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nam
2013-03-04 14:13:31 +09:00
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ALL: poster2.pdf
%.pdf: %.tex Makefile *.sty
#pdflatex --enable-write18 $< && pdflatex $< && pdflatex $<
pdflatex $<
clean:
rm -f *.aux *.bbl *.blg *.log poster.pdf *.nav *.out *.snm *.toc

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AEPSHEPposter/beamerposter.org.sty Executable file
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% Copyright 2007 by
% Philippe Dreuw <dreuw@cs.rwth-aachen.de> and
% Thomas Deselaers <deselaers@cs.rwth-aachen.de>
% Slight modifications made in August 2009 by Nathaniel Johnston (nathaniel@nathanieljohnston.com)
%
% This file may be distributed and/or modified
%
% 1. under the LaTeX Project Public License and/or
% 2. under the GNU Public License.
%
%
% ChangeLog:
%
% 1.07 - bugfixed custom size handling, portrait or landscape settings are ignored now
% 1.06 - added the type1cm package for scalable math fonts
% 1.05 - added version check for xkeyval package
% 1.04 - added custom size handling
% 1.03 - improved predefined size handling
% 1.02 - minor bugfixes
% 1.01 - bugfixed size handling
% 1.00 - first beamerposter release
%
\def\beamerposter@version{1.07}
\def\beamerposter@date{2008/03/11}
\def\beamerposter@msg{beamerposter: latex-beamer poster extension}
\typeout{Package: \beamerposter@date. v.\beamerposter@version. \beamerposter@msg}
\NeedsTeXFormat{LaTeX2e}
\ProvidesPackage{beamerposter}[\beamerposter@date. v.\beamerposter@version. \beamerposter@msg]
\RequirePackage{xkeyval}[2006/11/18]
\RequirePackage{type1cm} %% get it from ftp://cam.ctan.org/tex-archive/macros/latex/contrib/type1cm.zip
\newif\ifportrait
\newif\ifcustomsize
\newif\ifdebug
\DeclareOptionX{size}[a0]{
\typeout{beamerposter: checking size input, please wait.}
\XKV@cc*+[\val\nr]{#1}{a0b,a0,a1,a2,a3,a4,custom}{%
\typeout{beamerposter: the input \val\ \nr\ was correct, we proceed.}
\ifcase\nr\relax
%a0b
\setlength{\paperwidth}{119cm}
\setlength{\paperheight}{88cm}
\setlength{\textwidth}{116cm}
\setlength{\textheight}{88cm}
\or
%a0
\setlength{\paperwidth}{118.82cm}
\setlength{\paperheight}{83.96cm}
\setlength{\textwidth}{117.82cm}
\setlength{\textheight}{82.96cm}
\or
%a1
\setlength{\paperwidth}{83.96cm}
\setlength{\paperheight}{59.4cm}
\setlength{\textwidth}{82.96cm}
\setlength{\textheight}{58.4cm}
\or
%a2
\setlength{\paperwidth}{59.4cm}
\setlength{\paperheight}{41.98cm}
\setlength{\textwidth}{58.4cm}
\setlength{\textheight}{40.98cm}
\or
%a3
\setlength{\paperwidth}{41.98cm}
\setlength{\paperheight}{29.7cm}
\setlength{\textwidth}{40.98cm}
\setlength{\textheight}{28.7cm}
\or
%a4
\setlength{\paperwidth}{29.7cm}
\setlength{\paperheight}{21.0cm}
\setlength{\textwidth}{28.7cm}
\setlength{\textheight}{20.0cm}
\or
\customsizetrue
\fi
}{%
\PackageWarning{beamerposter}{the input \val\ was incorrect and was ignored.}
}%
\typeout{beamerposter: finished size input check.}
}
\DeclareOptionX{orientation}[portrait]{
\typeout{beamerposter: checking orientation input, please wait.}
\XKV@cc*+[\val\nr]{#1}{portrait,landscape}{%
\typeout{beamerposter: the input \val\ \nr\ was correct, we proceed.}
\ifcase\nr\relax
\portraittrue
\or
\portraitfalse
\fi
}{%
\PackageWarning{beamerposter}{the input \val\ was incorrect and was ignored.}
}%
\typeout{beamerposter: finished orientation check.}
}
\DeclareOptionX{scale}[1.0]{\edef\myfontscale{#1}\typeout{beamerposter: myfontscale=\myfontscale}}
\DeclareOptionX{width}{\edef\customwidth{#1}\typeout{beamerposter: custom poster width=\customwidth}}
\DeclareOptionX{height}{\edef\customheight{#1}\typeout{beamerposter: custom poster height=\customheight}}
\DeclareOptionX{debug}{\typeout{beamerposter: enabled debug mode}\debugtrue}
\DeclareOptionX*{\PackageWarning{beamerposter}{Unknown option ignored: \CurrentOption}}
%\DeclareOptionX*{\PassOptionsToClass{\CurrentOption}{beamer}}
\ExecuteOptionsX{size=a0,scale=1.0}
\ProcessOptionsX\relax
\ifdebug
\RequirePackage[debug]{fp}
\else
\RequirePackage{fp}
\fi
%% swap sizes for portrait orientation
\ifportrait
\newdimen\tmp
\setlength{\tmp}{\paperwidth}
\setlength{\paperwidth}{\paperheight}
\setlength{\paperheight}{\tmp}
\setlength{\tmp}{\textwidth}
\setlength{\textwidth}{\textheight}
\setlength{\textheight}{\tmp}
\else\relax
\fi
%% overwrite dimensions if custom size
\ifcustomsize
\setlength{\paperwidth}{\customwidth cm}
\setlength{\paperheight}{\customheight cm}
\FPupn{\resulttextwidth}{1 customwidth -}
\FPupn{\resulttextheight}{1 customheight -}
\setlength{\textwidth}{\resulttextwidth cm}
\setlength{\textheight}{\resulttextheight cm}
\fi
%% Setting proper dimensions for a DIN A0 printer
\setlength{\headheight}{0 cm}
\setlength{\headsep}{0 cm}
\setlength{\topmargin}{-12.7 mm} % -1in +1.47cm
\setlength{\oddsidemargin}{-25.4 mm} % -1in +0.4cm
%% For the page layout
\ifdebug
\typeout{beamerposter: paperwidth=\the\paperwidth, paperheight=\the\paperheight}
\typeout{beamerposter: textwidth=\the\textwidth, textwidth=\the\textheight}
\fi
\geometry{
paperwidth=\the\paperwidth,
paperheight=\the\paperheight,
hmargin=1cm,%
vmargin=0cm,%
head=0.5cm, %
headsep=0pt,%
foot=0.5cm %
}
%% scalable vector fonts
\edef\fontSizeX{14.4}\edef\fontSizeY{18}
\FPupn{\resultscriptsizeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultscriptsizeY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\tiny}{\fontsize{\resultscriptsizeX}{\resultscriptsizeY}\selectfont}
\edef\fontSizeX{17.28}\edef\fontSizeY{22}
\FPupn{\resultfootnotesizeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultfootnotesizeY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\scriptsize}{\fontsize{\resultfootnotesizeX}{\resultfootnotesizeY}\selectfont}
\edef\fontSizeX{20.74}\edef\fontSizeY{25}
\FPupn{\resultsmallX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultsmallY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\footnotesize}{\fontsize{\resultsmallX}{\resultsmallY}\selectfont}
\edef\fontSizeX{24.88}\edef\fontSizeY{30}
\FPupn{\resultnormalsizeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultnormalsizeY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\small}{\fontsize{\resultnormalsizeX}{\resultnormalsizeY}\selectfont}
\edef\fontSizeX{29.86}\edef\fontSizeY{37}
\FPupn{\resultlargeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultlargeY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\normalsize}{\fontsize{\resultlargeX}{\resultlargeY}\selectfont}
\edef\fontSizeX{35.83}\edef\fontSizeY{45}
\FPupn{\resultLargeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultLargeY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\large}{\fontsize{\resultLargeX}{\resultLargeY}\selectfont}
\edef\fontSizeX{43}\edef\fontSizeY{54}
\FPupn{\resultLARGEX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultLARGEY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\Large}{\fontsize{\resultLARGEX}{\resultLARGEY}\selectfont}
\edef\fontSizeX{51.6}\edef\fontSizeY{64}
\FPupn{\resulthugeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resulthugeY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\LARGE}{\fontsize{\resulthugeX}{\resulthugeY}\selectfont}
\edef\fontSizeX{61.92}\edef\fontSizeY{77}
\FPupn{\resultHugeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultHugeY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\huge}{\fontsize{\resultHugeX}{\resultHugeY}\selectfont}
\edef\fontSizeX{74.3}\edef\fontSizeY{93}
\FPupn{\resultveryHugeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultveryHugeY}{myfontscale fontSizeY * 2 round}
\renewcommand*{\Huge}{\fontsize{\resultveryHugeX}{\resultveryHugeY}\selectfont}
\edef\fontSizeX{80.3}\edef\fontSizeY{101}
\FPupn{\resultVeryHugeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultVeryHugeY}{myfontscale fontSizeY * 2 round}
\newcommand*{\veryHuge}{\fontsize{\resultVeryHugeX}{\resultVeryHugeY}\selectfont}
\edef\fontSizeX{107}\edef\fontSizeY{134}
\FPupn{\resultVERYHugeX}{myfontscale fontSizeX * 2 round}
\FPupn{\resultVERYHugeY}{myfontscale fontSizeY * 2 round}
\newcommand*{\VeryHuge}{\fontsize{\resultVERYHugeX}{\resultVERYHugeY}\selectfont}
% set the normalfont (default)
\renewcommand*{\normalfont}{\normalsize}

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AEPSHEPposter/beamerthemeconfposter.sty Executable file
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%==============================================================================
% Beamer style for the poster template posted at
% http://www.nathanieljohnston.com/2009/08/latex-poster-template/
%
% Created by the Computational Physics and Biophysics Group at Jacobs University
% https://teamwork.jacobs-university.de:8443/confluence/display/CoPandBiG/LaTeX+Poster
% Modified by Nathaniel Johnston (nathaniel@nathanieljohnston.com) in August 2009
% Modified by Tran Hoai Nam in 2012-10-09, adapt for A0 size
% =============================================================================
\ProvidesPackage{beamerthemeconfposter}
\RequirePackage{tikz} % for drawing the nice rounded boxes
\usetikzlibrary{arrows,backgrounds}
\RequirePackage[T1]{fontenc}
\RequirePackage{lmodern}
\RequirePackage{textcomp}
\RequirePackage{amsmath,amssymb}
\usefonttheme{professionalfonts}
\newcommand{\makeruleinbox}{{\usebeamercolor[bg]{block alerted title}\centering\hspace*{-0.7cm}\rule{\inboxrule}{0.5cm}}}
\usepackage{ragged2e}
%-----------------------------------------------------------
% Define a whole bunch of custom colours and fonts
%-----------------------------------------------------------
\definecolor{lgreen} {RGB}{180,210,100}
\definecolor{dblue} {RGB}{20,66,129}
\definecolor{ddblue} {RGB}{11,36,69}
\definecolor{lred} {RGB}{220,0,0}
\definecolor{nred} {RGB}{224,0,0}
\definecolor{norange}{RGB}{230,120,20}
\definecolor{nyellow}{RGB}{255,221,0}
\definecolor{ngreen} {RGB}{98,158,31}
\definecolor{dgreen} {RGB}{78,138,21}
\definecolor{nblue} {RGB}{28,130,185}
\definecolor{jblue} {RGB}{20,50,100}
%----------------------------------------------------------------------------
% More colours added due to conflict with Colordvi package
% Addition done by Nishan Mudalige (math.mudalige@uoguelph.ca) in April 2011
%----------------------------------------------------------------------------
\definecolor{GreenYellow} {RGB}{217, 229, 6} % GreenYellow Approximate PANTONE 388
\definecolor{Yellow} {RGB}{254, 223, 0} % Yellow Approximate PANTONE YELLOW
\definecolor{Goldenrod} {RGB}{249, 214, 22} % Goldenrod Approximate PANTONE 109
\definecolor{Dandelion} {RGB}{253, 200, 47} % Dandelion Approximate PANTONE 123
\definecolor{Apricot} {RGB}{255, 170, 123} % Apricot Approximate PANTONE 1565
\definecolor{Peach} {RGB}{255, 127, 69} % Peach Approximate PANTONE 164
\definecolor{Melon} {RGB}{255, 129, 141} % Melon Approximate PANTONE 177
\definecolor{YellowOrange} {RGB}{240, 171, 0} % YellowOrange Approximate PANTONE 130
\definecolor{Orange} {RGB}{255, 88, 0} % Orange Approximate PANTONE ORANGE-021
\definecolor{BurntOrange} {RGB}{199, 98, 43} % BurntOrange Approximate PANTONE 388
\definecolor{Bittersweet} {RGB}{189, 79, 25} % Bittersweet Approximate PANTONE 167
\definecolor{RedOrange} {RGB}{222, 56, 49} % RedOrange Approximate PANTONE 179
\definecolor{Mahogany} {RGB}{152, 50, 34} % Mahogany Approximate PANTONE 484
\definecolor{Maroon} {RGB}{152, 30, 50} % Maroon Approximate PANTONE 201
\definecolor{BrickRed} {RGB}{170, 39, 47} % BrickRed Approximate PANTONE 1805
\definecolor{Red} {RGB}{255, 0, 0} % Red Approx PANTONE LUMINOUS VIVID RED
\definecolor{BrilliantRed} {RGB}{237, 41, 57} % Red VERY-Approx PANTONE RED
\definecolor{OrangeRed} {RGB}{231, 58, 0} % OrangeRed No PANTONE match (TRIED PANTONE VIVID ORANGE RED)
\definecolor{RubineRed} {RGB}{202, 0, 93} % RubineRed Approximate PANTONE RUBINE-RED
\definecolor{WildStrawberry} {RGB}{203, 0, 68} % WildStrawberry Approximate PANTONE 206
\definecolor{Salmon} {RGB}{250, 147, 171} % Salmon Approximate PANTONE 183
\definecolor{CarnationPink} {RGB}{226, 110, 178} % CarnationPink Approximate PANTONE 218
\definecolor{Magenta} {RGB}{255, 0, 144} % Magenta Approximate PANTONE PROCESS-MAGENTA
\definecolor{VioletRed} {RGB}{215, 31, 133} % VioletRed Approximate PANTONE 219
\definecolor{Rhodamine} {RGB}{224, 17, 157} % Rhodamine Approximate PANTONE RHODAMINE-RED
\definecolor{Mulberry} {RGB}{163, 26, 126} % Mulberry Approximate PANTONE 241
\definecolor{RedViolet} {RGB}{161, 0, 107} % RedViolet Approximate PANTONE 234
\definecolor{Fuchsia} {RGB}{155, 24, 137} % Fuchsia Approximate PANTONE 248
\definecolor{Lavender} {RGB}{240, 146, 205} % Lavender Approximate PANTONE 223
\definecolor{Thistle} {RGB}{222, 129, 211} % Thistle Approximate PANTONE 245
\definecolor{Orchid} {RGB}{201, 102, 205} % Orchid Approximate PANTONE 252
\definecolor{DarkOrchid} {RGB}{153, 50, 204} % DarkOrchid No PANTONE match
\definecolor{Purple} {RGB}{182, 52, 187} % Purple Approximate PANTONE PURPLE
\definecolor{Plum} {RGB}{79, 50, 76} % Plum VERY-Approx PANTONE 518
\definecolor{Violet} {RGB}{75, 8, 161} % Violet Approximate PANTONE VIOLET
\definecolor{RoyalPurple} {RGB}{82, 35, 152} % RoyalPurple Approximate PANTONE 267
\definecolor{BlueViolet} {RGB}{33, 7, 106} % BlueViolet Approximate PANTONE 2755
\definecolor{Periwinkle} {RGB}{136, 132, 213} % Periwinkle Approximate PANTONE 2715
\definecolor{CadetBlue} {RGB}{95, 158, 160} % CadetBlue Approximate PANTONE (534+535)/2, Could not find get on my own so used PANTONE-CADET BLUE
\definecolor{CornflowerBlue} {RGB}{99, 177, 229} % CornflowerBlue Approximate PANTONE 292
\definecolor{MidnightBlue} {RGB}{0, 65, 101} % MidnightBlue Approximate PANTONE 302
\definecolor{NavyBlue} {RGB}{0, 70, 173} % NavyBlue Approximate PANTONE 293
\definecolor{RoyalBlue} {RGB}{0, 35, 102} % RoyalBlue No PANTONE match
\definecolor{Blue} {RGB}{0, 24, 168} % Blue Approximate PANTONE BLUE-072
\definecolor{Cerulean} {RGB}{0, 122, 201} % Cerulean Approximate PANTONE 3005
\definecolor{Cyan} {RGB}{0, 159, 218} % Cyan Approximate PANTONE PROCESS-CYAN
\definecolor{ProcessBlue} {RGB}{0, 136, 206} % ProcessBlue Approximate PANTONE PROCESS-BLUE
\definecolor{SkyBlue} {RGB}{91, 198, 232} % SkyBlue Approximate PANTONE 2985
\definecolor{Turquoise} {RGB}{0, 255, 239} % Turquoise Approximate PANTONE (312+313)/2, Could not find get on my own so used PANTONE-TURQUOISE
\definecolor{TealBlue} {RGB}{0, 124, 146} % TealBlue Approximate PANTONE 3145
\definecolor{Aquamarine} {RGB}{0, 148, 179} % Aquamarine Approximate PANTONE 3135
\definecolor{BlueGreen} {RGB}{0, 154, 166} % BlueGreen Approximate PANTONE 320
\definecolor{Emerald} {RGB}{80, 200, 120} % Emerald No PANTONE match
\definecolor{JungleGreen} {RGB}{0, 115, 99} % JungleGreen Approximate PANTONE 328
\definecolor{SeaGreen} {RGB}{0, 176, 146} % SeaGreen Approximate PANTONE 3268
\definecolor{Green} {RGB}{0, 173, 131} % Green VERY-Approx PANTONE GREEN
\definecolor{ForestGreen} {RGB}{0, 105, 60} % ForestGreen Approximate PANTONE 349
\definecolor{PineGreen} {RGB}{0, 98, 101} % PineGreen Approximate PANTONE 323
\definecolor{LimeGreen} {RGB}{50, 205, 50} % LimeGreen No PANTONE match
\definecolor{YellowGreen} {RGB}{146, 212, 0} % YellowGreen Approximate PANTONE 375
\definecolor{SpringGreen} {RGB}{201, 221, 3} % SpringGreen Approximate PANTONE 381
\definecolor{OliveGreen} {RGB}{135, 136, 0} % OliveGreen Approximate PANTONE 582
\definecolor{RawSienna} {RGB}{149, 82, 20} % RawSienna Approximate PANTONE 154
\definecolor{Sepia} {RGB}{98, 60, 27} % Sepia Approximate PANTONE 161
\definecolor{Brown} {RGB}{134, 67, 30} % Brown Approximate PANTONE 1615
\definecolor{Tan} {RGB}{210, 180, 140} % Tan No PANTONE match
\definecolor{Gray} {RGB}{139, 141, 142} % Gray Approximate PANTONE COOL-GRAY-8
\definecolor{Black} {RGB}{30, 30, 30} % Black Approximate PANTONE PROCESS-BLACK
\definecolor{White} {RGB}{255, 255, 255} % White No PANTONE match
% set the basic colors
\setbeamercolor{palette primary} {fg=black,bg=white}
\setbeamercolor{palette secondary} {fg=black,bg=white}
\setbeamercolor{palette tertiary} {bg=jblue,fg=white}
\setbeamercolor{palette quaternary}{fg=black,bg=white}
\setbeamercolor{structure}{fg=jblue}
\setbeamercolor{titlelike} {bg=jblue,fg=white}
\setbeamercolor{frametitle} {bg=jblue!10,fg=jblue}
\setbeamercolor{cboxb}{fg=black,bg=jblue}
\setbeamercolor{cboxr}{fg=black,bg=red}
% set colors for itemize/enumerate
\setbeamercolor{item}{fg=ngreen}
\setbeamercolor{item projected}{fg=white,bg=ngreen}
% set colors for blocks
\setbeamercolor{block title}{fg=ngreen,bg=white}
\setbeamercolor{block body}{fg=black,bg=white}
% set colors for alerted blocks (blocks with frame)
\setbeamercolor{block alerted title}{fg=white,bg=jblue}
\setbeamercolor{block alerted body}{fg=black,bg=jblue!10}
% set the fonts
\setbeamerfont{section in head/foot}{series=\bfseries}
\setbeamerfont{block title}{series=\bfseries}
\setbeamerfont{block alerted title}{series=\bfseries}
\setbeamerfont{frametitle}{series=\bfseries}
\setbeamerfont{frametitle}{size=\Large}
\setbeamerfont{block body}{series=\rmfamily}
% set some beamer theme options
\setbeamertemplate{title page}[default][colsep=-4bp,rounded=true]
\setbeamertemplate{sections/subsections in toc}[square]
\setbeamertemplate{items}[circle]
\setbeamertemplate{blocks}[width=0.0]
\beamertemplatenavigationsymbolsempty
% set bibliography style
\setbeamertemplate{bibliography item}[text]
\setbeamercolor{bibliography item}{fg=black,bg=white}
\setbeamercolor{bibliography entry author}{fg=black,bg=white}
\setbeamercolor{bibliography item}{fg=black,bg=white}
% define some length variables that are used by the template
\newlength{\inboxwd}
\newlength{\iinboxwd}
\newlength{\inboxrule}
\makeatletter
\makeatother
%==============================================================================
% build the poster title
%==============================================================================
\setbeamertemplate{headline}{
\leavevmode
\begin{columns}
\begin{column}{\linewidth}
\vskip1cm
\centering
\usebeamercolor{title in headline}{\color{jblue}\Huge{\textbf{\inserttitle}}\\[0.5ex]}
\usebeamercolor{author in headline}{\color{fg}\Large{\insertauthor}\\[1ex]}
\usebeamercolor{institute in headline}{\color{fg}\large{\insertinstitute}\\[1ex]}
\vskip1cm
\end{column}
\vspace{1cm}
\end{columns}
\vspace{0.5in}
%this is the original one, for 48x36 in poster
%\hspace{0.5in}\begin{beamercolorbox}[wd=47in,colsep=0.15cm]{cboxb}\end{beamercolorbox}
%modified version for landscape A0 size: 1189X814 mm
\hspace{12mm}\begin{beamercolorbox}[wd=1165mm,colsep=0.15cm]{cboxb}\end{beamercolorbox}
%modified version for portrait A1 size: 841 X 594 mm
%\hspace{12mm}\begin{beamercolorbox}[wd=570mm,colsep=0.15cm]{cboxb}\end{beamercolorbox}
\vspace{0.1in}
}
% Block definition
\setbeamertemplate{block begin}
{
\par\vskip\medskipamount
\begin{beamercolorbox}[colsep*=0ex,dp={2ex},center]{block title}
\vskip-0.25cm
\usebeamerfont{block title}\large\insertblocktitle
\begin{flushleft}
\vskip-1cm
\begin{tikzpicture}[remember picture,overlay]
\shade [inner color=gray,outer color=white]
(0,0) rectangle (\textwidth,0.3cm);
\end{tikzpicture}
\end{flushleft}
\end{beamercolorbox}
{\parskip0pt\par}
\ifbeamercolorempty[bg]{block title}
{}
{\ifbeamercolorempty[bg]{block body}{}{\nointerlineskip\vskip-0.5pt}}
\usebeamerfont{block body}
\vskip-0.5cm
\begin{beamercolorbox}[colsep*=0ex,vmode]{block body}
\justifying
}
\setbeamertemplate{block end}
{
\end{beamercolorbox}
\vskip\smallskipamount
}
% Alert block definition (with frame)
\setbeamertemplate{block alerted begin}
{
\par\vskip\medskipamount
\begin{beamercolorbox}[sep=0ex,rounded=true,center,dp={2ex}]{block alerted title}
\vskip0.01cm
\usebeamerfont{block title}\large\insertblocktitle
\end{beamercolorbox}
{\parskip0pt\par}
\usebeamerfont{block body}
\vskip-0.8cm
\begin{beamercolorbox}[sep=0.5cm, rounded=true,center]{block alerted title}
\setlength{\inboxwd}{\linewidth}
\addtolength{\inboxwd}{-1cm}
\begin{beamercolorbox}[rounded=true,wd={\inboxwd},center]{block alerted body}
\setlength{\iinboxwd}{\inboxwd}
\setlength{\inboxrule}{\inboxwd}
\addtolength{\iinboxwd}{-0.5cm}
\addtolength{\inboxrule}{0.5cm}
\begin{center}
\begin{minipage}{\iinboxwd}
\justifying
}
\setbeamertemplate{block alerted end}
{
\end{minipage}
\end{center}
\end{beamercolorbox}
\end{beamercolorbox}
\vskip\smallskipamount
}

