr\"om, Corinne Charbonnel, Bengt Gustafsson, Susume Inoue, Karsten Jedamzik, Georges Michaud, John Norris, Keith Olive, Olivier Richard, Gary Steigman, Elisabeth Vangioni and Achim Weiss. We thank Wako Aoki for kindly providing the Subaru spectrum of HD\,140283 for an independent analysis and Piercarlo Bonifacio for sharing the results of the First Stars program prior to publication. This work has been supported by the Australian Research Council through the grants DP0342613 and DP0558836. DLL acknowledges the support of the Robert A. Welch Foundation of Houston, Texas. \newpage %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{thebibliography}{} \bibitem[1966]{ali66} Ali, A.W., \& Griem, H.R. 1966, Phys. 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It accepts BibTeX % output intended for many other packages, and therefore acts as a % general, all-purpose citation-style interface. % % With standard numerical .bst files, only numerical citations are % possible. With an author-year .bst file, both numerical and % author-year citations are possible. % % If author-year citations are selected, \bibitem must have one of the % following forms: % \bibitem[Jones et al.(1990)]{key}... % \bibitem[Jones et al.(1990)Jones, Baker, and Williams]{key}... % \bibitem[Jones et al., 1990]{key}... % \bibitem[\protect\citeauthoryear{Jones, Baker, and Williams}{Jones % et al.}{1990}]{key}... % \bibitem[\protect\citeauthoryear{Jones et al.}{1990}]{key}... % \bibitem[\protect\astroncite{Jones et al.}{1990}]{key}... % \bibitem[\protect\citename{Jones et al., }1990]{key}... % \harvarditem[Jones et al.]{Jones, Baker, and Williams}{1990}{key}... % % This is either to be made up manually, or to be generated by an % appropriate .bst file with BibTeX. % Author-year mode || Numerical mode % Then, \citet{key} ==>> Jones et al. (1990) || Jones et al. [21] % \citep{key} ==>> (Jones et al., 1990) || [21] % Multiple citations as normal: % \citep{key1,key2} ==>> (Jones et al., 1990; Smith, 1989) || [21,24] % or (Jones et al., 1990, 1991) || [21,24] % or (Jones et al., 1990a,b) || [21,24] % \cite{key} is the equivalent of \citet{key} in author-year mode % and of \citep{key} in numerical mode % Full author lists may be forced with \citet* or \citep*, e.g. % \citep*{key} ==>> (Jones, Baker, and Williams, 1990) % Optional notes as: % \citep[chap. 2]{key} ==>> (Jones et al., 1990, chap. 2) % \citep[e.g.,][]{key} ==>> (e.g., Jones et al., 1990) % \citep[see][pg. 34]{key}==>> (see Jones et al., 1990, pg. 34) % (Note: in standard LaTeX, only one note is allowed, after the ref. % Here, one note is like the standard, two make pre- and post-notes.) % \citealt{key} ==>> Jones et al. 1990 % \citealt*{key} ==>> Jones, Baker, and Williams 1990 % \citealp{key} ==>> Jones et al., 1990 % \citealp*{key} ==>> Jones, Baker, and Williams, 1990 % Additional citation possibilities (both author-year and numerical modes) % \citeauthor{key} ==>> Jones et al. % \citeauthor*{key} ==>> Jones, Baker, and Williams % \citeyear{key} ==>> 1990 % \citeyearpar{key} ==>> (1990) % \citetext{priv. comm.} ==>> (priv. comm.) % Note: full author lists depends on whether the bib style supports them; % if not, the abbreviated list is printed even when full requested. % % For names like della Robbia at the start of a sentence, use % \Citet{dRob98} ==>> Della Robbia (1998) % \Citep{dRob98} ==>> (Della Robbia, 1998) % \Citeauthor{dRob98} ==>> Della Robbia % % % Citation aliasing is achieved with % \defcitealias{key}{text} % \citetalias{key} ==>> text % \citepalias{key} ==>> (text) % % Defining the citation style of a given bib style: % Use \bibpunct (in the preamble only) with 6 mandatory arguments: % 1. opening bracket for citation % 2. closing bracket % 3. citation separator (for multiple citations in one \cite) % 4. the letter n for numerical styles, s for superscripts % else anything for author-year % 5. punctuation between authors and date % 6. punctuation between years (or numbers) when common authors missing % One optional argument is the character coming before post-notes. It % appears in square braces before all other arguments. May be left off. % Example (and default) \bibpunct[, ]{(}{)}{;}{a}{,}{,} % % To make this automatic for a given bib style, named newbib, say, make % a local configuration file, natbib.cfg, with the definition % \newcommand{\bibstyle@newbib}{\bibpunct...} % Then the \bibliographystyle{newbib} will cause \bibstyle@newbib to % be called on THE NEXT LATEX RUN (via the aux file). % % Such preprogrammed definitions may be invoked in the text (preamble only) % by calling \citestyle{newbib}. This is only useful if the style specified % differs from that in \bibliographystyle. % % With \citeindextrue and \citeindexfalse, one can control whether the % \cite commands make an automatic entry of the citation in the .idx % indexing file. For this, \makeindex must also be given in the preamble. % % LaTeX2e Options: (for selecting punctuation) % round - round parentheses are used (default) % square - square brackets are used [option] % curly - curly braces are used {option} % angle - angle brackets are used