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AEPSHEPposter/beamerthemecpbgposter.sty Normal file
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%==============================================================================
% beamer style for posters of the
% Computatinal Physics and Biophysics Group
%
% version 1.03
% - added required packages for nice fonts
% - added tikz package
% version 1.02
% - added jblue, the jacobs blue
% - use jblue as standart color for borders and boxes
% version 1.01
% - fix logo width for landscape posters
% version 1.00
% - inital release
% =============================================================================
\ProvidesPackage{beamerthemecpbgposter}
\RequirePackage{tikz}
\usetikzlibrary{arrows,decorations.pathmorphing,backgrounds,calc}
\RequirePackage[T1]{fontenc}
\RequirePackage{lmodern}
\RequirePackage{textcomp}
\RequirePackage{amsmath,amssymb}
\usefonttheme{professionalfonts}
\newlength{\inboxwd}
\newlength{\iinboxwd}
\newlength{\inboxrule}
\newlength{\logocolw}
\newcommand{\makeruleinbox}
{{\usebeamercolor[bg]{block alerted title}\centering\hspace*{-0.7cm}
\rule{\inboxrule}{0.5cm}}
}
%this is needed to get the block text justified
\usepackage{ragged2e}
%define some nice colors
\definecolor{lgreen} {RGB}{180,210,100}
\definecolor{dblue} {RGB}{20,66,129}
\definecolor{lred} {RGB}{220,0,0}
\definecolor{nred} {RGB}{224,0,0}
\definecolor{norange}{RGB}{230,120,20}
\definecolor{nyellow}{RGB}{255,221,0}
\definecolor{ngreen} {RGB}{98,158,31}
\definecolor{dgreen} {RGB}{78,138,21}
\definecolor{nblue} {RGB}{28,130,185}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% LaTeX poster template
% Created by Nathaniel Johnston
% August 2009
% http://www.nathanieljohnston.com/2009/08/latex-poster-template/
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\documentclass[final]{beamer}
\usepackage[scale=1.24]{beamerposter}
\usepackage{graphicx} % allows us to import images
%-----------------------------------------------------------
% Define the column width and poster size
% To set effective sepwid, onecolwid and twocolwid values, first choose how
% many columns you want and how much separation you want between columns The
% separation I chose is 0.024 and I want 4 columns
% Then set onecolwid to be (1-(4+1)*0.024)/4 = 0.22
% Set twocolwid to be 2*onecolwid + sepwid = 0.464
%-----------------------------------------------------------
\newlength{\sepwid}
\newlength{\onecolwid}
\newlength{\twocolwid}
\newlength{\threecolwid}
\setlength{\paperwidth}{594mm}
\setlength{\paperheight}{841mm}
\setlength{\sepwid}{0.024\paperheight}
\setlength{\onecolwid}{0.22\paperheight}
\setlength{\twocolwid}{0.464\paperheight}
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%\setlength{\twocolwid}{0.464\paperwidth}
%\setlength{\threecolwid}{0.708\paperwidth}
\setlength{\topmargin}{-0.5in}
\usetheme{confposter}
\usepackage{exscale}
%-----------------------------------------------------------
% The next part fixes a problem with figure numbering. Thanks Nishan!
% When including a figure in your poster, be sure that the commands are typed
% in the following order: \begin{figure}
% \includegraphics[...]{...}
% \caption{...}
% \end{figure}
% That is, put the \caption after the \includegraphics
%-----------------------------------------------------------
\usecaptiontemplate{
\small
\structure{\insertcaptionname~\insertcaptionnumber:}
\insertcaption}
%-----------------------------------------------------------
% Define colours (see beamerthemeconfposter.sty to change these colour definitions)
%-----------------------------------------------------------
\setbeamercolor{block title}{fg=ngreen,bg=white}
\setbeamercolor{block body}{fg=black,bg=white}
\setbeamercolor{block alerted title}{fg=white,bg=dblue!70}
\setbeamercolor{block alerted body}{fg=black,bg=dblue!10}
%-----------------------------------------------------------
% Some new commands
%-----------------------------------------------------------
\newcommand{\compresslist}{%
\setlength{\itemsep}{1pt}%
\setlength{\parskip}{0pt}%
\setlength{\parsep}{0pt}%
}
%-----------------------------------------------------------
% Name and authors of poster/paper/research
%-----------------------------------------------------------
%\title{Study of Muon Capture for $\boldsymbol{\mu-e}$ Conversion Experiments}
\title{Measurement of Charged Particles Emission From Muon Capture}
\author{Tran Hoai Nam}
\institute{Department of Physics, Graduate School of Science, Osaka Univerity}
%-----------------------------------------------------------
% Start the poster itself
%-----------------------------------------------------------
\begin{document}
\begin{frame}[t]
\begin{columns}[t] % the [t] option aligns the column's content at the top
%An empty column to help positioning the whole content at the center of the
%paper
\begin{column}
{0.3\sepwid}
\end{column}
%-----------------------------------------------------------
% Actual content
%-----------------------------------------------------------
\begin{column}{\onecolwid}
% Introduction
%\setbeamercolor{block alerted body}{fg=black,bg=white}
\begin{block}{Introduction - Searches for cFLV}
\begin{itemize}
\item Charged lepton flavor violation (cFLV), if observed, is a clear
evidence of new physics beyond the Standard Model (fig.
\ref{fig:SMmeg}).
\begin{figure}[h!]
\begin{center}
\includegraphics[width=0.8\onecolwid]{figs/SM-meg2}
\end{center}
\caption{One of the diagrams of massive neutrino contributions to
$\mu \rightarrow e\gamma$}
\label{fig:SMmeg}
\end{figure}
\item Event signal of $\mu - e$ conversion
\item COMET schedule
\end{itemize}
\end{block}
\vskip2ex
\begin{block}{Introduction$\boldsymbol{\mu^-N \rightarrow e^-N}$}
\vskip1ex
\begin{itemize}
\item Two major experiments search for $\mu-e$ conversion:
COMET@J-PARC and Mu2e@FNAL
\item Design issue from muon capture process: optimization of the
target thickness and the absorber to reduce hit rate of protons
\begin{figure}[]
\includegraphics[width=22cm]{figs/phase1det}
\caption{Concept of the tracking detector of COMET Phase I [ref]}
\label{fig:phase1det}
\end{figure}
\item Current status: no data available for relevant target and
energy range. Mu2e and COMET are using a parameterization of muon
capture data taken from the Si active target in 1968.
\begin{figure}[]
\includegraphics[width=22cm]{figs/si-proton}
\caption{Silicon data [ref]}
\label{fig:sidata}
\end{figure}
\end{itemize}
\end{block}
\vskip2ex
\begin{block}{The new measurement of charged particles emission
from muon capture}
\begin{itemize}
\item A joint collaboration between COMET and Mu2e
\item Goals of the experiment:
\begin{itemize}
\item[-] measure rate and energy spectra of the charged particles
(p, d, $\alpha$) emitted after muon capture on some targets:
Al, Si and Si (active target),
\item[-] required precision: 5\% for both the rate and the energy
spectra in the range from 2.5 $-$ 12 MeV
\end{itemize}
\item Will be conducted at TRIUMF (Canada) and PSI (Switzerland).
\end{itemize}
\vskip1ex
\end{block}
\end{column}
%\begin{column}{0.3\sepwid}
%\end{column} % empty spacer column
% create a three-column-wide column and then we will split it up later
\begin{column}{\twocolwid}
% Methods
\begin{block}{Methods}
\begin{minipage}[t]{\onecolwid}
\begin{figure}[]
\includegraphics[width=0.95\onecolwid]{figs/setup}
\caption{Schematic view of the experimental set up}
\label{fig:setup}
\end{figure}
\end{minipage} % Do not put another blank line after this line because
%that will mess up the alignment of the two minipages
\begin{minipage}[t]{\onecolwid}
The schematic view of the experimental set up is shown in the Figure
\ref{fig:setup}:
\begin{itemize}
\item Low momentum muon beam: to ensure a high rate of stopped
muons, and a well determined range of muons in the targets. A
cloud muon of 30 $-$ 34 MeV/c from a surface muon channel is
optimal.
\item The charged particles are measured by dE/dx method
by two pairs of silicon detectors. Active area of each silicon
detector is 5$\times$5 cm$^2$, the dE detectors are 65 $\mu m$
thick, and the E detectors are 1500 $\mu m$ thick.
\item Muon normalization: muonic X-ray measurement by a germanium
detector.
\item Correction for energy loss of charged particles in the
targets: using a response function obtained from the use of the
active silicon target, where the energy loss can be measured. A
waveform digitizer will be used to readout signals from the
active target.
\end{itemize}
\end{minipage}
\end{block}
\vskip2ex
% Simulation result
\begin{block}{Calculations}
\begin{itemize}
\item Using Geant4, with assumptions:
\begin{itemize}
\item [-] Muon momentum 30 MeV/c, momentum spread 5\%.
\item [-] Muon intensity: 10$^4$ muons/sec.
\item [-] Proton emission rate is 0.15 per muon capture, the same
value as being used in COMET and Mu2e calculations.
\item [-] Efficiency of silicon detectors are 100\%.
\item [-] Energy resolution (FWHM) of silicon detectors are: 140
keV for the 65 $\mu m$-thick detectors, and 40 keV for the
$140 \mu m$-thick detectors.
\end{itemize}
\item Simulation results of particle identification and rate
estimation is shown in Figure \ref{fig:dEdx} and Table
\ref{tb:rates}.
\end{itemize}
%\begin{minipage}[]{1.1\onecolwid}
\begin{figure}[]
\includegraphics[width=1.25\onecolwid]{figs/dEdx}
\caption{Particle identification with two silicon detectors}
\label{fig:dEdx}
\end{figure}
%\end{minipage}
%\begin{minipage}[c]{0.9\onecolwid}
%\begin{table}[htb!]
%\begin{center}
%\begin{tabular}{|c|c|c|c|c|c|} \hline
%Target & \% Stopping & Event rate (Hz) & Event rate (Hz) \\
%thickness ($\mu$m)& in target & All particles & Protons \\
%\hline
%50 & 2 & 8.1 & 1.0 \\ \hline
%100 & 16 & 21.3 & 1.5 \\ \hline
%150 & 38 & 39.9 & 2.1 \\ \hline
%200 & 53 & 51.1 & 2.4 \\ \hline
%\end{tabular}
%\end{center}
%\caption{Estimated event rates for various targets of different
%thickness. }
%\label{tb:rates}
%\end{table}
%\end{minipage}
\end{block}
%\begin{columns}[t,totalwidth=\twocolwid] % split up that three-column-wide column
%\begin{column}{\onecolwid}
%\setbeamercolor{block title}{fg=red,bg=white}%frame color
%\setbeamercolor{block body}{fg=black,bg=white}%body color
%\begin{block}{Block Colours}
%For the standard blocks there are two colours; one for the title and one for the block body:\\
%\begin{semiverbatim}
%{\color{red}\\setbeamercolor}\{block title\}\newline \{fg=red,bg=white\}
%\end{semiverbatim}
%\begin{semiverbatim}
%{\color{red}\\setbeamercolor}\{block body\}\newline \{fg=black,bg=white\}
%\end{semiverbatim}
%The \emph{fg} colour sets the text colour and \emph{bg} sets the background colour.
%For the normal blocks it makes no sense to use a background colour other than white. You \emph{can} change it, but it will look weird!
%\end{block}
%\end{column}
%\begin{column}{\onecolwid}
%\setbeamercolor{block alerted title}{fg=black,bg=norange} % frame color
%\setbeamercolor{block alerted body}{fg=black,bg=white} % body color
%\begin{alertblock}{Alert Block Colours}
%You can similarly modify the colours for alert blocks (but try not to overdo it):\\
%\begin{semiverbatim}
%{\color{red}\\setbeamercolor}\{block title\}\newline \{fg=black,bg=norange\}
%\end{semiverbatim}
%\begin{semiverbatim}
%{\color{red}\\setbeamercolor}\{block body\}\newline \{fg=black,bg=white\}
%\end{semiverbatim}
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%\end{column}
%\end{columns}
%\vskip2.5ex
\end{column}
%\begin{column}{0.3\sepwid}
%\end{column} % empty spacer column
\begin{column}{\onecolwid}
\begin{block}{Calculations (cont.)}
\begin{table}[htb!]
\begin{center}
\scalebox{0.95}{
\begin{tabular}{|c|c|c|c|c|c|} \hline
Target & \% Stopping & Event rate (Hz) & Event rate (Hz) \\
thickness ($\mu$m)& in target & All particles & Protons \\
\hline
50 & 2 & 8.1 & 1.0 \\ \hline
100 & 16 & 21.3 & 1.5 \\ \hline
150 & 38 & 39.9 & 2.1 \\ \hline
200 & 53 & 51.1 & 2.4 \\ \hline
\end{tabular}
}
\end{center}
\caption{Estimated event rates for various targets of different
thickness. }
\label{tb:rates}
\end{table}
\end{block}
\vskip2ex
\begin{block}{Plan}
\begin{itemize}
\item July 2012: submitted the proposal to TRIUMF as experiment
S1371, requested 36 shifts (3 weeks) beam time
\item September 2012: the proposal was accepted with high priority
\item Late November 2012: beam test
\item Early 2013: physics run, 36 shifts
\item A proposal will be submitted to PSI
\end{itemize}
\end{block}
\vskip2ex
\begin{block}{References}
Some references and a graphic to show you how it's done:
\small{\begin{thebibliography}{99}
\bibitem{KLPL06} D.~W. Kribs, R. Laflamme, D. Poulin, M. Lesosky, Quantum Inf. \& Comp. \textbf{6} (2006), 383-399.
\bibitem{zanardi97} P. Zanardi, M. Rasetti, Phys. Rev. Lett. \textbf{79}, 3306 (1997).
\end{thebibliography}}
\vspace{0.75in}
\begin{center}
\includegraphics[width=5in]{figs/canada.jpg}
\end{center}
\end{block}
\end{column}
\end{columns}
\hspace{12mm}\begin{beamercolorbox}[wd=1165mm,colsep=0.15cm]{cboxb}\end{beamercolorbox}
\end{frame}
\end{document}

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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% LaTeX poster template
% Created by Nathaniel Johnston
% August 2009
% http://www.nathanieljohnston.com/2009/08/latex-poster-template/
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\documentclass[final]{beamer}
\usepackage[scale=1.24]{beamerposter}
\usepackage{graphicx} % allows us to import images
%-----------------------------------------------------------
% Define the column width and poster size
% To set effective sepwid, onecolwid and twocolwid values, first choose how
% many columns you want and how much separation you want between columns The
% separation I chose is 0.024 and I want 4 columns
% Then set onecolwid to be (1-(4+1)*0.024)/4 = 0.22
% Set twocolwid to be 2*onecolwid + sepwid = 0.464
%-----------------------------------------------------------
\newlength{\sepwid}
\newlength{\onecolwid}
\newlength{\twocolwid}
\newlength{\threecolwid}
\setlength{\paperwidth}{1198mm}
\setlength{\paperheight}{841mm}
\setlength{\sepwid}{0.024\paperheight}
\setlength{\onecolwid}{0.22\paperheight}
\setlength{\twocolwid}{0.464\paperheight}
\setlength{\threecolwid}{0.708\paperheight}
%\setlength{\sepwid}{0.024\paperwidth}
%\setlength{\onecolwid}{0.22\paperwidth}
%\setlength{\twocolwid}{0.464\paperwidth}
%\setlength{\threecolwid}{0.708\paperwidth}
\setlength{\topmargin}{-0.5in}
\usetheme{confposter}
\usepackage{exscale}
%-----------------------------------------------------------
% The next part fixes a problem with figure numbering. Thanks Nishan!
% When including a figure in your poster, be sure that the commands are typed
% in the following order: \begin{figure}
% \includegraphics[...]{...}
% \caption{...}
% \end{figure}
% That is, put the \caption after the \includegraphics
%-----------------------------------------------------------
\usecaptiontemplate{
\small
\structure{\insertcaptionname~\insertcaptionnumber:}
\insertcaption}
%-----------------------------------------------------------
% Define colours (see beamerthemeconfposter.sty to change these colour definitions)
%-----------------------------------------------------------
\setbeamercolor{block title}{fg=ngreen,bg=white}
\setbeamercolor{block body}{fg=black,bg=white}
\setbeamercolor{block alerted title}{fg=white,bg=dblue!70}
\setbeamercolor{block alerted body}{fg=black,bg=dblue!10}
%-----------------------------------------------------------
% Some new commands
%-----------------------------------------------------------
\newcommand{\compresslist}{%
\setlength{\itemsep}{1pt}%
\setlength{\parskip}{0pt}%
\setlength{\parsep}{0pt}%
}
%-----------------------------------------------------------
% Name and authors of poster/paper/research
%-----------------------------------------------------------
%\title{Study of Muon Capture for $\boldsymbol{\mu-e}$ Conversion Experiments}
\title{Measurement of Charged Particles Emission From Muon Capture}
\author{Tran Hoai Nam}
\institute{Department of Physics, Graduate School of Science, Osaka Univerity}
%-----------------------------------------------------------
% Start the poster itself
%-----------------------------------------------------------
\begin{document}
\begin{frame}[t]
\begin{columns}[t] % the [t] option aligns the column's content at the top
%An empty column to help positioning the whole content at the center of the
%paper
\begin{column}
{0.3\sepwid}
\end{column}
%-----------------------------------------------------------
% Actual content
%-----------------------------------------------------------
\begin{column}{\onecolwid}
% Introduction
%\setbeamercolor{block alerted body}{fg=black,bg=white}
\begin{alertblock}{Introduction - Searches for cFLV}
\begin{itemize}
\item Charged lepton flavor violation (cFLV), if observed, is a clear
evidence of new physics beyond the Standard Model (fig.
\ref{fig:SMmeg}).
\begin{figure}[h!]
\begin{center}
\includegraphics[width=0.8\onecolwid]{figs/SM-meg2}
\end{center}
\caption{One of the diagrams of massive neutrino contributions to
$\mu \rightarrow e\gamma$}
\label{fig:SMmeg}
\end{figure}
\item Event signal of $\mu - e$ conversion
\item COMET schedule
\end{itemize}
\end{block}
\vskip2ex
\begin{block}{Introduction$\boldsymbol{\mu^-N \rightarrow e^-N}$}
\vskip1ex
\begin{itemize}
\item Two major experiments search for $\mu-e$ conversion:
COMET@J-PARC and Mu2e@FNAL
\item Design issue from muon capture process: optimization of the
target thickness and the absorber to reduce hit rate of protons
\begin{figure}[]
\includegraphics[width=22cm]{figs/phase1det}
\caption{Concept of the tracking detector of COMET Phase I [ref]}
\label{fig:phase1det}
\end{figure}
\item Current status: no data available for relevant target and
energy range. Mu2e and COMET are using a parameterization of muon
capture data taken from the Si active target in 1968.
\begin{figure}[]
\includegraphics[width=22cm]{figs/si-proton}
\caption{Silicon data [ref]}
\label{fig:sidata}
\end{figure}
\end{itemize}
\end{block}
\vskip2ex
\begin{block}{The new measurement of charged particles emission
from muon capture}
\begin{itemize}
\item A joint collaboration between COMET and Mu2e
\item Goals of the experiment:
\begin{itemize}
\item[-] measure rate and energy spectra of the charged particles
(p, d, $\alpha$) emitted after muon capture on some targets:
Al, Si and Si (active target),
\item[-] required precision: 5\% for both the rate and the energy
spectra in the range from 2.5 $-$ 12 MeV
\end{itemize}
\item Will be conducted at TRIUMF (Canada) and PSI (Switzerland).
\end{itemize}
\vskip1ex
\end{block}
\end{column}
%\begin{column}{0.3\sepwid}
%\end{column} % empty spacer column
% create a three-column-wide column and then we will split it up later
\begin{column}{\twocolwid}
% Methods
\begin{block}{Methods}
\begin{minipage}[t]{\onecolwid}
\begin{figure}[]
\includegraphics[width=0.95\onecolwid]{figs/setup}
\caption{Schematic view of the experimental set up}
\label{fig:setup}
\end{figure}
\end{minipage} % Do not put another blank line after this line because
%that will mess up the alignment of the two minipages
\begin{minipage}[t]{\onecolwid}
The schematic view of the experimental set up is shown in the Figure
\ref{fig:setup}:
\begin{itemize}
\item Low momentum muon beam: to ensure a high rate of stopped
muons, and a well determined range of muons in the targets. A
cloud muon of 30 $-$ 34 MeV/c from a surface muon channel is
optimal.
\item The charged particles are measured by dE/dx method
by two pairs of silicon detectors. Active area of each silicon
detector is 5$\times$5 cm$^2$, the dE detectors are 65 $\mu m$
thick, and the E detectors are 1500 $\mu m$ thick.
\item Muon normalization: muonic X-ray measurement by a germanium
detector.
\item Correction for energy loss of charged particles in the
targets: using a response function obtained from the use of the
active silicon target, where the energy loss can be measured. A
waveform digitizer will be used to readout signals from the
active target.
\end{itemize}
\end{minipage}
\end{block}
\vskip2ex
% Simulation result
\begin{block}{Calculations}
\begin{itemize}
\item Using Geant4, with assumptions:
\begin{itemize}
\item [-] Muon momentum 30 MeV/c, momentum spread 5\%.
\item [-] Muon intensity: 10$^4$ muons/sec.
\item [-] Proton emission rate is 0.15 per muon capture, the same
value as being used in COMET and Mu2e calculations.
\item [-] Efficiency of silicon detectors are 100\%.
\item [-] Energy resolution (FWHM) of silicon detectors are: 140
keV for the 65 $\mu m$-thick detectors, and 40 keV for the
$140 \mu m$-thick detectors.
\end{itemize}
\item Simulation results of particle identification and rate
estimation is shown in Figure \ref{fig:dEdx} and Table
\ref{tb:rates}.
\end{itemize}
%\begin{minipage}[]{1.1\onecolwid}
\begin{figure}[]
\includegraphics[width=1.25\onecolwid]{figs/dEdx}
\caption{Particle identification with two silicon detectors}
\label{fig:dEdx}
\end{figure}
%\end{minipage}
%\begin{minipage}[c]{0.9\onecolwid}
%\begin{table}[htb!]
%\begin{center}
%\begin{tabular}{|c|c|c|c|c|c|} \hline
%Target & \% Stopping & Event rate (Hz) & Event rate (Hz) \\
%thickness ($\mu$m)& in target & All particles & Protons \\
%\hline
%50 & 2 & 8.1 & 1.0 \\ \hline
%100 & 16 & 21.3 & 1.5 \\ \hline
%150 & 38 & 39.9 & 2.1 \\ \hline
%200 & 53 & 51.1 & 2.4 \\ \hline
%\end{tabular}
%\end{center}
%\caption{Estimated event rates for various targets of different
%thickness. }
%\label{tb:rates}
%\end{table}
%\end{minipage}
\end{block}
%\begin{columns}[t,totalwidth=\twocolwid] % split up that three-column-wide column
%\begin{column}{\onecolwid}
%\setbeamercolor{block title}{fg=red,bg=white}%frame color
%\setbeamercolor{block body}{fg=black,bg=white}%body color
%\begin{block}{Block Colours}
%For the standard blocks there are two colours; one for the title and one for the block body:\\
%\begin{semiverbatim}
%{\color{red}\\setbeamercolor}\{block title\}\newline \{fg=red,bg=white\}
%\end{semiverbatim}
%\begin{semiverbatim}
%{\color{red}\\setbeamercolor}\{block body\}\newline \{fg=black,bg=white\}
%\end{semiverbatim}
%The \emph{fg} colour sets the text colour and \emph{bg} sets the background colour.
%For the normal blocks it makes no sense to use a background colour other than white. You \emph{can} change it, but it will look weird!
%\end{block}
%\end{column}
%\begin{column}{\onecolwid}
%\setbeamercolor{block alerted title}{fg=black,bg=norange} % frame color
%\setbeamercolor{block alerted body}{fg=black,bg=white} % body color
%\begin{alertblock}{Alert Block Colours}
%You can similarly modify the colours for alert blocks (but try not to overdo it):\\
%\begin{semiverbatim}
%{\color{red}\\setbeamercolor}\{block title\}\newline \{fg=black,bg=norange\}
%\end{semiverbatim}
%\begin{semiverbatim}
%{\color{red}\\setbeamercolor}\{block body\}\newline \{fg=black,bg=white\}
%\end{semiverbatim}
%\end{alertblock}
%\end{column}
%\end{columns}
%\vskip2.5ex
\end{column}
%\begin{column}{0.3\sepwid}
%\end{column} % empty spacer column
\begin{column}{\onecolwid}
\begin{block}{Calculations (cont.)}
\begin{table}[htb!]
\begin{center}
\scalebox{0.95}{
\begin{tabular}{|c|c|c|c|c|c|} \hline
Target & \% Stopping & Event rate (Hz) & Event rate (Hz) \\
thickness ($\mu$m)& in target & All particles & Protons \\
\hline
50 & 2 & 8.1 & 1.0 \\ \hline
100 & 16 & 21.3 & 1.5 \\ \hline
150 & 38 & 39.9 & 2.1 \\ \hline
200 & 53 & 51.1 & 2.4 \\ \hline
\end{tabular}
}
\end{center}
\caption{Estimated event rates for various targets of different
thickness. }
\label{tb:rates}
\end{table}
\end{block}
\vskip2ex
\begin{block}{Plan}
\begin{itemize}
\item July 2012: submitted the proposal to TRIUMF as experiment
S1371, requested 36 shifts (3 weeks) beam time
\item September 2012: the proposal was accepted with high priority
\item Late November 2012: beam test
\item Early 2013: physics run, 36 shifts
\item A proposal will be submitted to PSI
\end{itemize}
\end{block}
\vskip2ex
\begin{block}{References}
Some references and a graphic to show you how it's done:
\small{\begin{thebibliography}{99}
\bibitem{KLPL06} D.~W. Kribs, R. Laflamme, D. Poulin, M. Lesosky, Quantum Inf. \& Comp. \textbf{6} (2006), 383-399.
\bibitem{zanardi97} P. Zanardi, M. Rasetti, Phys. Rev. Lett. \textbf{79}, 3306 (1997).
\end{thebibliography}}
\vspace{0.75in}
\begin{center}
\includegraphics[width=5in]{figs/canada.jpg}
\end{center}
\end{block}
\end{column}
\end{columns}
\hspace{12mm}\begin{beamercolorbox}[wd=1165mm,colsep=0.15cm]{cboxb}\end{beamercolorbox}
\end{frame}
\end{document}

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AEPSHEPposter/poster2.tex Normal file
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%==============================================================================
%== template for LATEX poster =================================================
%==============================================================================
%
%--A0 beamer slide-------------------------------------------------------------
\documentclass[final]{beamer} % use beamer
\usepackage[orientation=portrait,
size=a0, % poster size
scale=1.35 % font scale factor
]{beamerposter} % beamer in poster size
%
%--some needed packages--------------------------------------------------------
\usepackage[american]{babel} % language
\usepackage[utf8]{inputenc} % std linux encoding
\usepackage{booktabs}
\usepackage{multirow}
%
%==The poster style============================================================
\usetheme{cpbgposter} % our poster style
%--set colors for blocks (without frame)---------------------------------------
\setbeamercolor{block title}{fg=ngreen,bg=white}
\setbeamercolor{block body}{fg=black,bg=white}
%--set colors for alerted blocks (with frame)----------------------------------
%--textcolor = fg, backgroundcolor = bg, dblue is the jacobs blue
\setbeamercolor{block alerted title}{fg=white,bg=dblue!70}%frame color
\setbeamercolor{block alerted body}{fg=black,bg=dblue!10}%body color
%
\usecaptiontemplate{
\small
\structure{\insertcaptionname~\insertcaptionnumber:}
\insertcaption}
%==Titel, date and authors of the poster=======================================
%\title{Template for \LaTeX poster using the\\
%Computational Physics and Biophysics Group style}
%\title{Study of Muon Capture \\
%for $\boldsymbol{\mu^--e^-}$ Conversion Experiments}
\title{A Search for $\boldsymbol{\mu-e}$ Conversion \\
\vskip0.5ex
and a Study of Muon Capture Backgrounds}
\author{Tran Hoai Nam}
\institute{Department of Physics, Graduate School of Science, Osaka Univerity}
\date{\today}
%
%==some usefull qm commands====================================================
% |x>
\newcommand{\ket}[1]{\left\vert#1\right\rangle}
% <x|
\newcommand{\bra}[1]{\left\langle#1\right\vert}
% <x|y>
\newcommand{\braket}[2]{\left< #1 \vphantom{#2}\,
\right\vert\left.\!\vphantom{#1} #2 \right>}
% <x|a|y>
\newcommand{\sandwich}[3]{\left< #1 \vphantom{#2 #3} \right|
#2 \left|\vphantom{#1 #2} #3 \right>}
% d/dt
\newcommand{\ddt}{\frac{d}{dt}}
% D/Dx
\newcommand{\pdd}[1]{\frac{\partial}{\partial#1}}
% |x|
\newcommand{\abs}[1]{\left\vert#1\right\vert}
% k_{x}
\newcommand{\kv}[1]{\mathbf{k}_{#1}}
\newlength{\sepwid}
\newlength{\onecolwid}
\newlength{\twocolwid}
\setlength{\sepwid}{0.04\paperwidth}
\setlength{\onecolwid}{0.28\paperwidth}
\setlength{\twocolwid}{0.60\paperwidth}
%==============================================================================
%==the poster content==========================================================
%==============================================================================
\begin{document}
%--the poster is one beamer frame, so we have to start with:
\begin{frame}[t]
%--to seperate the poster in columns we can use the columns environment
\begin{columns}[t] % the [t] options aligns the columns content at the top
\begin{column}{0.28\paperwidth}% the right size for a 3-column layout
%--abstract block--------------------------------------------------------
\begin{block}{Introduction - Searches for cLFV}
\begin{itemize}
\item Charged lepton flavor violation (cLFV) is forbidden in the
Standard Model. However, it is predicted to occur in various
extensions of the model. Experimental observation
of cLFV process is a clear evidence of new physics beyond the
SM.
%\ref{fig:SMmeg}).
%\begin{figure}[h!]
%\begin{center}
%\includegraphics[width=0.8\onecolwid]{figs/SM-meg2}
%\end{center}
%\caption{One of the diagrams of massive neutrino contributions to
%$\mu \rightarrow e\gamma$}
%\label{fig:SMmeg}
%\end{figure}
\item Two major experiments are going to start to search for the
cLFV \textcolor{red}{$\mu-e$ conversion}: COMET and Mu2e.
%\vskip1ex
\begin{figure}[h!]
\begin{center}
\includegraphics[width=0.95\onecolwid]{figs/mueconv}
\end{center}
\caption{What and Why $\mu-e$ conversion}
\label{fig:mueconv}
\end{figure}
\item The COMET stands for COherent Muon to Electron Transition.
It has been approved by J-PARC in 2009 as experiment J-PARC E21.
The experiment will search for $\mu-e$ conversion on aluminum
target with a single-event sensitivity 10,000 times better
than the current limit. The COMET uses staging approach with two
phases \cite{loi}:
\begin{itemize}
\item [-] COMET Phase I (physics run in 2017): background study
for Phase II, and search for $\mu-e$ conversion with a
sensitivity of $\color{red}3.1\times10^{-15}$
\item [-] COMET Phase II (physics run in 2019): search for
$\mu-e$ conversion at a sensitivity of
$\color{red}3\times10^{-17}$
\begin{figure}[h!]
\begin{center}
\includegraphics[width=0.95\onecolwid]{figs/cometscheme}
\end{center}
\caption{Schematic lay out of the COMET Phase I and COMET
Phase II}
\label{fig:cometscheme}
\end{figure}
\end{itemize}
%\item Event signal of $\mu - e$ conversion: a single mono-energetic
%electron at 105 MeV
\item One issue of the experiment at Phase I: \textcolor{red}
{hit rate on the tracking detectors}. In order to optimize the
targets and the absorber, a study of charged particles,
especially protons, emitted after muon capture is needed.
\begin{figure}[h!]
\centering
\includegraphics[width=0.88\onecolwid]{figs/issue2}
\caption{Concept of the tracking detectors}
\label{fig:issue}
\end{figure}
\item There are \textcolor{red}{no experimental data}, in the
\textcolor{red}{relevant energy range}, on the
products of muon capture from \textcolor{red}{Al, and Ti target}.
Both COMET and Mu2e are using extrapolated data from a
measurement on an active Si target in 1968.
\begin{figure}[h!]
\includegraphics[width=0.85\onecolwid]{figs/si-proton}
\caption{Charged particles spectrum after muon capture on
Si$^{28}$ \cite{sidata}}
\label{fig:sidata}
\end{figure}
\end{itemize}
\end{block}
%% The proton measurement experiment
\end{column}
%===rightcolumn=================================================================
% here the the middle and right column are put into one big column, this allows
% to change between 2 and 3 column style
\begin{column}{0.60\paperwidth} %thats the big right column
\begin{block}{The new measurement of charged particles emission
from muon capture}
\begin{itemize}
\item A joint collaboration between COMET and Mu2e
\item Goals of the experiment:
\begin{itemize}
\item[$\bullet$] measure \textcolor{red}{rate and energy
spectra} of the charged
particles (p, d, $\alpha$) emitted after muon capture on
some targets:
\begin{itemize}
\item [-] Al: default target of COMET and Mu2e
\item [-] Ti: possible target for future $\mu-e$
conversion experiments
\item [-] Si: active target, for cross-checking against
previous experiment, and studying the energy loss of
charged particles inside the targets
\end{itemize}
\item[$\bullet$] required precision: \textcolor{red}{5\%}
for both the rate and the
energy spectra in the range from 2.5 $-$ 12 MeV
\end{itemize}
\item Will be conducted at TRIUMF (Canada) and PSI
(Switzerland).
\end{itemize}
\end{block}
\vskip1ex
% Methods
\begin{block}{Methods}
\begin{figure}[]
\includegraphics[width=0.95\twocolwid]{figs/setupa}
\caption{Experimental setup: schematic view (left) and image (right)}
\label{fig:setup}
\end{figure}
\begin{minipage}[t]{\onecolwid}
\begin{itemize}
\item Low momentum muon beam: to ensure a high rate of stopped
muons, and a well determined range of muons in the targets. A
cloud muon of 30 $-$ 34 MeV/c from a surface muon channel is
optimal.
\item The charged particles are measured by dE/dx method
by two pairs of silicon detectors. Active area of each silicon
detector is 5$\times$5 cm$^2$, the dE detectors are 65 $\mu m$
thick, and the E detectors are 1500 $\mu m$ thick.
\end{itemize}
\end{minipage} % Do not put another blank line after this line because
%that will mess up the alignment of the two minipages
\begin{minipage}[t]{\onecolwid}
\begin{itemize}
\item Muon normalization: muonic X-ray measurement by a germanium
detector.
\item Correction for energy loss of charged particles in the
targets: using a response function obtained from the use of the
active silicon target, where the energy loss can be measured. A
waveform digitizer will be used to readout signals from the
active target.
\end{itemize}
\end{minipage}
\end{block}
\vskip2ex
%===two right columns===========================================================
% we have to give the total width for the column wich is equal to the sum of
% two colums and the space between them, this is needed to make shure the two
% cols take all the space of the 'mother' column
\begin{columns}[t,totalwidth=0.60\paperwidth]
% and then we put in two normal sized columns
\begin{column}{0.28\paperwidth}
%--the Left block-----------------------------------------------------------
\begin{block}{Calculations}
\begin{itemize}
\item Using Geant4, with assumptions:
\begin{itemize}
\item [$\bullet$] Muon momentum 30 MeV/c, momentum spread 5\%.
\item [$\bullet$] Muon intensity: 10$^4$ muons/sec.
\item [$\bullet$] Proton emission rate is 0.15 per muon capture,
the same value as that is being used in COMET designing
calculations
\item [$\bullet$] Energy resolution (FWHM) of silicon detectors
are: 140 keV for the 65 $\mu m$-thick detectors, and 40 keV for
the 140 $\mu m$-thick detectors.
\item [$\bullet$] Thickness of the beam counter scintillator: 0.5 mm
\end{itemize}
\item Simulation results of particle identification and rate
estimation is shown in Figure \ref{fig:dEdx} and Table
\ref{tb:rates}.
\end{itemize}
\vskip2ex
\begin{figure}[]
\includegraphics[width=0.95\onecolwid]{figs/dEdx}
\caption{Particle identification with two silicon detectors}
\label{fig:dEdx}
\end{figure}
\end{block}
\end{column}
%--the Right block--------------------------------------------------------------
\begin{column}{\onecolwid}
\begin{block}{Calculations (cont.)}
\begin{table}[h!]
\begin{center}
\scalebox{0.75}{
\begin{tabular}{cccc}
\toprule
Target & \% Stopping & Event rate (Hz) & Event rate (Hz) \\
thickness ($\mu$m)& in target & All particles & Protons \\
\midrule
50 & 2 & 8.1 & 1.0 \\
100 & 16 & 21.3 & 1.5 \\
150 & 38 & 39.9 & 2.1 \\
200 & 53 & 51.1 & 2.4 \\
\bottomrule
\end{tabular}
}
\end{center}
\caption{Estimated event rates for various targets of different
thickness. }
\label{tb:rates}
\end{table}
\end{block}
\vskip2ex
\begin{block}{Plan}
\begin{itemize}
\item July 2012: submitted the proposal to TRIUMF as experiment
S1371, requested 36 shifts (3 weeks) beam time
\item September 2012: the proposal was accepted with high priority
\item Late November 2012: beam test
\item Early 2013: physics run, 36 shifts
\item A proposal will be submitted to PSI
\end{itemize}
\end{block}
\vskip2ex
\begin{block}{References}
\small{\begin{thebibliography}{99}
%\bibitem{cdr} The COMET Collaboration, ``Conceptual Design Report for
%Experimental Search for Lepton Flavor Violating $\mu^--e^-$
%Conversion at
%Sensitivity of $10^{-16}$ with a Slow-Extracted Bunched Proton Beam
%(COMET)'', KEK-2009-10
\bibitem{loi} The COMET Collaboration, ``Letter of Intent for Phase-I
of the COMET Experiment at J-PARC'', J-PARC-2012-3
\bibitem{sidata} S. E. Sobottka and E. L. Wills, ``Energy Spectrum
of Charged Particles Emitted Following Muon Capture in Si$^{28}$'',
Phys. Rev. Lett. \textbf{20} (1968) 596-598.
\end{thebibliography}}
\end{block}
\end{column}
\end{columns}
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% (TeXlive 2008, Miktex) and download the beamerthemecpbgposter.sty file from
% our teamwork page and put it in your local TeX directory.
%
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% awesome dude who created this insanely great poster style then don't
% hastitate to write an email to \emph{j.liebers@jacobs-university.de}
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\subsubsection*{ Experimental area}
$\pi$E1 beam line
\subsubsection*{Required beam properties}
\begin{itemize}
\item Particle: $\mu^-$
\item Momentum: 30--35 MeV/c
\item Momentum bin: $<2$ \% FWHM
\item Beam spot: $<2$ cm in diameter
\item Intensity: $2 \times 10^{4}$ s$^{-1}$
\item Beam purity: $<10$ \% electrons
\end{itemize}
\subsubsection*{ Duration of the experiment}
{\bf We request two 4 week PSI beam blocks, one scheduled in 2013 and the
next one in 2014.}
The first experiment would be used to commission the full set-up and shake down its
components for the three work-packages (WPs) planned. The priority would be to perform most of the proton
measurements (WP1), while simultaneously measuring the X-rays for
WP2. A first exploratory neutron measurement
to start WP3 is also anticipated. This part of the experiment is ready
in spring 2013, and we would prefer an
early running time during the 2013 schedule. After that,
the data would be analyzed and results reported at the BVR 2014. Depending on the outcome,
in 2014 additional proton statistics data taking and systematic studies are foreseen to achieve publication quality
data. But the main focus in 2014 will be on final neutron
measurements and operating the large NaI for the WP2 program.
The requested 2013 beam time will be structured in the following way:
\begin{itemize}
\item Week 1: Set-up. Commission beam counters, proton, X-ray and
neutron detectors. Vacuum in target chamber.
\item Week 2: Beam-optimization. Thick, then thin Si detectors
as active targets are used to study beam properties and optimize the
stopping fraction, to quantify background and select the
optimal geometry of the detector packages, relative to
target and beam. The X-ray detector will assist in the tuning process. First high statistics data set is taken
with thin Si in the target position, to calibrate the target
response function and normalize the X-ray detectors.
\item Week 3: High statistics measurements with 3 targets of
Al and Ti, 25-200 $\mu$m thickness.
\item Week 4: Continued Al, Ti measurements. Last days
dedicated neutron measurement, thick target, with proton vacuum chamber removed.
\end{itemize}

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\vspace{.0cm}
{\raggedleft December 10, 2012 \\
\par}
\vspace{.5cm}
\begin{center}
{\bf\LARGE Study of Muon Capture for\\\vspace{2mm}
Muon to Electron Conversion Experiments}
\vspace{.5cm}
\Large
AlCap Collaboration
\vspace{1.5cm}
%% ML - move this figure to the Intrduction
% \begin{figure}[h]
% %\vspace{-40mm}
% \includegraphics[width=\textwidth]{figs/comet-mu2e.png}
% \caption{Schematic layouts of the Mu2e (left) and the COMET (right).}
% \label{fg:mu2ecomet}
% %\vspace{-5mm}
% \end{figure}
% \vspace{10mm}
\end{center}
\begin{center}
%{\tt Preliminary version, final proposal will be uploaded on 12/14/2012}
%{\bf institutional representatives, please check and update}
\vspace{5mm}
D. Alexander\uh,
D.M. Asner\pnnl,
E. Barnes\bu,
R. Bernstein\fnal,
R. Bonicalzi\pnnl,
A. Daniel\uh,
A. Edmonds\ucl,
A. Empl\uh,
D. Hertzog\uw,
Y. Hino\osaka,
E. Hungerford\uh,
T. Itahashi\osaka,
D. Kawall\umass,
A. Kolakar\bu,
B. Krikler\icl,
\underline{P. Kammel\uw},
K. Kumar\umass,
\underline{Y. Kuno\osaka},
A. Kurup\icl,
M. Lancaster\ucl,
J. Miller\bu,
M. Murray\uw,
T.H. Nam\osaka,
V. Ruso\fnal,
H. Sakamoto\osaka,
A. Sato\osaka,
M. Schram\pnnl,
Y. Uchida\icl,
G. Warren\pnnl,
F. Wauters\uw,
P. Winter\anl,
M. Wing\ucl,
L. Wood\pnnl
\vspace{10mm}
\anl Argonne National Laboratory, Illinois (ANL)
\bu Boston University, Boston, Massachusetts (BU)
\fnal Fermilab National Accelerator Laboratory, Batavia, Illinois (FNAL)
\uh University of Houston, Houston, Texas (UH)
\icl Imperial College, London, UK (ICL)
\umass University of Massachusetts, Amhurst, Massachusetts (UMass)
\osaka Osaka University, Osaka, Japan (OU)
\pnnl Pacific Northwest National Laboratory, Richland, Washington (PNNL)
\ucl University College London, London, UK (UCL)
\uw University of Washington, Seattle, Washington (UW)
\vspace{15mm}
Co-spokespersons underlined.
\end{center}
\newpage
\vspace{2cm}
\begin{center}
{\bf Abstract}
\end{center}
The recent observation that neutrinos oscillate, change flavour, and so have
mass, requires an extension to the Standard Model (SM) and
demonstrates that lepton flavour is
not an absolutely conserved quantity. However, even when accommodating
finite neutrino mass in a minimal extension
to the SM, the rate of charged lepton flavour
violating (CLFV) interactions is predicted to be far too
small to be observed, ${\cal{O}}(10^{-50})$. Thus, any experimental
observation of CLFV would be clear evidence of new physics beyond the SM.
Two new projects will search for the CLFV in
\muec conversion. They are the Mu2e experiment at FNAL and the
COMET experiment at J-PARC. Both experiments utilise multi-kW
pulsed 8$-$9 GeV proton beams to achieve a branching ratio sensitivity lower
than 10$^{-16}$, that is 10,000 times better than the current best
limit established by SINDRUM II.
Both COMET Phase-I and Mu2e are subject to significant backgrounds
from the products from muon (and pion) nuclear capture. The
goals of this joint proposal between both Mu2e and COMET
collaborations are precision measurements of muon
capture reactions in candidate targets, at levels required
for the design and optimization of this new generation of experiments.
The initial focus of this proposal is on the measurement of low energy
charged particles after muon capture on a nucleus. This process
constitutes a severe background, and has inadequate
experimental information available. X-rays and
gamma-rays will be also observed, in order to verify that this
technique can be used to determine the number of $\mu$ captures in a
$\mu \to e$ experiment, and to
normalize the proposed capture measurements. Finally we propose to
study both neutron emission after $\mu$ capture and radiative decay of
the $\mu$ in the nuclear environment as these also provide crucial
information to be used in the design and simulation of the experiments.\\
PSI beam quality is critical to provide a pure, low-energy muon beam
with a small momentum spread. This is especially important for
charged-particle emission measurements, as thin targets of
aluminum, silicon and titanium are required so that the emitted
particles penetrate the targets with minimal energy loss.
This was a major problem in previous experiments and has prevented the
extraction of low-energy spectra.
\newpage

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As outlined in the introduction, the Mu2e and COMET collaborations
propose to study background reactions to the
\muec process for the candidate target materials (Al, Ti). These studies
are needed to optimise the designs of the two experiments, as existing
information on these background processes is limited and what is
known, is insufficiently precise.
The new piE1 beamline at PSI offers a unique opportunity for these
experiments, as emphasized in section~\ref{PSI}. Our experimental
program is organised in three distinct work packages (WP), directed
by different team leaders, given in parentheses.
\begin{itemize}
\item[WP1:] (Kammel (Seattle), Kuno(Osaka)) \textbf{Charged Particle
Emission after Muon Capture.}\\
Protons emitted after nuclear muon capture in the stopping target
dominate the single-hit rates in the tracking chambers for both the
Mu2e and COMET Phase-I experiments. We plan to measure both the total
rate and the energy spectrum to a precision of 5\% down to proton
energies of 2.5 MeV.
\item[WP2:] (Lynn(PNNL), Miller(BU)) \textbf{Gamma and X-ray Emission
after Muon Capture.}\\
A Ge detector will be used to measure X-rays from the muonic atomic
cascade, in order to provide the muon-capture normalization for WP1, and is
essential for very thin stopping targets. It is also the primary
method proposed for calibrating the number of muon stops in the
Mu2e and COMET experiments. Two
additional calibration techniques will also be explored; (1)
detection of delayed gamma rays from nuclei activated during nuclear
muon capture, and (2) measurement of the rate of photons
produced in radiative muon decay. The first of these would use a Ge
detector and the second a NaI detector.
The NaI
calorimeter will measure the rate of high energy photons from
radiative muon capture (RMC), electrons from muon decays in orbit
(DIO), and photons from radiative muon decay (RMD), as potential
background sources for the conversion measurement. As these rates are
expected to be extremely low near the conversion electron energy, only
data at energies well below 100 MeV will be obtained.
\item[WP3:] (Hungerford(UH), Winter(ANL)) \textbf{Neutron Emission
after Muon Capture.}\\
Neutron rates and spectra after capture in Al and Ti are not well
known. In particular, the low energy region below 10 MeV is
important for determining backgrounds in the Mu2e/COMET detectors and
veto counters as
well as evaluating the radiation damage to electronic
components. Carefully calibrated liquid scintillation detectors, employing
neutron-gamma discrimination and spectrum unfolding techniques, will
measure these spectra. The measurement will attempt to obtain spectra
as low or lower than 1 MeV up to 10 MeV. \\
\end{itemize}
WP1 is the most developed project in this program. Most of the
associated apparatus has been built and optimized. We are ready to
start this experiment in 2013, while preparing and completing test
measurements and simulations to undertake WP2 and WP3.
\subsubsection{WP1: Charged Particle Emission after Muon Capture}
\subsubsection*{Present knowledge}
The yield, energy spectrum and composition of the charged particles
emitted in muon capture on Al and Ti have not been measured directly
in the relevant energy range for COMET Phase-I and Mu2e. Only high
energy spectra are available for Al (Fig.~\ref{fg:AlHE}), while low
energy spectra are only measured for Si (
Figure~\ref{fg:silicon-proton}), where muons can be stopped and
captured in an active silicon detector \cite{sobo68}. The peak below
1.4~MeV is presumed to be due to recoiling heavy ions, mainly $^{27}$Al, when no
charged particles were emitted. Hungerford~\cite{hung34} fitted the
silicon spectrum in Fig.~\ref{fg:silicon-proton} with an empirical
function given by;
%
\begin{equation}
p(T) = A(1-{T_{th} \over T})^{\alpha} e^{-(T/T_0)}
\label{eq:protons}
\end{equation}
%
where $T$ is the kinetic energy and the fitted parameters are
$A=0.105$ MeV$^{-1}$, $T_{th}$ = 1.4 MeV, $\alpha$=1.328 and $T_0$ =
3.1 MeV. The spectrum is normalized to 0.1 per muon capture. Some
other results in the past experiments are summarized in
Table~\ref{tb:proton}.
\begin{table}[b!]
\centering
\caption{Probabilities in units of $10^{-3}$ per muon capture for
inclusive proton emission from~\cite{Lifshitz}. The numbers in
crescent parenthesis are estimates for the total inclusive rate
derived from the measured exclusive channels by the use of the
approximate regularity, such as $(\mu, \nu p):(\mu, \nu p n):(\mu, \nu
p 2n):(\mu. \nu p 3n) = 1:6:4:4$.}\label{tb:proton}
\vskip 3mm
\begin{tabular}{|c|c|c|c|c|}\hline
Target nucleus & Calculation & Experiment & Estimate & Comments \\ \hline
$_{10}$Ne & & $200\pm 40$ & & \\
$^{27}_{13}$Al & 40 & $>28 \pm 4$ & (70) & 7.5 for $T>40$ MeV \\
$^{28}_{14}$Si & 144 & $150\pm30$ & & 3.1 and 0.34 $d$ for $T>18$ MeV \\
$^{31}_{15}$P & 35 & $>61\pm6$ & (91) & \\
$^{46}_{22}$Ti & & & & \\
$^{51}_{23}$V & 25 & $>20\pm1.8$ & (32) & \\ \hline
\end{tabular}
\end{table}
\begin{figure}[htb!]
\begin{minipage}{0.35\textwidth}
\centering
\includegraphics[width=0.9\textwidth]{figs/AlHE.png}
\caption{Energetic charged particle spectrum from muon capture in Al
and other targets~\cite{Krane:1979}.}
\label{fg:AlHE}
\end{minipage}
\hspace{3mm}
\begin{minipage}{0.6\textwidth}
\centering
\includegraphics[width=0.9\textwidth]{figs/si-proton.eps}
\caption{Charged particle spectrum from muons stopping and being
captured in a silicon detector~\cite{sobo68}.}
\label{fg:silicon-proton}
\end{minipage}
\end{figure}
\subsubsection*{Relevance for $\mu-e$ Conversion Experiments}
The tracking detectors of COMET Phase-I and Mu2e are designed to
measure the helical trajectories of ~105 MeV conversion electrons in a
uniform, cylindrical magnetic field. The detector geometry coupled
with the field strength accepts charge particle momenta between ~54 to
~200 MeV/c. In this momentum range ``hits'' in a tracker plane are
dominated by proton emission after nuclear muon capture. Such events
are particularly troublesome due to their large energy deposition. In
addition to protons, electrons emitted during muon decays in
orbit (DIO) are also a source of background. Background events in the
tracking detector can produce ambiguous track reconstructions, which
may lead to mis-identified events in the signal region. Both
experiments plan to introduce thin, low-Z proton
absorbers in front of the tracking chambers to reduce proton hit
rates. These are effective at removing protons due to their very low energies
(~5 MeV for 100 MeV/c protons). However, such absorbers degrade the
momentum resolution of conversion electron
candidates and their thickness and geometry must be carefully
designed. For similar reasons, the design of the stopping target is
also important.
The limited information available at present makes it difficult to
arrive at a conclusive detector design. From Table~\ref{tb:proton},
the relative experimental yield for proton emission from Al for
energies above 40 MeV is 3\%. From theory the expectation is 4\%,
if estimated from the ratio of
exclusive channels from other nuclei it is 7\%, or it may be as
high as that from Si or Ne, 15-20\%. The energy spectrum can only be
inferred from the Si data or from Ref.~\cite{Bala67}. At this moment,
~\cite{Bala67} has been
used to estimate proton emission for both experiments. The emission of
deuterium and alpha particles is also not known. Charged particle
yields from Ti can only be estimated
from V to be around 3\%. Thus a measurement of the rate and spectrum
of proton emission after
muon capture is required in order to estimate background and optimize
the detector design.
% Typical background rates in a tracker are shown in Table
%~\ref{bk_hits} as a function of the time interval relative to the peak
%of the proton pulse.\\
In COMET Phase-I,
singles rates in the tracking chamber (cylindrical drift chamber) have
been estimated based on the spectrum given in
Eq.(\ref{eq:protons}). To reduce the proton flux entering the
tracking chamber, in addition to the inner wall of the drift chamber
(of 400 $\mu$m) a cylindrical proton absorber is located in front of
the tracking chamber. Monte Carlo simulations were run for three
different thicknesses of proton degrader, 0~mm, 5~mm, and
7.5~mm and are
are summarized in Table~\ref{tb:protonhits}, where the
proton emission rate of 0.15 per muon capture is assumed. For a
typical number of stopped muons and for a 5 mm degrader, the total
number of hits in the
first plane is estimated to be 530 kHz (1.3 MHz). According to simulations,
rates are similar
for Mu2e. In simulation studies of reconstructed conversion electron
tracks mixed with a nominal proton background, a decease of
approximately 17\% in energy resolution in the conversion electron
peak and a down shift of 0.7 MeV was found when a standard proton
absorber was inserted. A downshifted conversion peak is an issue as it
pushes the signal up the DIO background curve. \\
%
\begin{table}[ht!]
\begin{center}
\caption{Total numbers of hits in the first layer by protons
emitted from muon capture for different trigger counter
thickness. 100 k proton events were generated for COMET
Phase-I. 15 \% protons per muon capture is assumed.}
\label{tb:protonhits}
\vspace{5mm}
\begin{tabular}{|l|c|c|c|} \hline
proton degrader thickness & 0 mm & 5 mm& 7.5
mm\cr\hline\hline
hits & 2644 & 103 & 30 \cr\hline
hits per proton emission & 2.6 \% & 0.1 \% & 0.03 \% \cr\hline
hits per muon capture$^{*}$ & $3.9\times10^{-3}$ &
$1.5\times10^{-4}$ & $4.5\times10^{-5}$ \cr\hline
\end{tabular}
\end{center}
\end{table}
\subsubsection{WP2: Gamma and X-ray Emission after Muon Capture.}
\subsubsection*{Present knowledge}
When a negative muon is captured in an atomic orbit, it
cascades down to the 1s level within $10^{-13}$s. Initially the
cascade occurs with Auger emission, but near the $n =5$ atomic level,
muonic X-rays start to dominate the process.
Theoretical determination of the energy levels is complex, due to
effects such as screening of the nucleus by inner electrons, shift of
low-level states due to the finite charge distribution of the nucleus,
relativistic corrections, and fine structure splitting of levels.
Nevertheless, muonic X-rays have been used to identify the capturing
element, typically from the $2p \rightarrow 1s$ transition X-ray,
which occurs $\sim$80\% of the time. An X-ray spectrum for phosphorus
is shown in figure \ref{phos_spectrum}.
The spectra of prompt gammas from muon capture have been measured for
Al~\cite{MeasdayAl} but not for Ti, using time coincidences with the
incoming muon. To our knowledge there are no data for singles mode or
for delayed gammas from decays of unstable nuclei produced in the muon
capture process.
The RMD photon spectra have been measured in previous experiments
(including MEG) and is theoretically well reproduced for a free
muon. We propose to evaluate the feasibility of measuring the spectrum
using a NaI detector for energies between 20 and 54 MeV. In this
region the spectrum
is only slightly distorted by the fact that the muon is bound in
an atomic orbit.
We also propose to confirm with existing data, the high energy tail of
the electron and
photons from RMD, DIO, and RMC. We note that the high energy tails for
RMD and DIO are the result of
atomic binding, which is absent in free muon decay. There is a recent
theoretical calculation~\cite{czarnecki} of the DIO
electrons which should be tested. Due to rates at PSI, we would only be able to
observe spectra at energies below 80 MeV. The spectra near the
end-point energy can only be observed with the extremely
large number of stopped muons envisioned in the Mu2e and COMET
experiments.
\begin{figure}[htb]
\begin{center}
\includegraphics[scale=0.50]{figs/phos_spectrum.png}
\caption{A typical muonic X-ray spectrum \cite{shera80}.}
\label{phos_spectrum}
\end{center}
\end{figure}
\begin{figure}[htb]
\begin{center}
\includegraphics[scale=0.50]{figs/rmd-spect.png}
\caption{A typical radiative muon decay spectrum.}
\label{rmd-spect}
\end{center}
\end{figure}
\subsubsection*{Relevance for $\mu-e$ Conversion Experiments}
The rate of muon capture in the stopping target is critical
for proper normalization of data in the \muec experiments, and the
proposed method of observing this rate will count muonic
X-rays as the $\mu \to e$ data are collected.
A germanium detector will be placed far from the stopping
target to reduce both rate and damage to the detector. A dipole magnetic
field will be used to remove charged particles moving along the field
of view from the detector to the target.
However, the environment will be challenging, as high photon
rates and a significant neutron background will be present. Pacific
Northwest
National Laboratory is currently developing high-rate germanium
detectors utilizing such methods as custom fast preamplifiers and
segmented detectors. Measurements using these designs in muon
beam tests at PSI will be invaluable proofs of principle for the Mu2e
experiment. Also, identifying
how the gamma and neutron backgrounds affect the gamma and X-ray lines
as a function of dose is of critical importance.
In the past, experiments that have studied muonic X-ray spectra used time
coincidence between the observed X-ray and the
incident beam muon. In the
Mu2e experiment, the muon beam will be pulsed, with an average muon
stopping rate in excess of $10^{10}$ Hz. This is too large for a beam
gate to tag muon arrival. Thus, it is necessary
to operate the Ge detector in singles mode, and the PSI measurements
are essential to determine whether the X-rays can be detected above
background in this situation.
In case background in singles mode are too severe, two
alternate means to monitor the Mu2e stopping rate will be
evaluated. In one of the alternatives,
simultaneously with the collection of muonic
X-ray spectra, we will search for delayed gammas arising from the decay of
nuclei activated by nuclear muon capture.
For example, in the case of muon capture on $^{27}$Al, the reaction
$^{27}$Al($\mu^-,\nu)^{27}$Mg occurs in 16\% of the captures. The
lifetime of the $^{27}$Mg is 9.458~minutes. It decays to excited
states in $^{27}$Al, leading to a 1014.45~keV gamma 21\% of the time,
and an 843.76~MeV gamma 100\% of the time. In normal operation, Mu2e
will have a steady stream of 8~GeV proton pulses on the production
target (spaced at 1.5~microsecond intervals) for about 0.4~s, followed
by about 0.9~s period of beam-off. It may be possible to observe the
$^{27}$Mg decays
with a Ge detector in the reduced background environment when the beam
is off. At PSI, we would test whether these gammas can be cleanly
separated from background.
Another normalization alternative would be the measurement
of energetic photons from the radiative decays of the muons bound in
atomic orbits in the stopping target (RMD). Similar to free muon decay,
the branching ratio for photons above 10~MeV relative to regular decay
is about 1.4\% and the energy distribution peaks at low energy, uniformly
decreasing up to about 54~MeV (see
Fig.~\ref{rmd-spect}). Above 54~MeV, the free muon probability is
zero, but the energy endpoint actually goes above 100~MeV for bound
$\mu^-$, albeit with very small probability. In addition to this inner
bremsstrahlung process, there will be a calculable contribution from
the bremsstrahlung of electrons from the dominant decay mode of the
muon, DIO. At energies above ~10 MeV, the backgrounds
are much less than at lower energies, possibly allowing a good signal
to background ratio for a normalization measurement. Using tagged electrons from DIO, we would measure RMD as
well as DIO rates. Photons from RMD (and hence electrons from pair
production in the target surrounding materials) and electrons
from DIO have endpoint energies equal to the conversion electron
energy, with probabilities decreasing rapidly as the energy
approaches the endpoint. These potential backgrounds are controlled
with sufficiently good conversion electron energy resolution. We note that using RMD photons may not be as clean as using muonic X-rays or activation gammas, depending on the quality of photon collimation to the detector, since the RMD spectrum is not unique to the target species, and the energy distribution is not ideal, dropping rapidly with increasing energy.
A NaI calorimeter will be used to measure the higher energy photons
and electrons from RMD and DIO. We have access to a large NaI
detector, however we are searching for a more easily managed small
array of crystals for this task which will be easier to transport, mount, and
shield.
With the implementation of an NaI calorimeter, we have the additional
possibility to affirm old measurements of the rate of radiative muon
capture (RMC) at energies from 55~MeV (just above the bulk of the muon
decay flux) to about 75-85~MeV (where the rate becomes too small to
measure at the integrated fluxes envisioned at PSI). The branching
ratio is on the order of $10^{-5}$. Pair production from the photons
produce electrons detectable above background in approximately the
same energy range, with the precise endpoint depending on the rest energies of the daughter nuclei
\subsubsection{WP3: Neutron Emission after Muon Capture}
\subsubsection*{Present knowledge}
\noindent Nucleon emission after muon capture, particularly the nuclear
dynamics, is not well understood. Neutron emission is described by direct
and evaporative processes with energies ranging from thermal up to some
50 MeV. However, most neutrons, at least for heavy nuclei, are emitted by
evaporation after an excited nucleus is formed. Theoretical
studies indicate that giant resonance levels, ~\cite{Lifshitz, Uberall} are
important doorways leading to neutron emission. If this is the case, the
reaction occurs through a two-step process as described by;
\\
\begin{eqnarray}
\mu^{-} + A(N,p) &\rightarrow& \nu_{\mu} \, + A(N+1,p-1)^{*} \\
\nonumber
A(N+1,p-1)^* & \rightarrow & xN\,+ \, x^{\prime} p \, + \,
x^{\prime\prime}\gamma
\end{eqnarray}
\noindent In the above reactions, the $x$'s represent emission of
any number of particles including photons as the nucleus de-excites.
If neutrons are emitted from giant
resonance excitation, broad peaks at lower energies would be
expected and are observed, Figure ~\ref{expCO} ~\cite{Plett}. Also,
one would expect multi-particle
emission, as has indeed been
observed for various targets ~\cite{Macdonald, Wyttenbach}.
Multiplicity measurements for targets of relevance ( close to Atomic
Numbers of Al and
Ti) are shown in Table ~\ref{multi_neut}.
\begin{table}[h!]
\caption{Neutron multiplicities for various targets. The distribution
is adjusted to 0.545~\cite{Macdonald}.}
\label{multi_neut}
\begin{center}
\begin{tabular}{lccccc}
\hline
\multicolumn{2}{c}{ } & \multicolumn{3}{c}{Multiplicity} \\
Target & Avg. Mult. & 0 & 1 & 2 & 3 \\
\hline
Al& $1.262 \pm 0.059$ & $0.449 \pm 0.027$ & $0.464 \pm 0.028$
& $0.052 \pm 0.0013 $& $ 0.036 \pm 0.007$\\
Si & $0.864 \pm 0.072$ & $0.611 \pm 0.042$ & $0.338 \pm 0.042$
& $0.045 \pm 0.0018 $& $ 0.000 \pm 0.008$\\
Ca & $0.746 \pm 0.032$ & $0.633 \pm 0.021$ & $0.335 \pm 0.022$ & $0.025 \pm
0.0009 $& $ 0.004 \pm 0.006$\\
Fe & $1.125 \pm 0.041$ & $0.495 \pm 0.018$ & $0.416 \pm 0.019$ & $0.074 \pm
0.0011 $& $ 0.014 \pm 0.005$\\
\hline
\end{tabular}
\end{center}
\end{table}
At higher energies, direct emission
involves photo-production on a proton in the nucleus, with the emission of a
neutron. The end-point energy of this process is
approximately 6 MeV for at rest protons, but protons move with Fermi
motion in the nucleus so
an energy spectrum is produced. Thus correlated proton-neutron
emission and proton-photon emission would be expected. Examples of
this are described in radio-chemical experiments ~\cite{Wyttenbach}.
\begin{figure}[htb!]
\begin{center}
\begin{minipage}{8.cm}
\includegraphics[width=7.5cm] {figs/C_O_exp_spectrum.pdf}
\caption{\label{expCO}
Spectra of neutron energies after muon capture showing emission from
giant resonance excitations in C (above) and O (below). Note the
rise in evaporative emission at low energies ~\cite{Plett}.}
\end{minipage}
\parbox{0.3 cm}{ }
\begin{minipage}{7. cm}
\includegraphics[width=6.3 cm, angle=180]{figs/exp_neutron_spectra.pdf}
\caption{\label{exp_neutron_spectra} Higher energy neutron
spectrum for various light nuclei. Note the exponential decrease
with energy ~\cite{Sundelin}.}
\end{minipage}
\end{center}
\end{figure}
\noindent A number of
experiments studied high energy neutron emission from targets as light as Si
in order to observe the neutron asymmetry. In the process of such measurements neutron
spectra were extracted ~\cite{Sundelin} and
examples are shown in Figure
~\ref{exp_neutron_spectra}.
These spectra have a low energy cut-off ranging from 4 to 10 MeV as only
direct emission is expected to preserve asymmetric emission.
They are consistent with an exponential decrease as a function of
increasing energy, and show no
indication of an evaporative increase or resonance emission at lower
energies. However, the break in the slope of the spectrum in
heavier nuclei occurs around 10 MeV, and evidence of a spectrum break
may have been missed due to the energy cut off . From these
data on Si, the
measured number of emitted neutrons per muon capture above
approximately 4 MeV is approximately 0.43.
This experimental result is
corrected for multiple neutron emission which is small, at least at
the measured energies.\\
\noindent In summary, the neutron energy spectrum seems
reasonably determined for neutron energies above 10 MeV. Low energy
emission depends on nuclear structure and is less well defined. At
energies of less than a few MeV there is an evaporative increase as
well as emission from giant resonant states. \\
\subsubsection*{Relevance for $\mu-e$ Conversion Experiments}
The Mu2e and COMET experiments stop negative muons in an $^{27}$Al
target. The
signal of interest is an
electron, emitted with approximately 100 MeV/c momentum.
The Mu2e tracking detector, which is constructed of straw-tubes or a
drift chamber, is
relatively insensitive to neutrons, but this is not the case for
the calorimeter, the cosmic ray veto scintillators, and the
readout electronics inside the detector solenoid. There is a large
flux of neutrons from the production target which is reduced by
shielding
between the production and detection solenoids. With this shielding in
place, simulation shows that neutrons from muon captures in the
stopping target then dominate the neutron background in the tracker,
Table ~\ref{neut_background}. Due to their proximities, neutron backgrounds in
the cosmic ray veto, and
particularly the calorimeter, are more sensitive to neutrons emitted
after muon capture in the
beam-stop.
\begin{table}[h!]
\caption{Neutron Background Sources on the Tracker as a function of
Neutron Kinetic Energy, $T$}
\label{neut_background}
\begin{center}
\begin{tabular}{cccc}
\hline
\multicolumn{1}{c}{ } & \multicolumn{3}{c}{Neutrons/$cm^{2}$ ($\times
10^{10}$) }\\
Source & Thermal($ T < 1$ eV) & Epithermal ($1 \mbox{eV} <
T < 1$ MeV) & Fast ($T > 1$ eV)\\
\hline
Stopping Target & 16 & 77 & 100 \\
Muon Beam Stop & 0.2 & 2 & 0.8 \\
Beam Flash & 0.2 & 1 & 2 \\
Production Solenoid & 0.6 & 0.09 & 0 \\
\hline
\end{tabular}
\end{center}
\end{table}
Aside from radiation damage to the electronics, fast neutrons cause single
event upsets (SEU) during dynamic operations in electronic systems.
Depending on the upset, redundancy, and software verification, these
either could be ignored, result in data contamination, or in
electronic failure. A dose of $5 \times10^{4}\,
n/s/cm^{2}$ was found using a MARS estimate of the neutron spectrum from the
stopping target
(see Fig.~\ref{fg:mars}). Thus, for a
nominal IC area of 1cm2, each IC must be tolerant to about $ 10^{12}$
neutrons which would be expected in $4 \times 10^{7}$ beam-on-target
seconds. Better limits on these estimations should be obtained.
\begin{figure}[htb!]
\begin{center}
\includegraphics[scale=0.70]{figs/mars_spectra.pdf}
\caption{\label{fg:mars}
The neutron energy spectrum after emission
from an Al Target as obtained from a MARS Simulation
and used as input to neutron background calculations}
\end{center}
\end{figure}
Many muons, protons, and photons produced in the stopping target reach the
calorimeter. The estimated rates of neutrons and gammas in the
calorimeter are approximately 300 kHz and 85 kHz, respectively.
Simulation shows this introduces pileup probabilities of 40\% and
20\%, but with average
energy depositions of 0.5 MeV and 0.7 MeV, respectively.
Background (e.g. false cosmic ray vetoes) in the cosmic ray veto, CRV,
must not affect live time by
more than 1\%. Most neutrons reaching the CRV have kinetic energies
below 10 MeV, with the most probable energy about 1 MeV. The CRV is
shielded by concrete and most likely Boron loaded polyethylene, the
thickness to be determined by shielding simulations.
The CRV scintillator (C8H8) is sensitive to neutrons
which capture and scatter on protons with a
cross section increasing with decreasing energy
(~1/velocity for the captures). Thus thermal and epithermal neutron
energies are most important. These neutrons would be
produced by attenuation of MeV neutrons as they penetrate
the shielding between the CRV and the stopping target
or the beam dump. Simulation studies for the neutron spectrum
at the CRV use Geant3 GCALOR with an input spectrum from
MARS as shown in Fig.~\ref{fg:mars}. This
spectrum is certainly not correct at low energies as seen
when compared to the C and O experimental data in Figure
~\ref{expCO} above.
Thus since detector design and simulation are based on input of
estimated neutron emission, as discussed above, it is important to
obtain reliable experimental measurements for calibration. As
examples, we must know the impact of radiation effects on the
electronics, and must design the detectors to reduce the effects of
neutron backgrounds.

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A neutrino and a charged lepton form a natural doublet in the SM, and
are assigned a flavor quantum number. The
observation that neutrinos oscillate between flavours and thus have
mass, means that lepton number is not absolutely conserved in the
neutral lepton sector and this in
turn means that lepton number is also not conserved in charged lepton
interactions. However, due to the large difference in mass between the
neutrino and the $W$ boson, the branching ratio for charged lepton
flavour violation (CLFV) in a minimal extension to the SM which
includes massive neutrinos, is extremely small
(${\cal{O}}(10^{-50})$). Thus, any experimental observation of CLFV would be
unambiguous evidence of new physics beyond the SM (BSM), and
particle physics experiments searching for CLFV are amongst those with
highest priority ~\cite{Kuno:1999jp}.
Most extensions to the SM predict rates for CLFV that are within reach
of the next generation of experiments. Indeed current experiments such
as MEG search for the CLFV process, $\mu^{+} \rightarrow
e^{+}\gamma$, and already place severe constraints on models of BSM
physics. It is possible to construct a generic Lagrangian for BSM CLFV
interactions~\cite{deGouvea} comprising dipole and
contact interaction terms at a certain mass scale
($\Lambda$). The $\mu^{+} \rightarrow e^{+}\gamma$ being probed by MEG,
is mainly sensitive to dipole interactions whereas processes such as
$\mu^{+} \rightarrow e^{+}e^{-}e^{+}$ and the coherent neutrinoless
transition of a muon in the field of a nucleus, \muec, are mainly
sensitive to contact interactions. Thus in order to elucidate the
nature of any BSM physics it is necessary to make measurements of all
three processes. In Fig.~\ref{fg:deGouvea} the rates of CLFV are shown
as a function of $\Lambda$ and the relative contribution of the dipole
and contact interactions ($\kappa$).
\begin{center}
\begin{figure}[htbp]
\hspace{30mm}
\includegraphics[width=0.6\textwidth]{figs/deGouvea.png}
\caption{Branching ratios for two CLFV processes in a generic model of
BSM physics having both dipole and contact interactions as a function
of the scale ($\Lambda$) of the new physics.}
\label{fg:deGouvea}
%\vspace{-5mm}
\end{figure}
\end{center}
It can be seen from Fig.~\ref{fg:deGouvea} that CLFV processes
potentially probe new physics at scales beyond the LHC. Dipole and
contact interactions arise in many models of BSM
physics. Supersymmetric interactions naturally provide dipole
interactions which could result in significant rates for both the
$\mu^{+} \rightarrow e^{+}\gamma$ and \muec processes while
contact interaction terms arise in type-II Seesaw models that generate
light neutrino masses through mixing with an additional massive
neutrino. In general the Seesaw mechanism occurs at a very high mass scales
(${\cal{O}}(10^{10-14})$~GeV). CLFV effects are only large if
additional new physics e.g. supersymmetry or extra dimensions are
present at the TeV scale. In general CLFV processes probe
physics both at the GUT-scale and the
TeV-scale. Fig.~\ref{fg:deGouvea} also highlights the necessity of
searching for CLFV in both the $\mu^{+} \rightarrow e^{+}\gamma$ and
\muec process (and also the $\mu^{+} \rightarrow e^{+}e^{-}e^{+}$
process) where the ratio of the branching ratios can yield information
on $\kappa$.
The last search for \muec conversion was performed by the SINDRUM
II collaboration at PSI. The SINDRUM II spectrometer consisted of a
set of concentric cylindrical drift chambers inside a superconducting
solenoid magnet of 1.2 Tesla. The experiment set an upper limit of \muec in Au
of $B(\mu^{-} + Au \rightarrow e^{-} + Au) < 7 \times
10^{-13}$~\cite{SindrumGold}. Two new searches for
CLFV in the \muec process are being pursued by
experiments under construction in the USA (Mu2e~\cite{mu2e08}) and
Japan (COMET~\cite{come07}), both of which seek to probe the
\muec process with a sensitivity better than $\sim
10^{-16}$. Schematic layouts of the experiments are shown in
Fig.~\ref{fg:mu2ecomet}. For BSM interactions dominated by dipole
operators these experiments have a similar sensitivity to the upgraded
MEG experiment but have a far greater sensitivity to contact
interactions.
The Mu2e and COMET experiments are seeking to improve on the SINDRUM
II sensitivity by a factor of 10,000. Both experiments utilise
multi-kW pulsed proton beams of energy 8--9~GeV produced by the FNAL
(Mu2e) and J-PARC (COMET) accelerator complexes. Mu2e received CD1 DOE
approval in July 2012 and the staged construction of COMET was
approved in March 2012 and construction of the beamline will begin in
2013. In the Phase-I COMET experiment, shown in Fig.~\ref{fg:phase1},
there is a reduced beamline and a cylindrical drift chamber will
immediately surround the target where the muons are captured. Thus, it is
very sensitive to the products of muon (and pion) nuclear capture. In
Mu2e there is a similar sensitivity since the straw tracking detector
is immediately downstream of the muon target.
\begin{center}
\begin{figure}[h]
%\vspace{-40mm}
\includegraphics[width=\textwidth]{figs/comet-mu2e.png}
\caption{Schematic layouts of the Mu2e (left) and the COMET Phase-II experiments (right).}
\label{fg:mu2ecomet}
%\vspace{-5mm}
\end{figure}
\end{center}
The $\mu^{-}N \rightarrow e^{-}N$ process is particularly
attractive since the experimental signature is very straightforward: a
single mono-energetic electron with an energy of approximately $m_\mu
- B$ where $B$ is the binding energy of the muon in the 1{\em s} level
in the muonic atom (N). This single particle signature does not suffer
from the accidental background which occurs when coincidences are
required; e.g. between $e^{+}$ and $\gamma$ in the $\mu^{+} \rightarrow
e^{+}\gamma$ process. This is a particularly important, limiting
background at
high muon rates. The energy of the mono-energetic electron from the \muec
process has far higher energy than in Michel decays, and for $\mu$
decays in orbit (DIO) the phase space for electron energies
approaching the endpoint rapidly vanishes.
In addition to the DIO process or the CLFV process a muon in the 1{\em
s} state in a muonic atom can be captured by the nucleus via the
process: $\mu^{-} + N(A,Z) \rightarrow \nu_{\mu} + N(A,Z-1)$. In
general this process is also accompanied by the emission of photons,
neutrons and charged particles (particularly protons) and it is the
measurement of these emitted particles that is the subject of this
proposal. In order to optimize $\mu \to e$ experiments, it is important
to accurately know the rate and energy spectra of these particles,
since they can form significant backgrounds, degrade the
efficiency of electron tracking, and damage the readout electronics.
Photons can Compton scatter or convert,
producing electrons which cause ambiguities in track reconstruction
and degrade detector resolutions. In addition to these problems, low
energy protons can
saturate the electronic amplifiers due to large energy losses, and
prematurely ``age'' detector components.
Neutrons cause recoil protons and can get captured,
producing photons. Low-energy neutron cross sections are large and
are difficult to shield. They can cause significant radiation damage.
Monte-Carlo simulations of these nuclear
capture processes rely on spectra
data taken over twenty years ago for a limited number of nuclei in
a restricted energy range. Low energy energy neutron spectra are
particularly dependent on the nucleus. The
motivation for this proposal is to make precision measurements for the
target materials that will be used by Mu2e and COMET over the entire
relevant energy region.
\begin{center}
\begin{figure}[htbp]
\hspace{15mm}
\includegraphics[width=0.8\textwidth]{figs/comet_phase1_tracker.pdf}
\caption{The COMET Phase-I detector where a cylindrical drift chamber immediately surrounds the muon stopping target and is therefore subject to the products of the nuclear muon capture process.}
\label{fg:phase1}
%\vspace{-5mm}
\end{figure}
\end{center}

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file = ProposalPSI
all:
pdflatex $(file)
bibtex $(file)
pdflatex $(file)
pdflatex $(file)
clean:
rm *.aux *.log *.bbl *.dvi *.blg *.out *.toc

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\input{neutronsPW.tex}

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The organization and responsibilities for the three work packages is given below.
\begin{table}[ht!]
\begin{center}
\caption{Main responsibilities for work packages of the AlCap experiment} \label{tb:organization}
\vspace{5mm}
\begin{tabular}{cccccc} \hline
Work Package & Set-up & Detectors & Electronics & DAQ & Simulation/Analysis \\
\hline
WP1 & UW, OU & UW, OU, FNAL & UW, OU &
OU, UCL & OU, UCL, UW \\
WP2 & PNNL & PNNL, BU & PNNL,UW & PNNL, OU &
PNNL, BU \\
WP3 & UH, ANL & UH, UW & ANL & ANL, OU & UH, ANL \\
\hline
\end{tabular}
\end{center}
\end{table}
\subsubsection{WP1}
We have a vacuum chamber and Si detectors, which were used for a
similar measurement at PSI in 2009. The
vacuum chamber is being tested now at University of Washington
(UW). The two exiting Si detectors are also being
tested at UW. A
possibility to prepare another set of Si detectors is being
considered. Amplifiers for the existing SI detects are available. The
Osaka University (OU) group is preparing DAQ system based on a PSI
standard data acquisition system (MIDAS). Monte Carlo
simulations necessary to optimize detector configuration is undergoing
at OU and University College London (UCL).
Data will be analyzed independently at Osaka University, University of
Washington, and University College London, using standard analysis libraries
and our own analysis routines. There is no special requirement on data analysis
support to PSI.
\subsubsection{WP2}
PNNL has a number of HPGe detectors available; one appropriate for the
experiment will be chosen and tested in advance. A mechanical cooling
system is currently under test at PNNL as well and is expected to be
used at PSI. Due to the desired high rate and resolution requirements
for the raw HPGe pulse data, PNNL will provide its own DAQ system for
data collection. The raw data will be provided to the other DAQ
system if desired, and the coordination and timestamps between the two
systems will be handled carefully.
HPGe data will be analyzed at Pacific Northwest National Laboratory
using standard analysis libraries and our own analysis routines.
There is no special requirement on data analysis support to PSI.
\subsubsection{WP3}
As mentioned above, we plan to use existing neutron detectors and
readout electronics provided by the MuSun collaboration. We are also
considering to build a small neutron detectors, with optimal
resolution. We plan to calibrate the detectors before the final
experiment and have started to study and test unfolding methods.

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%[This is not official and for distribution, as we still have to discuss with TRIUMF management.]
An initial test run for measuring protons emitted from Al targets was performed by a subset of this collaboration
at PSI in 2009. It helped to commission part of the apparatus used for the current proposal. It also showed
deficiencies which helped to define and optimize the set-up proposed here. In particular, the beam
quality, the X-ray detection, the thin dE/dx detectors, the shielding of stray muons etc. need additional
careful attention.
In 2012, a joint COMET/Mu2e project on charged particle emission was started, when the high relevance of
proton emission for the new COMET Phase-I idea was realized. Due to the geographical advantage of
Vancouver, as a good crossing point for the Fermilab and J-PARC collaboration, a proposal~\cite{triumf12}
was submitted to TRIUMF in summer 2012, and accepted with high priority. The PAC recommendation reads:\\
{\it\bf ``The proposed set of muon capture background measurements are deemed crucial to the design and understanding of future neutrino-less muon-to-electron decay experiments, such as COMET and mu2e. Thus the committee approves this proposal with high scientific priority.
It is noted that it is not yet clear which muon beamline will be available for this study with the desired negative muon properties.
Once a suitable beamline has been identified that will be ready and available on the required timescales, the committee recommends that the full 36 shifts be granted.''}
Unfortunately, the above-mentioned availability of a suitable beamline for low energy $\mu^-$ turned out to be a problem.
The allocated test beam times in fall of 2012 could not be realized, as the M9B beamline experienced vacuum problems
at the T2 target station as well as difficulties with the superconducting decay channel. Moreover, TRIUMF cloud beamlines
with better momentum bin essential for this experiment, are not foreseen to be operated with negative muons.
In this situation, the collaboration asked the TRIUMF management to put S1371 on standby.
Meanwhile, PSI built a new low energy muon beam for particle physics, initially for the MuSun experiment. This
beamline was successfully commissioned by the MuSun collaboration, including some members of the present
collaboration. The results were extremely positive. In particular, the beamline appears to be the world-wide
superior channel for experiments needing muon beam \textit{at low energies with very narrow energy spread}.
This advantage is due to the high proton intensity at PSI, combined with a special cloud muon channel,
which selects the momentum with three bending magnets and thus allows for a dispersive focus.
The initial commissioning results by the MuSun collaboration promise excellent conditions for the thin
targets anticipated in AlCap. Further beam details are discussed in the MuSun progress report, submitted to this BVR.

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We anticipate that the WP1, WP2 and WP3 can be executed in two 4 weeks PSI beam blocks scheduled in
2013 and 2014. The first experiment would be used to commission the full set-up and shake down its
components. The priority would be to perform most of the proton measurements, while simultaneously
measuring the X-rays for WP2. A first neutron measurement is also anticipated. This part of the experiment
is ready in spring 2013, and we would prefer an early running time during the 2013 schedule. After that,
the data would be analyzed and results reported at the BVR 2014. Depending on the outcome, in the run
2014, additional statistics data taking and systematic studies are foreseen to achieve publication quality
data. In addition, the large NaI would be installed for WP2 measurements.
\vspace{5mm}

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@article{deGouvea,
author = "A. deGouvea",
title = "{(Charged) Lepton Flavor Violation}",
journal = "Nucl. Phys. B (Proc. Suppl.)",
volume = "188",
pages = "303-308",
doi = "10.1016/j.nuclphysbps.2009.02.071",
year = "2009",
}
@Unpublished{hung34,
author = {{E. Hungerford}},
title = "{Comment on Proton Emission after Muon
Capture, MECO Note 34}",
note = {},
}
@article{mu2e08,
author = "{R. M. Carey {\it et al.} (Mu2e Collaboration)}",
title = "{Proposal to search for $\mu^-N \rightarrow e^- N$ with a single
event sensitivity below 10$^{-16}$}",
collaboration = "Mu2e Collaboration",
year = "2008",
reportNumber = "FERMILAB-PROPOSAL-0973",
SLACcitation = "%%CITATION = FERMILAB-PROPOSAL-0973 ETC.;%%",
}
@Article{phaseI,
author = "{Y. Kuno {\it et al.} (COMET collaboration)}",
title = "{Letter of
Intent of Phase-I for the COMET Experiment at J-PARC}",
journal = {},
year = {2012},
}
@Article{shera80,
author = {{E. B. Shera}},
title = "{Pionic and muonic atoms}",
journal = {Nucl. Phys. A},
volume = {335},
issue = {1},
pages = {75--82},
year = {1980},
publisher = {Elsevier}
}
@article{sobo68,
title = "{Energy Spectrum of Charged Particles Emitted Following Muon Capture in Si$^{28}$}",
author = {{S. Sobottka and E. Wills}},
journal = {Phys. Rev. Lett.},
volume = {20},
issue = {12},
pages = {596--598},
year = {1968},
doi = {10.1103/PhysRevLett.20.596},
publisher = {American Physical Society}
}
@Unpublished{triumf12,
author = "{P. Kammel, Y. Kuno {\it et al.} (AlCap collaboration)}",
title = "{TRIUMF Experiment S1371: Study of Muon Capture for Muon to Electron Conversion Experiments}",
note = {},
OPTkey = {},
OPTmonth = {},
year = {2012},
OPTannote = {}
}

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\documentclass[10pt]{article}
\usepackage{geometry}
\geometry{verbose,tmargin=20mm,bmargin=20mm,lmargin=30mm,rmargin=30mm}
\usepackage{graphics}
\usepackage{rotating}
\usepackage{subfigure}
\usepackage{textcomp}
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\usepackage[latin1]{inputenc}
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\usepackage{array}
\usepackage{longtable}
\usepackage{lscape}
\usepackage{calc}
\usepackage{multirow}
\usepackage{nomencl}
\usepackage{hhline}
\usepackage{ifthen}
\usepackage{url}
%\usepackage{cite}
\usepackage{lscape}
\usepackage[pdftex,bookmarks,colorlinks]{hyperref}
\hypersetup{
bookmarks=true, % show bookmarks bar?
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pdffitwindow=false, % window fit to page when opened
pdfstartview={FitH}, % fits the width of the page to the window
pdftitle={My title}, % title
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pdfcreator={Creator}, % creator of the document
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pdfkeywords={keyword1} {key2} {key3}, % list of keywords
pdfnewwindow=true, % links in new window
colorlinks=true, % false: boxed links; true: colored links
linkcolor=blue, % color of internal links (change box color with linkbordercolor)
citecolor=blue, % color of links to bibliography
filecolor=magenta, % color of file links
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\renewcommand{\thetable}{\arabic{table}}
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\begin{document}
\newlength{\gnumericTableWidth}
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\newcommand{\is}{$s^{-1}$}
\bibliographystyle{IEEEtran}
%\bibliographystyle{nature}
%\bibliographystyle{arnuke_revised}
\include{defs}
\input{Cover.tex}
% Yoshi, Peter, Jim
\tableofcontents
\newpage
\section{Beam Requirements and Beam Request}
\label{BeamRequirements}
\input{BeamRequirements.tex}
% Peter
\newpage
\section{Safety}
\label{}
\input{Safety.tex}
% Peter, Nam
\newpage
\section{Physics Motivation and Status}
\subsection{Introduction}
\label{Introduction}
\input{Introduction.tex}
% Yoshi, Jim
\subsection{Experimental Goals and Physics Processes}
\label{Goals}
\input{Goals.tex}
% Peter, Ed, Jim, Lynn Osaka, BU, UCL
\subsection{Project History and Unique PSI Capablities}
\label{PSI}
\input{PSI.tex}
%Peter
\section{Experimental Strategy and Equipment}
\subsection{Charged Particle Emission after Muon Capture}
\label{Protons}
\input{Protons.tex}
% Osaka, UW
\subsection{Gamma and X-ray emission after Muon Capture}
\label{Xray}
\input{Xray.tex}
% Lynn et al
\subsection{Neutrons Emission after Muon Capture}
\label{Neutrons}
\input{Neutrons.tex}
% Ed et al, Peter Winter
\section{Organization}
\subsection{Organization and Responsibilites}
\label{Organization}
\input{Organization.tex}
% Peter, Yoshi, Jim et al
%\subsection{Measuring Program and Timeline}
%\label{Program}
%\input{Program.tex}
% overview Peter, separate projects teamleaders
\subsection{Requests to PSI}
\label{Requests}
\input{Requests.tex}
% Yoshi, Peter
\newpage
\bibliography{ProposalPSI.bib}
\end{document}

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The goal of the experiment is a measurement of the rates and energy spectra of
charged particle emission after muon capture in; 1) the favored
conversion target,
Al, 2) in Si (as normalization and cross check), and 3) Ti (as an alternative
conversion target material). Both the rate and energy spectrum
would be measured at
5\% precision down to an energy of 2.5 MeV.
The basic requirements are summarized is Fig.~\ref{basic.fig}. As the emitted
charged particles deposit a significant amount of energy during their passage
through the target material, thin targets and thus excellent momentum
resolution of the low energy muon beam are critical for the experiment. This
is exactly the reason, why the older experiments, which were performed
with thick targets and less sophisticated beams, are unsuitable for providing
the required yield and spectral information at low energies.
The observed energy spectrum $g(T_f)$ of protons emitted from the stopping
target is a convolution of the initial capture spectrum $f(T_i)$ with a
response function $k(T_f,T_i)$:
\begin{equation}
g(T_f) = \int_0^\infty k(T_f,T_i) f(T_i) dT_i
\end{equation}
The response function can be readily calculated for a uniform muon stopping
distribution within the target depth. The resulting distortion of the original
energy distribution taken from Equ.~\ref{eq:protons} is illustrated in
Fig.~\ref{response.fig} for different target thickness.
\begin{figure}[htb]
\begin{center}
\includegraphics[width=\textwidth]{figs/protonrange.png}
\caption{Left: Momentum vs. energy for p, d, $\alpha$,
right: proton range
vs. energy in targets.}
\label{basic.fig}
\end{center}
\end{figure}
%\vskip-5ex
\begin{figure}[tb]
\begin{center}
\includegraphics[width=0.6\textwidth]{figs/Si_emitted.pdf}
\caption{Calculated proton emission spectrum as
function of target
thickness (red: 0 $\mu m$, green: 50 $\mu m$, blue:
100 $\mu m$, black :
1000 $\mu m$).}
\label{response.fig}
\end{center}
\end{figure}
\begin{figure}[tb]
\begin{center}
\includegraphics[width=0.39\textwidth]{figs/expcad.png}\hspace{1mm}\includegraphics[width=0.59\textwidth]{figs/exp.png}
\caption{Left: CAD of layout, right: picture of vacuum
vessel with detectors.}
\label{setup.fig}
\end{center}
\end{figure}
A schematic layout of the experimental setup is shown in Fig.~\ref{setup.fig}.
It will be an improved version of a test experiment performed by part of this
collaboration at PSI in 2009.
Low energy muons will be detected by external beam counters (scintillator and
wire chamber, not shown). The muons then enter a vacuum vessel though
a thin mylar
window and a fraction stopped in passive Al and Ti foils of 25 to 100 $\mu m$
thickness. These foils are aligned 45 degrees with respect to the
beam direction. As a cross check, muons
will also be stopped in active Si detectors used as targets. Two packages
of charged particle detectors are positioned on opposite sides, perpendicular
to the target surface. The geometry is chosen so as to minimize the path length
of the emitted protons, and limit their direction to be nearly perpendicular to
the detectors. This improves the PID resolution by dE/dx separation. The main
detector of the package is a 5$\times$5 cm$^2$ Si detector of 1500 $\mu m$
thickness (MSX), which will stop protons up to about 12 MeV. Plastic
scintillators positioned
behind this Si detector observe higher energy protons and veto
through-going electrons. To provide dE/dx information some data will be taken
with two 10x10 cm$^2$ thin Si detectors (65 $\mu m$, MSQ). These detectors are
4-fold segmented. Since their large capacitance deteriorates the overall
resolution, measurements with and without them are foreseen. The symmetry
between the left and right Si stations allows for a powerful monitor of
systematic effects. Differences between the detectors would indicate background
due to different stopping materials, non--uniform stopping distributions, or
differences due to muon scattering. Careful shielding of direct or scattered
muons is required, as the stopping fraction is small and proton emission is a
rare capture branch. As shown, we are considering a geometry, where there is no
direct line of sight between any low Z material exposed to muons. Thus, all
shielding uses lead.
In order to normalize the number of muon-stops in the aluminum target, a
Germanium detector will be used to measure muonic X-rays from muons
that stop in the aluminum
target. We also will have telescopes to detect electrons from
muons for an additional normalization of muon-stops.
The main systematic issues are as follows.
\begin{itemize}
\item Deconvolute the original proton spectrum $f(T_i)$. An optimal
cloud muon beam is requested for the experiment. Then an active
Si target allows an experimental calibration of the response function,
because both $T_i$ and $T_f$ are accessible with an active target.
\item Absolute calibration. The number of muon stops will be determined with
the Ge detector. Again, the use of an active Si target allows a cross
calibration. The proton detection efficiency will be simulated
by Geant and calibrated with the active Si target.
\item PID. The PID of emitted charged particles will be determined by dE/dx.
The use of time of flight will be investigated.
\item Background. Electron background will be determined with $\mu^+$, neutron
recoils by absorbing the proton component before the Si detectors. A
dangerous background are muons stops in walls and scattered into the Si
detector.\footnote{If the low energy target scattering is too
high, we are also studying a configuration, with the two Si
detectors positioned symmetrically and perpendicular to the beam.}
\end{itemize}
A realistic Geant4 simulation is being developed. It will serve as an important
tool to optimize the geometry, in particular the investigation of the
background and response
function. Currently the geometry of the PSI test run is being implemented for a
realistic check of the simulation.
\begin{figure}[htb]
\begin{center}
\includegraphics[width=0.8\textwidth]{figs/dEdx_new.pdf}
\caption{Two dimensional plots of energy deposit in
Si1 (65 $\mu$m) vs sum of that in Si1 (65 $\mu$m) and Si2 (1500$\mu$m)
(horizontal) counters. The protons can be distinguished from
deuterons and
tritons in the range of 2.5 $-$ 10
MeV. The low energy particles near zero point are electrons
and photons.}
\label{fg:dedx}
\end{center}
\end{figure}
\begin{table}[htb]
\begin{center}
\caption{
\label{tb:rates} Estimated event rates for various targets of different
thickness. Incoming $10^{4}$ muons/sec and proton
emission rate of
0.15 per muon capture are assumed. The efficiency of
Si detector of
100 \% is also assumed. \label{tb:rates} }
\vskip1ex
%\scalebox{0.75}{
\begin{tabular}{|c|c|c|c|c|}
\hline
Target & Muon momentum &\% Stopping & Event rate (Hz) & Event rate (Hz) \\
thickness ($\mu$m)& (MeV/c) &in target & All particles
& Protons \\
\hline
50 & 26 & 22.2 & 34.8 & 4.6 \\
100 & 27 & 32.9 & 48.5 & 5.4 \\
150 & 28 & 38.5 & 54.5 & 4.8 \\
200 & 28 & 51.2 & 47.7 & 4.5 \\
%50 & 26 & 22.2 & 14.8 & 2.3 \\
%100 & 27 & 32.9 & 18.5 & 2.1 \\
%150 & 28 & 38.5 & 16.6 & 1.7 \\
%200 & 28 & 51.2 & 19.8 & 2.0 \\
\hline
\end{tabular}
%}
\end{center}
\end{table}
Figure~\ref{fg:dedx} shows Monte Carlo simulation studies of two-dimensional
plots of energy in the MSQ counter (dE/dX) vs. energy of the MSX counter. From
Fig.~\ref{fg:dedx}, it is clearly seen that we can discriminate protons,
deuterons, scattered muons, and electrons up to 10 MeV.
The event rates are estimated based on Monte Carlo simulation. Preliminary
results are summarized in Table~\ref{tb:rates}. They will be updated once we
have full information about the PSI beam properties. As seen in
Table~\ref{tb:rates}, proton rates are not large. Additional collimation,
if required to obtain background reduction, and the low muon momenta,
which might require the use of degraders, may further reduce the rates
below these estimates.
A muon beam
of low and well defined momentum is of critical importance.

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We request limited hardware support from PSI. This includes\\
\begin{enumerate}
\item A temperature controlled tent for the set-up - probably the MuSun installation can be used,\\
\item 4 NIM and 1 VME crate and 2 racks,\\
\item Standard NIM electronic modules, to be specified. \\
\item Availability of liquid nitrogen for cooling of the germanium detector, if the mechanical cooler is identified as insufficient.\\
\end{enumerate}

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\begin{enumerate}
\item Radiation: standard PSI calibration sources will be used.
\item High voltages for photomultiplier and MWPCs: commercial
and safety accredited
HV supply units, cables and SHV connectors will be used.
\item Fire and explosion: no explosive material will be used in the
experiment.
\item Cryogenic apparatus: liquid nitrogen may be used for the Ge detector,
standard precautions will be taken.
\item The proton measurement uses an evacuated target chamber, with a mylar
window of standard PSI beam window design.
\item Flammable gas with small flux ($<$ 50 cc/min) will be used for the wire chamber;
standard gas detectors and alarm system will monitor gas leaks.
\end{enumerate}

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The conversion experiment proposes to monitor the number of stopped muons
by measuring the various muonic X-rays generated by the captured muons
as they cascade down to the muonic atom ground state. We propose to
test this scheme at PSI, as well as two alternate normalization
methods.
At PSI, we propose to install a high-purity germanium detector at a
port in the stopping target vacuum vessel to measure the rate of
muonic X-ray production and hence the number of muons stopped in the
target. Table \ref{tb:xray_energies} lists the most prevalent gamma
rays from the Si, Al, and Ti targets.
Typical energy resolution of the HPGe detector will be of order 2~keV
for 1~MeV photons. Normalization of the other measurements in this
proposal will rely on the HPGe detector, although use of an active Si
target will provide a useful cross-check.
A mechanical cooling system will be provided for the HPGe detector,
eliminating the need for a liquid nitrogen supply, although cooling
with cryogens is still a possibility if the mechanical system is
deemed insufficient. A high-speed, 14-16 bit data acquisition system
will be used to record and store high-resolution raw waveforms for
offline analysis, although real-time spectra will also be available
for monitoring. The raw data stream will be provided to the
DAQ systems of the other detectors.
Measurements of particular interest using the Mu2e germanium detector
include the muonic X-ray and gamma spectra as well as careful analysis
of both immediate and long-term effects of neutron on the detector.
Fast neutrons can create spurious peaks due to excitation of Ge nuclei
through inelastic neutron scattering, background signals from activation
products in both the detector and surrounding cryostat, and long-term
resolution degradation due to creation of hole-trapping defects in the
germanium lattice. The distance between the target and HPGe detector
in the PSI experiment will be selected such that long-term damage to
the HPGe is minimized, although the actual neutron flux is expected to
be small.
A large NaI detector will be used to measure the high energy photons
from the muon stopping target, with the primary goal of evaluating alternative
means of monitoring the stopped muon rate. Photons from radiative muon
decay have a probability distribution that decreases to nearly zero at
about 54~MeV. The NaI detector has 9 PMTs viewing a large single
crystal, whose signals will be digitized using waveform digitizers and
then fed into the regular DAQ data stream. The rate of photons from
radiative muon capture, ranging up to about 80-90~MeV, will also be
measured.
\begin{table}[ht!]
\begin{center}
\caption{Energies of muonic X-rays in selected target elements.}
\label{tb:xray_energies}
\vspace{5mm}
\begin{tabular}{|l|rrr|}
\hline
Transition & Si (keV) & Al (keV) & Ti (keV) \\
\hline
$2p \rightarrow 1s$ & 400 & 347 & 1021 \\
$3p \rightarrow 1s$ & 477 & 413 & 1210 \\
$4p \rightarrow 1s$ & 504 & 436 & 1277 \\
$3d \rightarrow 2p$ & 77 & 66 & 189 \\
\hline
\end{tabular}
\end{center}
\end{table}

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%.pdf: %.tex Makefile
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#pdflatex $<
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689 1096 bf 8 6 698 1096 bf 9 6 706 1096 bf 9 6 715 1096 bf 8 6 724 1096 bf 9 6 732 1096 bf 9 6 741 1096 bf 9 6 750 1096 bf 8 6 759 1096 bf 9 6 767 1096 bf 9 6 776 1096 bf 8 6 785 1096 bf 9 6 793 1096 bf 9 6 802 1096 bf 8 6 811 1096 bf 9 6 819 1096
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628 1116 bf 8 7 637 1116 bf 9 7 645 1116 bf 9 7 654 1116 bf 8 7 663 1116 bf 9 7 671 1116 bf 9 7 680 1116 bf 9 7 689 1116 bf 8 7 698 1116 bf 9 7 706 1116 bf 9 7 715 1116 bf 8 7 724 1116 bf 9 7 732 1116 bf 9 7 741 1116 bf 9 7 750 1116 bf 8 7 759 1116
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776 1163 bf 8 7 785 1163 bf 9 7 793 1163 bf 9 7 802 1163 bf 8 7 811 1163 bf 9 7 828 1163 bf 9 7 837 1163 bf 8 7 846 1163 bf 9 7 854 1163 bf 8 7 872 1163 bf 9 7 898 1163 bf 9 7 915 1163 bf 9 7 227 1170 bf 9 7 236 1170 bf 9 7 253 1170 bf 8 7 428 1170
bf 9 7 436 1170 bf 9 7 445 1170 bf 8 7 454 1170 bf 9 7 462 1170 bf 9 7 471 1170 bf 9 7 480 1170 bf 8 7 489 1170 bf 9 7 497 1170 bf 9 7 506 1170 bf 8 7 515 1170 bf 9 7 523 1170 bf 9 7 532 1170 bf 9 7 541 1170 bf 8 7 550 1170 bf 9 7 558 1170 bf 9 7
567 1170 bf 8 7 576 1170 bf 9 7 584 1170 bf 8 7 637 1170 bf 9 7 645 1170 bf 9 7 689 1170 bf 8 7 724 1170 bf 9 7 732 1170 bf 9 7 741 1170 bf 9 7 750 1170 bf 8 7 759 1170 bf 9 7 767 1170 bf 9 7 776 1170 bf 8 7 785 1170 bf 9 7 793 1170 bf 9 7 802 1170
bf 8 7 811 1170 bf 9 7 819 1170 bf 9 7 828 1170 bf 8 7 846 1170 bf 9 7 889 1170 bf 9 6 227 1177 bf 9 6 236 1177 bf 9 6 410 1177 bf 9 6 419 1177 bf 8 6 428 1177 bf 9 6 436 1177 bf 9 6 445 1177 bf 8 6 454 1177 bf 9 6 462 1177 bf 9 6 471 1177 bf 9 6
480 1177 bf 8 6 489 1177 bf 9 6 497 1177 bf 9 6 506 1177 bf 9 6 532 1177 bf 8 6 550 1177 bf 9 6 584 1177 bf 9 6 593 1177 bf 8 6 602 1177 bf 8 6 637 1177 bf 9 6 680 1177 bf 9 6 689 1177 bf 9 6 706 1177 bf 9 6 715 1177 bf 8 6 724 1177 bf 9 6 732 1177
bf 9 6 741 1177 bf 9 6 750 1177 bf 8 6 759 1177 bf 9 6 767 1177 bf 9 6 776 1177 bf 9 6 793 1177 bf 9 6 802 1177 bf 8 6 811 1177 bf 9 6 819 1177 bf 9 6 837 1177 bf 9 6 854 1177 bf 9 6 924 1177 bf 9 6 950 1177 bf 9 7 236 1183 bf 8 7 245 1183 bf 8 7
393 1183 bf 9 7 401 1183 bf 9 7 419 1183 bf 8 7 428 1183 bf 9 7 436 1183 bf 9 7 445 1183 bf 8 7 454 1183 bf 9 7 462 1183 bf 9 7 471 1183 bf 9 7 480 1183 bf 8 7 489 1183 bf 9 7 497 1183 bf 9 7 506 1183 bf 8 7 515 1183 bf 9 7 523 1183 bf 9 7 532 1183
bf 9 7 541 1183 bf 8 7 550 1183 bf 8 7 602 1183 bf 9 7 628 1183 bf 9 7 654 1183 bf 9 7 680 1183 bf 8 7 698 1183 bf 9 7 706 1183 bf 9 7 732 1183 bf 9 7 741 1183 bf 9 7 750 1183 bf 8 7 759 1183 bf 9 7 767 1183 bf 9 7 776 1183 bf 8 7 785 1183 bf 9 7
802 1183 bf 8 7 811 1183 bf 9 7 915 1183 bf 9 7 941 1183 bf 9 7 950 1183 bf 8 7 959 1183 bf 9 7 985 1183 bf 8 7 994 1183 bf 9 7 236 1190 bf 8 7 245 1190 bf 9 7 401 1190 bf 9 7 410 1190 bf 9 7 419 1190 bf 8 7 428 1190 bf 9 7 436 1190 bf 9 7 445 1190
bf 8 7 454 1190 bf 9 7 462 1190 bf 9 7 471 1190 bf 9 7 480 1190 bf 8 7 489 1190 bf 9 7 497 1190 bf 9 7 506 1190 bf 8 7 515 1190 bf 9 7 523 1190 bf 9 7 532 1190 bf 8 7 550 1190 bf 9 7 558 1190 bf 8 7 576 1190 bf 9 7 619 1190 bf 9 7 628 1190 bf 8 7
637 1190 bf 9 7 645 1190 bf 9 7 654 1190 bf 9 7 671 1190 bf 9 7 680 1190 bf 9 7 689 1190 bf 8 7 698 1190 bf 9 7 706 1190 bf 9 7 715 1190 bf 9 7 732 1190 bf 9 7 767 1190 bf 9 7 828 1190 bf 9 7 941 1190 bf 9 7 950 1190 bf 9 7 976 1190 bf 8 7 994 1190
bf 8 7 245 1197 bf 9 7 253 1197 bf 9 7 384 1197 bf 9 7 401 1197 bf 9 7 410 1197 bf 9 7 419 1197 bf 8 7 428 1197 bf 9 7 436 1197 bf 9 7 445 1197 bf 8 7 454 1197 bf 9 7 462 1197 bf 9 7 471 1197 bf 9 7 480 1197 bf 8 7 489 1197 bf 9 7 497 1197 bf 9 7
567 1197 bf 9 7 584 1197 bf 8 7 637 1197 bf 9 7 645 1197 bf 8 7 663 1197 bf 9 7 671 1197 bf 9 7 680 1197 bf 9 7 689 1197 bf 8 7 698 1197 bf 9 7 706 1197 bf 9 7 715 1197 bf 8 7 724 1197 bf 9 7 732 1197 bf 9 7 741 1197 bf 8 7 759 1197 bf 9 7 802 1197
bf 9 7 854 1197 bf 9 7 863 1197 bf 8 7 872 1197 bf 9 7 880 1197 bf 9 7 889 1197 bf 8 7 907 1197 bf 8 6 245 1204 bf 9 6 253 1204 bf 8 6 393 1204 bf 9 6 401 1204 bf 9 6 410 1204 bf 9 6 419 1204 bf 8 6 428 1204 bf 9 6 436 1204 bf 9 6 445 1204 bf 8 6
454 1204 bf 9 6 462 1204 bf 9 6 471 1204 bf 9 6 480 1204 bf 8 6 489 1204 bf 9 6 497 1204 bf 9 6 506 1204 bf 9 6 523 1204 bf 8 6 602 1204 bf 9 6 619 1204 bf 9 6 628 1204 bf 8 6 637 1204 bf 9 6 645 1204 bf 8 6 663 1204 bf 9 6 671 1204 bf 9 6 680 1204
bf 9 6 689 1204 bf 8 6 698 1204 bf 9 6 706 1204 bf 9 6 741 1204 bf 9 6 750 1204 bf 9 6 767 1204 bf 8 6 846 1204 bf 9 6 854 1204 bf 9 6 863 1204 bf 8 6 872 1204 bf 9 6 924 1204 bf 9 6 941 1204 bf 9 7 253 1210 bf 9 7 384 1210 bf 8 7 393 1210 bf 9 7
401 1210 bf 9 7 410 1210 bf 9 7 419 1210 bf 8 7 428 1210 bf 9 7 436 1210 bf 9 7 445 1210 bf 8 7 454 1210 bf 9 7 471 1210 bf 9 7 480 1210 bf 8 7 489 1210 bf 9 7 506 1210 bf 9 7 584 1210 bf 9 7 610 1210 bf 9 7 619 1210 bf 9 7 628 1210 bf 8 7 637 1210
bf 9 7 645 1210 bf 9 7 654 1210 bf 8 7 663 1210 bf 9 7 680 1210 bf 9 7 689 1210 bf 9 7 706 1210 bf 9 7 715 1210 bf 9 7 776 1210 bf 8 7 907 1210 bf 9 7 924 1210 bf 9 7 950 1210 bf 9 7 253 1217 bf 9 7 262 1217 bf 9 7 384 1217 bf 8 7 393 1217 bf 9 7
401 1217 bf 9 7 410 1217 bf 9 7 419 1217 bf 8 7 428 1217 bf 9 7 436 1217 bf 9 7 445 1217 bf 8 7 454 1217 bf 9 7 462 1217 bf 8 7 489 1217 bf 9 7 497 1217 bf 9 7 523 1217 bf 9 7 584 1217 bf 9 7 593 1217 bf 8 7 602 1217 bf 9 7 610 1217 bf 9 7 619 1217
bf 9 7 628 1217 bf 9 7 645 1217 bf 8 7 663 1217 bf 8 7 698 1217 bf 9 7 715 1217 bf 9 7 776 1217 bf 9 7 802 1217 bf 8 7 811 1217 bf 9 7 828 1217 bf 9 7 837 1217 bf 9 7 863 1217 bf 9 7 915 1217 bf 8 7 933 1217 bf 9 7 967 1217 bf 9 7 253 1224 bf 9 7
262 1224 bf 8 7 393 1224 bf 9 7 401 1224 bf 9 7 410 1224 bf 9 7 419 1224 bf 8 7 428 1224 bf 9 7 436 1224 bf 9 7 445 1224 bf 8 7 454 1224 bf 9 7 462 1224 bf 9 7 471 1224 bf 9 7 480 1224 bf 8 7 489 1224 bf 8 7 515 1224 bf 9 7 567 1224 bf 8 7 576 1224
bf 9 7 584 1224 bf 9 7 593 1224 bf 8 7 602 1224 bf 9 7 610 1224 bf 9 7 619 1224 bf 9 7 628 1224 bf 8 7 637 1224 bf 9 7 645 1224 bf 9 7 654 1224 bf 8 7 663 1224 bf 9 7 715 1224 bf 9 7 767 1224 bf 9 7 793 1224 bf 8 7 811 1224 bf 9 7 819 1224 bf 9 7
837 1224 bf 9 7 854 1224 bf 9 6 262 1231 bf 9 6 271 1231 bf 8 6 367 1231 bf 9 6 375 1231 bf 9 6 384 1231 bf 8 6 393 1231 bf 9 6 401 1231 bf 9 6 410 1231 bf 9 6 419 1231 bf 8 6 428 1231 bf 9 6 436 1231 bf 8 6 454 1231 bf 9 6 462 1231 bf 9 6 471 1231
bf 9 6 558 1231 bf 9 6 567 1231 bf 8 6 576 1231 bf 9 6 593 1231 bf 8 6 602 1231 bf 9 6 610 1231 bf 9 6 619 1231 bf 9 6 628 1231 bf 8 6 637 1231 bf 9 6 645 1231 bf 9 6 654 1231 bf 8 6 663 1231 bf 9 6 671 1231 bf 8 6 724 1231 bf 9 6 732 1231 bf 9 6
741 1231 bf 8 6 785 1231 bf 9 6 793 1231 bf 9 6 802 1231 bf 8 6 811 1231 bf 9 7 262 1237 bf 9 7 271 1237 bf 9 7 358 1237 bf 8 7 367 1237 bf 9 7 375 1237 bf 9 7 384 1237 bf 8 7 393 1237 bf 9 7 401 1237 bf 9 7 410 1237 bf 9 7 419 1237 bf 8 7 428 1237
bf 9 7 436 1237 bf 9 7 445 1237 bf 8 7 454 1237 bf 9 7 462 1237 bf 9 7 497 1237 bf 9 7 523 1237 bf 9 7 558 1237 bf 9 7 567 1237 bf 8 7 576 1237 bf 9 7 584 1237 bf 8 7 602 1237 bf 9 7 610 1237 bf 9 7 645 1237 bf 9 7 680 1237 bf 8 7 724 1237 bf 9 7
767 1237 bf 9 7 802 1237 bf 9 7 271 1244 bf 8 7 280 1244 bf 9 7 288 1244 bf 9 7 349 1244 bf 9 7 358 1244 bf 8 7 367 1244 bf 9 7 375 1244 bf 9 7 384 1244 bf 8 7 393 1244 bf 9 7 401 1244 bf 9 7 410 1244 bf 9 7 419 1244 bf 8 7 454 1244 bf 8 7 489 1244
bf 9 7 523 1244 bf 9 7 532 1244 bf 8 7 550 1244 bf 9 7 558 1244 bf 9 7 567 1244 bf 8 7 576 1244 bf 9 7 584 1244 bf 9 7 593 1244 bf 8 7 602 1244 bf 9 7 619 1244 bf 9 7 628 1244 bf 8 7 637 1244 bf 9 7 671 1244 bf 9 7 715 1244 bf 8 7 759 1244 bf 9 7
776 1244 bf 8 7 785 1244 bf 9 7 793 1244 bf 9 7 271 1251 bf 8 7 280 1251 bf 9 7 297 1251 bf 8 7 367 1251 bf 9 7 375 1251 bf 9 7 384 1251 bf 8 7 393 1251 bf 9 7 401 1251 bf 9 7 410 1251 bf 9 7 419 1251 bf 9 7 445 1251 bf 8 7 454 1251 bf 9 7 541 1251
bf 8 7 550 1251 bf 9 7 558 1251 bf 9 7 567 1251 bf 8 7 576 1251 bf 9 7 584 1251 bf 9 7 593 1251 bf 9 7 628 1251 bf 8 7 698 1251 bf 9 7 715 1251 bf 8 7 724 1251 bf 9 7 732 1251 bf 9 7 741 1251 bf 9 7 750 1251 bf 9 7 776 1251 bf 9 6 271 1258 bf 8 6
280 1258 bf 8 6 341 1258 bf 9 6 358 1258 bf 8 6 367 1258 bf 9 6 375 1258 bf 9 6 384 1258 bf 8 6 393 1258 bf 9 6 401 1258 bf 9 6 410 1258 bf 9 6 419 1258 bf 8 6 428 1258 bf 8 6 515 1258 bf 9 6 523 1258 bf 9 6 541 1258 bf 8 6 550 1258 bf 9 6 558 1258
bf 9 6 567 1258 bf 9 6 584 1258 bf 9 6 593 1258 bf 9 6 610 1258 bf 9 6 628 1258 bf 9 6 689 1258 bf 8 6 698 1258 bf 9 6 706 1258 bf 9 6 715 1258 bf 8 6 724 1258 bf 9 6 741 1258 bf 9 6 750 1258 bf 8 6 759 1258 bf 9 6 776 1258 bf 8 6 785 1258 bf 8 7
280 1264 bf 9 7 288 1264 bf 8 7 341 1264 bf 9 7 349 1264 bf 9 7 358 1264 bf 8 7 367 1264 bf 9 7 375 1264 bf 9 7 384 1264 bf 8 7 393 1264 bf 9 7 401 1264 bf 9 7 419 1264 bf 8 7 428 1264 bf 9 7 436 1264 bf 9 7 497 1264 bf 9 7 506 1264 bf 9 7 523 1264
bf 9 7 532 1264 bf 9 7 541 1264 bf 8 7 550 1264 bf 9 7 558 1264 bf 8 7 576 1264 bf 9 7 680 1264 bf 9 7 689 1264 bf 8 7 698 1264 bf 9 7 732 1264 bf 9 7 750 1264 bf 8 7 280 1271 bf 9 7 288 1271 bf 9 7 358 1271 bf 8 7 367 1271 bf 9 7 375 1271 bf 9 7
384 1271 bf 8 7 393 1271 bf 9 7 401 1271 bf 8 7 428 1271 bf 9 7 436 1271 bf 8 7 489 1271 bf 9 7 497 1271 bf 9 7 506 1271 bf 9 7 523 1271 bf 9 7 532 1271 bf 9 7 541 1271 bf 8 7 550 1271 bf 8 7 576 1271 bf 9 7 645 1271 bf 9 7 654 1271 bf 8 7 663 1271
bf 9 7 680 1271 bf 8 7 698 1271 bf 9 7 706 1271 bf 9 7 715 1271 bf 9 7 741 1271 bf 9 7 750 1271 bf 9 7 776 1271 bf 9 7 288 1278 bf 8 7 341 1278 bf 9 7 349 1278 bf 9 7 358 1278 bf 8 7 367 1278 bf 9 7 375 1278 bf 9 7 384 1278 bf 8 7 393 1278 bf 9 7
401 1278 bf 9 7 419 1278 bf 8 7 428 1278 bf 9 7 471 1278 bf 9 7 497 1278 bf 9 7 506 1278 bf 8 7 515 1278 bf 9 7 523 1278 bf 9 7 532 1278 bf 9 7 541 1278 bf 8 7 550 1278 bf 8 7 637 1278 bf 9 7 671 1278 bf 9 7 680 1278 bf 8 7 698 1278 bf 9 7 706 1278
bf 9 6 288 1285 bf 9 6 297 1285 bf 9 6 349 1285 bf 9 6 358 1285 bf 8 6 367 1285 bf 9 6 375 1285 bf 9 6 384 1285 bf 9 6 401 1285 bf 9 6 410 1285 bf 9 6 419 1285 bf 9 6 436 1285 bf 9 6 471 1285 bf 9 6 497 1285 bf 9 6 506 1285 bf 8 6 515 1285 bf 9 6
523 1285 bf 9 6 532 1285 bf 9 6 541 1285 bf 8 6 550 1285 bf 9 6 654 1285 bf 8 6 663 1285 bf 9 6 680 1285 bf 8 6 698 1285 bf 9 6 706 1285 bf 9 7 288 1291 bf 9 7 297 1291 bf 9 7 349 1291 bf 9 7 358 1291 bf 8 7 367 1291 bf 9 7 375 1291 bf 9 7 384 1291
bf 8 7 393 1291 bf 9 7 401 1291 bf 8 7 489 1291 bf 9 7 497 1291 bf 9 7 506 1291 bf 8 7 515 1291 bf 9 7 610 1291 bf 9 7 619 1291 bf 9 7 654 1291 bf 9 7 706 1291 bf 9 7 297 1298 bf 8 7 306 1298 bf 8 7 341 1298 bf 9 7 349 1298 bf 9 7 358 1298 bf 8 7
367 1298 bf 9 7 375 1298 bf 9 7 384 1298 bf 9 7 410 1298 bf 8 7 428 1298 bf 9 7 480 1298 bf 8 7 489 1298 bf 9 7 497 1298 bf 9 7 506 1298 bf 8 7 515 1298 bf 9 7 532 1298 bf 9 7 541 1298 bf 8 7 602 1298 bf 9 7 619 1298 bf 8 7 637 1298 bf 9 7 671 1298
bf 9 7 741 1298 bf 8 7 759 1298 bf 9 7 297 1305 bf 8 7 306 1305 bf 9 7 332 1305 bf 8 7 341 1305 bf 9 7 349 1305 bf 9 7 358 1305 bf 8 7 367 1305 bf 9 7 375 1305 bf 9 7 384 1305 bf 8 7 428 1305 bf 9 7 462 1305 bf 9 7 471 1305 bf 8 7 489 1305 bf 9 7
497 1305 bf 9 7 541 1305 bf 9 7 610 1305 bf 9 7 671 1305 bf 8 6 306 1312 bf 9 6 314 1312 bf 9 6 349 1312 bf 9 6 358 1312 bf 8 6 367 1312 bf 9 6 375 1312 bf 9 6 384 1312 bf 8 6 393 1312 bf 9 6 471 1312 bf 9 6 480 1312 bf 8 6 489 1312 bf 9 6 497 1312
bf 9 6 506 1312 bf 8 6 515 1312 bf 8 6 576 1312 bf 9 6 584 1312 bf 9 6 619 1312 bf 8 6 637 1312 bf 8 7 306 1318 bf 9 7 314 1318 bf 8 7 341 1318 bf 9 7 349 1318 bf 9 7 358 1318 bf 9 7 375 1318 bf 8 7 393 1318 bf 9 7 401 1318 bf 9 7 462 1318 bf 9 7
471 1318 bf 9 7 480 1318 bf 8 7 489 1318 bf 9 7 497 1318 bf 9 7 506 1318 bf 9 7 523 1318 bf 9 7 610 1318 bf 9 7 628 1318 bf 8 7 637 1318 bf 9 7 645 1318 bf 9 7 654 1318 bf 8 7 785 1318 bf 9 7 314 1325 bf 9 7 323 1325 bf 8 7 341 1325 bf 9 7 349 1325
bf 9 7 358 1325 bf 8 7 367 1325 bf 9 7 375 1325 bf 9 7 384 1325 bf 8 7 393 1325 bf 9 7 471 1325 bf 9 7 497 1325 bf 9 7 523 1325 bf 9 7 567 1325 bf 8 7 602 1325 bf 9 7 610 1325 bf 8 7 637 1325 bf 9 7 802 1325 bf 9 7 314 1332 bf 9 7 323 1332 bf 9 7
332 1332 bf 8 7 341 1332 bf 9 7 349 1332 bf 9 7 358 1332 bf 8 7 367 1332 bf 9 7 384 1332 bf 9 7 401 1332 bf 9 7 436 1332 bf 9 7 445 1332 bf 8 7 454 1332 bf 9 7 471 1332 bf 8 7 602 1332 bf 9 7 628 1332 bf 8 7 785 1332 bf 9 6 323 1339 bf 9 6 332 1339
bf 8 6 341 1339 bf 9 6 349 1339 bf 9 6 358 1339 bf 8 6 367 1339 bf 8 6 454 1339 bf 9 6 462 1339 bf 9 6 471 1339 bf 9 6 480 1339 bf 8 6 489 1339 bf 9 6 497 1339 bf 8 6 550 1339 bf 9 6 558 1339 bf 8 6 576 1339 bf 9 6 584 1339 bf 9 6 593 1339 bf 9 6
610 1339 bf 9 6 680 1339 bf 9 7 323 1345 bf 9 7 332 1345 bf 8 7 341 1345 bf 9 7 349 1345 bf 9 7 358 1345 bf 9 7 384 1345 bf 8 7 393 1345 bf 9 7 419 1345 bf 9 7 445 1345 bf 8 7 454 1345 bf 9 7 471 1345 bf 8 7 489 1345 bf 9 7 541 1345 bf 9 7 567 1345
bf 8 7 576 1345 bf 9 7 584 1345 bf 8 7 602 1345 bf 9 7 628 1345 bf 9 7 323 1352 bf 9 7 332 1352 bf 9 7 349 1352 bf 9 7 358 1352 bf 8 7 367 1352 bf 9 7 375 1352 bf 9 7 436 1352 bf 9 7 445 1352 bf 8 7 454 1352 bf 9 7 462 1352 bf 9 7 558 1352 bf 8 7
576 1352 bf 9 7 584 1352 bf 9 7 593 1352 bf 9 7 332 1359 bf 8 7 341 1359 bf 9 7 349 1359 bf 9 7 358 1359 bf 9 7 375 1359 bf 9 7 384 1359 bf 9 7 410 1359 bf 9 7 436 1359 bf 9 7 445 1359 bf 8 7 454 1359 bf 9 7 462 1359 bf 9 7 471 1359 bf 8 7 515 1359
bf 9 7 567 1359 bf 8 7 602 1359 bf 9 6 332 1366 bf 8 6 341 1366 bf 9 6 349 1366 bf 9 6 375 1366 bf 9 6 401 1366 bf 8 6 428 1366 bf 9 6 436 1366 bf 9 6 445 1366 bf 8 6 454 1366 bf 9 6 462 1366 bf 9 6 541 1366 bf 8 7 341 1372 bf 9 7 349 1372 bf 9 7
384 1372 bf 8 7 393 1372 bf 9 7 436 1372 bf 9 7 445 1372 bf 8 7 454 1372 bf 9 7 532 1372 bf 9 7 558 1372 bf 8 7 341 1379 bf 9 7 349 1379 bf 8 7 393 1379 bf 9 7 401 1379 bf 9 7 419 1379 bf 8 7 428 1379 bf 9 7 436 1379 bf 9 7 445 1379 bf 9 7 462 1379
bf 9 7 541 1379 bf 9 7 567 1379 bf 9 7 349 1386 bf 9 7 358 1386 bf 8 7 367 1386 bf 9 7 375 1386 bf 8 7 428 1386 bf 9 7 436 1386 bf 9 7 445 1386 bf 9 7 532 1386 bf 9 6 349 1393 bf 9 6 358 1393 bf 9 6 375 1393 bf 8 6 393 1393 bf 9 6 410 1393 bf 8 6
428 1393 bf 9 6 436 1393 bf 9 6 445 1393 bf 9 6 497 1393 bf 9 6 506 1393 bf 9 6 558 1393 bf 9 7 358 1399 bf 8 7 393 1399 bf 9 7 410 1399 bf 8 7 428 1399 bf 9 7 436 1399 bf 9 7 445 1399 bf 9 7 462 1399 bf 9 7 506 1399 bf 9 7 358 1406 bf 8 7 367 1406
bf 9 7 419 1406 bf 8 7 428 1406 bf 8 7 454 1406 bf 8 7 515 1406 bf 9 7 523 1406 bf 9 7 358 1413 bf 8 7 367 1413 bf 9 7 401 1413 bf 9 7 410 1413 bf 9 7 419 1413 bf 8 7 428 1413 bf 9 7 436 1413 bf 8 7 489 1413 bf 9 7 497 1413 bf 9 7 506 1413 bf 8 7
515 1413 bf 9 7 523 1413 bf 9 7 541 1413 bf 9 7 584 1413 bf 8 6 367 1420 bf 9 6 384 1420 bf 9 6 419 1420 bf 9 6 523 1420 bf 8 7 367 1426 bf 9 7 375 1426 bf 9 7 410 1426 bf 9 7 419 1426 bf 9 7 436 1426 bf 8 7 454 1426 bf 9 7 480 1426 bf 9 7 506 1426
bf 8 7 515 1426 bf 9 7 802 1426 bf 8 7 367 1433 bf 9 7 375 1433 bf 8 7 393 1433 bf 9 7 401 1433 bf 9 7 410 1433 bf 8 7 428 1433 bf 9 7 445 1433 bf 8 7 515 1433 bf 9 7 532 1433 bf 9 7 567 1433 bf 9 7 375 1440 bf 9 7 384 1440 bf 9 7 401 1440 bf 8 7
428 1440 bf 8 7 454 1440 bf 9 7 497 1440 bf 9 6 375 1447 bf 9 6 384 1447 bf 8 6 393 1447 bf 9 6 410 1447 bf 9 6 419 1447 bf 9 6 436 1447 bf 9 6 480 1447 bf 8 6 489 1447 bf 9 6 497 1447 bf 9 7 384 1453 bf 8 7 393 1453 bf 9 7 401 1453 bf 9 7 410 1453
bf 9 7 419 1453 bf 9 7 384 1460 bf 8 7 393 1460 bf 9 7 401 1460 bf 8 7 454 1460 bf 8 7 393 1467 bf 9 7 410 1467 bf 9 7 471 1467 bf 8 7 489 1467 bf 8 7 515 1467 bf 8 6 393 1474 bf 9 6 401 1474 bf 9 6 410 1474 bf 9 6 480 1474 bf 9 7 401 1480 bf 9 7
410 1480 bf 9 7 471 1480 bf 9 7 819 1480 bf 9 7 401 1487 bf 9 7 410 1487 bf 9 7 445 1487 bf 9 7 462 1487 bf 9 7 480 1487 bf 9 7 401 1494 bf 9 7 410 1494 bf 9 7 462 1494 bf 9 6 410 1501 bf 9 6 419 1501 bf 9 6 445 1501 bf 9 7 410 1507 bf 9 7 419 1507
bf 8 7 428 1507 bf 8 7 454 1507 bf 9 7 480 1507 bf 9 7 419 1514 bf 9 7 445 1514 bf 9 7 419 1521 bf 8 7 428 1521 bf 9 7 436 1521 bf 8 6 428 1528 bf 9 6 436 1528 bf 8 6 454 1528 bf 9 6 462 1528 bf 9 6 471 1528 bf 8 7 428 1534 bf 9 7 462 1534 bf 8 7
428 1541 bf 9 7 462 1541 bf 9 7 436 1548 bf 8 7 454 1548 bf 9 6 436 1555 bf 9 6 445 1555 bf 8 6 454 1555 bf 9 7 445 1561 bf 8 7 454 1561 bf 9 7 445 1568 bf 8 7 454 1568 bf 9 7 445 1575 bf 8 7 454 1575 bf 8 6 454 1582 bf 9 6 462 1582 bf 8 7 454 1588
bf 9 7 462 1588 bf 9 7 462 1595 bf 9 7 471 1602 bf 9 6 471 1609 bf 9 7 471 1615 bf 9 7 471 1622 bf 9 7 480 1622 bf 9 7 480 1629 bf 9 6 480 1636 bf 8 6 489 1636 bf 9 6 506 1636 bf 8 7 489 1642 bf 8 7 489 1649 bf 1 1 1 c black 132 981 m 870 X s
gsave 1088 844 23 896 C 569.206 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 1001 m -20 Y s 149 991 m -10 Y s 166 991 m -10 Y s 184 991 m -10 Y s 201 991 m -10 Y s 219 1001 m -20 Y s 236 991 m
-10 Y s 253 991 m -10 Y s 271 991 m -10 Y s 288 991 m -10 Y s 306 1001 m -20 Y s 323 991 m -10 Y s 341 991 m -10 Y s 358 991 m -10 Y s 375 991 m -10 Y s 393 1001 m -20 Y s 410 991 m -10 Y s 428 991 m -10 Y s 445 991 m -10 Y s 462 991 m -10 Y s 480
1001 m -20 Y s 497 991 m -10 Y s 515 991 m -10 Y s 532 991 m -10 Y s 550 991 m -10 Y s 567 1001 m -20 Y s 584 991 m -10 Y s 602 991 m -10 Y s 619 991 m -10 Y s 637 991 m -10 Y s 654 1001 m -20 Y s 671 991 m -10 Y s 689 991 m -10 Y s 706 991 m -10 Y
s 724 991 m -10 Y s 741 1001 m -20 Y s 759 991 m -10 Y s 776 991 m -10 Y s 793 991 m -10 Y s 811 991 m -10 Y s 828 1001 m -20 Y s 846 991 m -10 Y s 863 991 m -10 Y s 880 991 m -10 Y s 898 991 m -10 Y s 915 1001 m -20 Y s 933 991 m -10 Y s 950 991 m
-10 Y s 967 991 m -10 Y s 985 991 m -10 Y s 1002 1001 m -20 Y s
gsave 1088 844 23 896 C 120.672 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 182.146 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 268.665 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 355.185 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 441.704 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 23 896 C 530.5 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 23 896 C 617.019 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 23 896 C 703.539 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 23 896 C 790.058 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
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642 bf 9 7 445 682 bf 1 1 1 c black 132 102 m 870 X s
gsave 1088 843 23 18 C 569.206 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 122 m -20 Y s 149 112 m -10 Y s 166 112 m -10 Y s 184 112 m -10 Y s 201 112 m -10 Y s 219 122 m -20 Y s 236 112 m -10 Y
s 253 112 m -10 Y s 271 112 m -10 Y s 288 112 m -10 Y s 306 122 m -20 Y s 323 112 m -10 Y s 341 112 m -10 Y s 358 112 m -10 Y s 375 112 m -10 Y s 393 122 m -20 Y s 410 112 m -10 Y s 428 112 m -10 Y s 445 112 m -10 Y s 462 112 m -10 Y s 480 122 m -20
Y s 497 112 m -10 Y s 515 112 m -10 Y s 532 112 m -10 Y s 550 112 m -10 Y s 567 122 m -20 Y s 584 112 m -10 Y s 602 112 m -10 Y s 619 112 m -10 Y s 637 112 m -10 Y s 654 122 m -20 Y s 671 112 m -10 Y s 689 112 m -10 Y s 706 112 m -10 Y s 724 112 m
-10 Y s 741 122 m -20 Y s 759 112 m -10 Y s 776 112 m -10 Y s 793 112 m -10 Y s 811 112 m -10 Y s 828 122 m -20 Y s 846 112 m -10 Y s 863 112 m -10 Y s 880 112 m -10 Y s 898 112 m -10 Y s 915 122 m -20 Y s 933 112 m -10 Y s 950 112 m -10 Y s 967 112
m -10 Y s 985 112 m -10 Y s 1002 122 m -20 Y s
gsave 1088 843 23 18 C 120.672 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 23 18 C 182.146 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 23 18 C 268.665 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 23 18 C 355.185 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 23 18 C 441.704 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 843 23 18 C 530.5 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 843 23 18 C 617.019 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 843 23 18 C 703.539 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 843 23 18 C 790.058 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 843 23 18 C 876.577 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 843 23 18 C 956.266 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 777 m 870 X s 132 757 m 20 Y s 149 767 m 10 Y s 166 767 m 10 Y s 184 767 m 10 Y s 201 767 m 10 Y s 219 757 m 20 Y s 236 767 m 10 Y s 253
767 m 10 Y s 271 767 m 10 Y s 288 767 m 10 Y s 306 757 m 20 Y s 323 767 m 10 Y s 341 767 m 10 Y s 358 767 m 10 Y s 375 767 m 10 Y s 393 757 m 20 Y s 410 767 m 10 Y s 428 767 m 10 Y s 445 767 m 10 Y s 462 767 m 10 Y s 480 757 m 20 Y s 497 767 m 10 Y
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102 m 675 Y s
gsave 1088 843 23 18 C 54.6438 521.393 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 158 102 m -26 X s 145 118 m -13 X s 145 134 m -13 X s 145 150 m -13 X s 145 166 m -13 X s 158 182 m -26 X s 145 198 m -13 X s 145
214 m -13 X s 145 231 m -13 X s 145 247 m -13 X s 158 263 m -26 X s 145 279 m -13 X s 145 295 m -13 X s 145 311 m -13 X s 145 327 m -13 X s 158 343 m -26 X s 145 359 m -13 X s 145 375 m -13 X s 145 391 m -13 X s 145 407 m -13 X s 158 423 m -26 X s
145 439 m -13 X s 145 455 m -13 X s 145 472 m -13 X s 145 488 m -13 X s 158 504 m -26 X s 145 520 m -13 X s 145 536 m -13 X s 145 552 m -13 X s 145 568 m -13 X s 158 584 m -26 X s 145 600 m -13 X s 145 616 m -13 X s 145 632 m -13 X s 145 648 m -13 X
s 158 664 m -26 X s 145 680 m -13 X s 145 697 m -13 X s 145 713 m -13 X s 145 729 m -13 X s 158 745 m -26 X s 158 745 m -26 X s 145 761 m -13 X s 145 777 m -13 X s
gsave 1088 843 23 18 C 107.011 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 23 18 C 72.8584 170.762 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 843 23 18 C 54.6438 250.451 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 23 18 C 54.6438 330.139 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 843 23 18 C 54.6438 409.828 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 23 18 C 54.6438 491.794 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 843 23 18 C 54.6438 571.483 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 23 18 C 54.6438 651.172 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 843 23 18 C 54.6438 733.137 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 1002 102 m 675 Y s 976 102 m 26 X s 989 118 m 13 X s 989 134 m 13 X s 989 150 m 13 X s 989 166 m 13 X s 976 182 m 26 X s 989 198 m 13 X s 989
214 m 13 X s 989 231 m 13 X s 989 247 m 13 X s 976 263 m 26 X s 989 279 m 13 X s 989 295 m 13 X s 989 311 m 13 X s 989 327 m 13 X s 976 343 m 26 X s 989 359 m 13 X s 989 375 m 13 X s 989 391 m 13 X s 989 407 m 13 X s 976 423 m 26 X s 989 439 m 13 X
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13 X s 989 697 m 13 X s 989 713 m 13 X s 989 729 m 13 X s 976 745 m 26 X s 976 745 m 26 X s 989 761 m 13 X s 989 777 m 13 X s 0.386667 0 1 c 49 34 1008 102 bf 0.2 0 1 c 49 33 1008 136 bf 0 0.0800001 1 c 49 34 1008 169 bf 0 0.266667 1 c 49 34 1008
203 bf 0 0.546666 1 c 49 34 1008 237 bf 0 0.733333 1 c 49 33 1008 271 bf 0 1 0.986667 c 49 34 1008 304 bf 0 1 0.8 c 49 34 1008 338 bf 0 1 0.52 c 49 34 1008 372 bf 0 1 0.333333 c 49 33 1008 406 bf 0 1 0.0533333 c 49 34 1008 439 bf 0.133333 1 0 c 49
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34 1008 743 bf black 1057 102 m 675 Y s 1031 102 m 26 X s 1031 172 m 26 X s 1031 243 m 26 X s 1031 313 m 26 X s 1031 383 m 26 X s 1031 453 m 26 X s 1031 524 m 26 X s 1031 594 m 26 X s 1031 664 m 26 X s 1031 735 m 26 X s 1031 735 m 26 X s
gsave 1088 843 23 18 C 1061 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 23 18 C 1061 161.654 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5) show NC gr
gsave 1088 843 23 18 C 1061 229.959 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 843 23 18 C 1061 300.541 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (15) show NC gr
gsave 1088 843 23 18 C 1061 371.122 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (20) show NC gr
gsave 1088 843 23 18 C 1061 441.704 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (25) show NC gr
gsave 1088 843 23 18 C 1061 512.285 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (30) show NC gr
gsave 1088 843 23 18 C 1061 580.59 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (35) show NC gr
gsave 1088 843 23 18 C 1061 651.172 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (40) show NC gr
gsave 1088 843 23 18 C 1061 721.753 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (45) show NC gr 1 1 1 c 445 42 34 815 bf black 34 815 m 445 X s 479 815 m 42 Y s 479 857 m -445 X s 34 857 m -42 Y s 1 1 1 c black
gsave 1088 843 23 18 C 68.3047 824.21 t 0 r /Helvetica-Bold findfont 34.204 sf 0 0 m (Protons and deuterons) show NC gr 1 1 1 c 1088 843 1157 18 bf black 1 1 1 c 871 675 1265 102 bf black 871 675 1265 102 bl 1 1 1 c 871 675 1265 102 bf black 871
675 1265 102 bl 1 1 1 c 0 0.546666 1 c 9 7 1265 102 bf 0 0.266667 1 c 9 6 1265 109 bf 0.386667 0 1 c 8 6 1292 109 bf 9 6 1596 109 bf 0 0.0800001 1 c 9 7 1265 115 bf 0.386667 0 1 c 9 7 1274 115 bf 0 0.546666 1 c 9 7 1274 122 bf 0.386667 0 1 c 8 7
1884 122 bf 0 0.733333 1 c 9 7 1274 129 bf 0.386667 0 1 c 9 7 1283 129 bf 9 7 1788 129 bf 9 7 1953 129 bf 9 7 1962 129 bf 8 7 2119 129 bf 9 6 1274 136 bf 0 1 0.986667 c 9 6 1283 136 bf 0.386667 0 1 c 9 6 1387 136 bf 9 6 1892 136 bf 9 6 2014 136 bf 8
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bf 9 6 166 1042 bf 9 6 175 1042 bf 8 6 184 1042 bf 9 6 192 1042 bf 9 6 201 1042 bf 9 6 210 1042 bf 8 6 219 1042 bf 9 6 227 1042 bf 9 6 236 1042 bf 8 6 245 1042 bf 9 6 253 1042 bf 9 6 262 1042 bf 9 6 271 1042 bf 8 6 280 1042 bf 9 6 297 1042 bf 8 6
306 1042 bf 9 6 323 1042 bf 9 6 349 1042 bf 9 6 558 1042 bf 9 6 593 1042 bf 8 6 759 1042 bf 9 6 776 1042 bf 8 6 872 1042 bf 9 6 889 1042 bf 9 6 898 1042 bf 8 6 907 1042 bf 9 6 915 1042 bf 8 6 933 1042 bf 9 6 941 1042 bf 9 6 950 1042 bf 8 6 959 1042
bf 9 6 967 1042 bf 9 6 985 1042 bf 8 6 994 1042 bf 8 7 158 1048 bf 9 7 166 1048 bf 9 7 175 1048 bf 8 7 184 1048 bf 9 7 192 1048 bf 9 7 201 1048 bf 9 7 210 1048 bf 8 7 219 1048 bf 9 7 236 1048 bf 9 7 253 1048 bf 9 7 271 1048 bf 9 7 288 1048 bf 9 7
297 1048 bf 9 7 314 1048 bf 9 7 349 1048 bf 8 7 367 1048 bf 9 7 375 1048 bf 9 7 384 1048 bf 8 7 454 1048 bf 9 7 541 1048 bf 8 7 663 1048 bf 8 7 759 1048 bf 9 7 767 1048 bf 8 7 785 1048 bf 9 7 828 1048 bf 9 7 854 1048 bf 9 7 863 1048 bf 8 7 872 1048
bf 9 7 880 1048 bf 9 7 898 1048 bf 8 7 907 1048 bf 9 7 915 1048 bf 9 7 941 1048 bf 8 7 959 1048 bf 9 7 967 1048 bf 9 7 976 1048 bf 9 7 985 1048 bf 9 7 166 1055 bf 9 7 175 1055 bf 8 7 184 1055 bf 9 7 210 1055 bf 8 7 219 1055 bf 9 7 227 1055 bf 9 7
236 1055 bf 9 7 271 1055 bf 8 7 280 1055 bf 9 7 288 1055 bf 9 7 314 1055 bf 9 7 332 1055 bf 8 7 393 1055 bf 9 7 558 1055 bf 9 7 584 1055 bf 8 7 698 1055 bf 9 7 706 1055 bf 9 7 741 1055 bf 9 7 767 1055 bf 8 7 785 1055 bf 9 7 793 1055 bf 8 7 811 1055
bf 9 7 819 1055 bf 9 7 828 1055 bf 9 7 837 1055 bf 9 7 854 1055 bf 8 7 872 1055 bf 9 7 880 1055 bf 9 7 889 1055 bf 9 7 898 1055 bf 8 7 907 1055 bf 9 7 915 1055 bf 9 7 924 1055 bf 8 7 933 1055 bf 9 7 941 1055 bf 9 7 950 1055 bf 9 7 985 1055 bf 8 7
994 1055 bf 9 7 166 1062 bf 9 7 175 1062 bf 8 7 184 1062 bf 9 7 192 1062 bf 8 7 219 1062 bf 9 7 236 1062 bf 9 7 262 1062 bf 9 7 271 1062 bf 9 7 288 1062 bf 9 7 297 1062 bf 8 7 306 1062 bf 9 7 314 1062 bf 9 7 384 1062 bf 8 7 428 1062 bf 8 7 489 1062
bf 9 7 593 1062 bf 9 7 645 1062 bf 9 7 671 1062 bf 9 7 680 1062 bf 9 7 689 1062 bf 8 7 698 1062 bf 9 7 706 1062 bf 9 7 715 1062 bf 8 7 724 1062 bf 9 7 732 1062 bf 9 7 741 1062 bf 9 7 767 1062 bf 8 7 785 1062 bf 9 7 793 1062 bf 8 7 811 1062 bf 9 7
828 1062 bf 9 7 837 1062 bf 8 7 846 1062 bf 8 7 872 1062 bf 9 7 880 1062 bf 9 7 889 1062 bf 9 7 898 1062 bf 8 7 907 1062 bf 9 7 915 1062 bf 9 7 924 1062 bf 8 7 933 1062 bf 9 7 941 1062 bf 9 7 950 1062 bf 8 7 959 1062 bf 9 7 967 1062 bf 9 7 976 1062
bf 9 7 985 1062 bf 9 6 175 1069 bf 8 6 184 1069 bf 9 6 201 1069 bf 9 6 210 1069 bf 8 6 245 1069 bf 9 6 262 1069 bf 9 6 271 1069 bf 9 6 288 1069 bf 9 6 314 1069 bf 9 6 323 1069 bf 9 6 332 1069 bf 9 6 384 1069 bf 8 6 637 1069 bf 9 6 645 1069 bf 9 6
671 1069 bf 9 6 680 1069 bf 9 6 689 1069 bf 9 6 706 1069 bf 9 6 715 1069 bf 8 6 724 1069 bf 9 6 732 1069 bf 9 6 741 1069 bf 9 6 750 1069 bf 8 6 759 1069 bf 9 6 767 1069 bf 9 6 776 1069 bf 8 6 785 1069 bf 9 6 793 1069 bf 9 6 802 1069 bf 8 6 811 1069
bf 9 6 828 1069 bf 9 6 837 1069 bf 8 6 846 1069 bf 9 6 854 1069 bf 9 6 863 1069 bf 8 6 872 1069 bf 9 6 880 1069 bf 9 6 889 1069 bf 9 6 898 1069 bf 8 6 907 1069 bf 9 6 915 1069 bf 9 6 924 1069 bf 8 6 933 1069 bf 9 6 941 1069 bf 9 6 950 1069 bf 8 6
959 1069 bf 9 6 967 1069 bf 9 6 976 1069 bf 9 6 985 1069 bf 8 6 994 1069 bf 9 7 175 1075 bf 8 7 184 1075 bf 9 7 201 1075 bf 9 7 236 1075 bf 9 7 253 1075 bf 9 7 262 1075 bf 9 7 271 1075 bf 8 7 280 1075 bf 9 7 297 1075 bf 8 7 306 1075 bf 9 7 314 1075
bf 8 7 341 1075 bf 9 7 358 1075 bf 9 7 584 1075 bf 8 7 602 1075 bf 9 7 619 1075 bf 9 7 628 1075 bf 8 7 637 1075 bf 9 7 645 1075 bf 9 7 654 1075 bf 8 7 663 1075 bf 9 7 671 1075 bf 9 7 680 1075 bf 9 7 689 1075 bf 9 7 706 1075 bf 9 7 715 1075 bf 8 7
724 1075 bf 9 7 732 1075 bf 9 7 741 1075 bf 9 7 750 1075 bf 8 7 759 1075 bf 9 7 767 1075 bf 9 7 776 1075 bf 8 7 785 1075 bf 9 7 793 1075 bf 9 7 802 1075 bf 8 7 811 1075 bf 9 7 819 1075 bf 9 7 828 1075 bf 9 7 837 1075 bf 8 7 846 1075 bf 9 7 854 1075
bf 9 7 863 1075 bf 8 7 872 1075 bf 9 7 880 1075 bf 9 7 889 1075 bf 9 7 898 1075 bf 9 7 915 1075 bf 9 7 924 1075 bf 8 7 933 1075 bf 9 7 941 1075 bf 9 7 950 1075 bf 8 7 959 1075 bf 9 7 967 1075 bf 9 7 976 1075 bf 9 7 985 1075 bf 8 7 994 1075 bf 9 7
175 1082 bf 8 7 184 1082 bf 9 7 192 1082 bf 8 7 219 1082 bf 9 7 253 1082 bf 9 7 262 1082 bf 8 7 280 1082 bf 9 7 297 1082 bf 8 7 306 1082 bf 8 7 341 1082 bf 9 7 375 1082 bf 9 7 593 1082 bf 9 7 610 1082 bf 9 7 619 1082 bf 8 7 637 1082 bf 9 7 645 1082
bf 9 7 654 1082 bf 8 7 663 1082 bf 9 7 671 1082 bf 9 7 680 1082 bf 9 7 689 1082 bf 8 7 698 1082 bf 9 7 706 1082 bf 9 7 715 1082 bf 8 7 724 1082 bf 9 7 732 1082 bf 9 7 741 1082 bf 9 7 750 1082 bf 8 7 759 1082 bf 9 7 767 1082 bf 9 7 776 1082 bf 8 7
785 1082 bf 9 7 793 1082 bf 9 7 802 1082 bf 8 7 811 1082 bf 9 7 819 1082 bf 9 7 828 1082 bf 9 7 837 1082 bf 8 7 846 1082 bf 9 7 854 1082 bf 9 7 863 1082 bf 8 7 872 1082 bf 9 7 880 1082 bf 9 7 889 1082 bf 9 7 898 1082 bf 8 7 907 1082 bf 9 7 915 1082
bf 9 7 924 1082 bf 8 7 933 1082 bf 9 7 941 1082 bf 8 7 959 1082 bf 9 7 967 1082 bf 9 7 976 1082 bf 8 7 994 1082 bf 8 7 184 1089 bf 9 7 192 1089 bf 9 7 236 1089 bf 8 7 245 1089 bf 9 7 271 1089 bf 8 7 306 1089 bf 8 7 341 1089 bf 9 7 558 1089 bf 9 7
567 1089 bf 9 7 584 1089 bf 8 7 602 1089 bf 9 7 610 1089 bf 9 7 619 1089 bf 9 7 628 1089 bf 8 7 637 1089 bf 9 7 645 1089 bf 9 7 654 1089 bf 8 7 663 1089 bf 9 7 671 1089 bf 9 7 680 1089 bf 9 7 689 1089 bf 8 7 698 1089 bf 9 7 706 1089 bf 9 7 715 1089
bf 8 7 724 1089 bf 9 7 732 1089 bf 9 7 741 1089 bf 9 7 750 1089 bf 8 7 759 1089 bf 9 7 767 1089 bf 9 7 776 1089 bf 8 7 785 1089 bf 9 7 802 1089 bf 8 7 811 1089 bf 9 7 819 1089 bf 9 7 828 1089 bf 9 7 837 1089 bf 8 7 846 1089 bf 9 7 854 1089 bf 9 7
863 1089 bf 8 7 872 1089 bf 9 7 880 1089 bf 9 7 889 1089 bf 9 7 898 1089 bf 8 7 907 1089 bf 9 7 915 1089 bf 8 7 933 1089 bf 9 7 950 1089 bf 8 7 959 1089 bf 9 7 967 1089 bf 9 7 985 1089 bf 8 7 994 1089 bf 8 6 184 1096 bf 9 6 192 1096 bf 9 6 210 1096
bf 8 6 306 1096 bf 9 6 314 1096 bf 9 6 332 1096 bf 9 6 541 1096 bf 8 6 550 1096 bf 9 6 558 1096 bf 9 6 567 1096 bf 8 6 576 1096 bf 9 6 593 1096 bf 8 6 602 1096 bf 9 6 610 1096 bf 9 6 619 1096 bf 9 6 628 1096 bf 9 6 645 1096 bf 9 6 654 1096 bf 8 6
663 1096 bf 9 6 671 1096 bf 9 6 680 1096 bf 9 6 689 1096 bf 8 6 698 1096 bf 9 6 706 1096 bf 9 6 715 1096 bf 8 6 724 1096 bf 9 6 732 1096 bf 9 6 741 1096 bf 9 6 750 1096 bf 8 6 759 1096 bf 9 6 767 1096 bf 9 6 776 1096 bf 8 6 785 1096 bf 9 6 793 1096
bf 9 6 802 1096 bf 8 6 811 1096 bf 9 6 819 1096 bf 9 6 828 1096 bf 9 6 837 1096 bf 8 6 846 1096 bf 9 6 854 1096 bf 9 6 863 1096 bf 8 6 872 1096 bf 9 6 880 1096 bf 9 6 889 1096 bf 9 6 898 1096 bf 8 6 907 1096 bf 9 6 915 1096 bf 9 6 924 1096 bf 8 6
933 1096 bf 9 6 941 1096 bf 9 6 950 1096 bf 8 6 959 1096 bf 9 6 976 1096 bf 9 6 985 1096 bf 8 6 994 1096 bf 9 7 192 1102 bf 9 7 201 1102 bf 9 7 210 1102 bf 9 7 236 1102 bf 8 7 245 1102 bf 9 7 262 1102 bf 9 7 271 1102 bf 9 7 480 1102 bf 8 7 515 1102
bf 9 7 532 1102 bf 9 7 558 1102 bf 8 7 576 1102 bf 9 7 584 1102 bf 9 7 593 1102 bf 9 7 610 1102 bf 9 7 619 1102 bf 9 7 628 1102 bf 8 7 637 1102 bf 9 7 645 1102 bf 9 7 654 1102 bf 8 7 663 1102 bf 9 7 671 1102 bf 9 7 680 1102 bf 9 7 689 1102 bf 8 7
698 1102 bf 9 7 706 1102 bf 9 7 715 1102 bf 8 7 724 1102 bf 9 7 732 1102 bf 9 7 741 1102 bf 9 7 750 1102 bf 8 7 759 1102 bf 9 7 767 1102 bf 9 7 776 1102 bf 8 7 785 1102 bf 9 7 793 1102 bf 9 7 802 1102 bf 8 7 811 1102 bf 9 7 819 1102 bf 9 7 828 1102
bf 9 7 837 1102 bf 9 7 854 1102 bf 9 7 863 1102 bf 8 7 872 1102 bf 9 7 880 1102 bf 9 7 889 1102 bf 9 7 898 1102 bf 8 7 907 1102 bf 9 7 924 1102 bf 9 7 941 1102 bf 9 7 967 1102 bf 9 7 976 1102 bf 9 7 985 1102 bf 8 7 994 1102 bf 9 7 192 1109 bf 9 7
201 1109 bf 9 7 253 1109 bf 8 7 280 1109 bf 9 7 288 1109 bf 9 7 401 1109 bf 9 7 471 1109 bf 8 7 515 1109 bf 9 7 523 1109 bf 9 7 532 1109 bf 9 7 541 1109 bf 8 7 550 1109 bf 9 7 558 1109 bf 9 7 567 1109 bf 8 7 576 1109 bf 9 7 584 1109 bf 9 7 593 1109
bf 8 7 602 1109 bf 9 7 610 1109 bf 9 7 619 1109 bf 9 7 628 1109 bf 8 7 637 1109 bf 9 7 645 1109 bf 9 7 654 1109 bf 8 7 663 1109 bf 9 7 671 1109 bf 9 7 680 1109 bf 9 7 689 1109 bf 8 7 698 1109 bf 9 7 706 1109 bf 9 7 715 1109 bf 8 7 724 1109 bf 9 7
732 1109 bf 9 7 741 1109 bf 9 7 750 1109 bf 8 7 759 1109 bf 9 7 767 1109 bf 9 7 776 1109 bf 8 7 785 1109 bf 9 7 793 1109 bf 9 7 802 1109 bf 8 7 811 1109 bf 9 7 819 1109 bf 9 7 828 1109 bf 8 7 846 1109 bf 9 7 854 1109 bf 9 7 863 1109 bf 8 7 872 1109
bf 9 7 880 1109 bf 9 7 898 1109 bf 8 7 907 1109 bf 9 7 915 1109 bf 9 7 924 1109 bf 8 7 933 1109 bf 9 7 941 1109 bf 9 7 950 1109 bf 9 7 967 1109 bf 9 7 201 1116 bf 9 7 210 1116 bf 9 7 227 1116 bf 8 7 341 1116 bf 9 7 480 1116 bf 8 7 489 1116 bf 9 7
497 1116 bf 9 7 506 1116 bf 8 7 515 1116 bf 9 7 523 1116 bf 9 7 532 1116 bf 8 7 550 1116 bf 9 7 558 1116 bf 9 7 567 1116 bf 8 7 576 1116 bf 9 7 584 1116 bf 9 7 593 1116 bf 8 7 602 1116 bf 9 7 610 1116 bf 9 7 619 1116 bf 9 7 628 1116 bf 8 7 637 1116
bf 9 7 645 1116 bf 9 7 654 1116 bf 8 7 663 1116 bf 9 7 671 1116 bf 9 7 680 1116 bf 9 7 689 1116 bf 8 7 698 1116 bf 9 7 706 1116 bf 9 7 715 1116 bf 8 7 724 1116 bf 9 7 732 1116 bf 9 7 741 1116 bf 9 7 750 1116 bf 8 7 759 1116 bf 9 7 767 1116 bf 9 7
776 1116 bf 8 7 785 1116 bf 9 7 793 1116 bf 9 7 802 1116 bf 8 7 811 1116 bf 9 7 828 1116 bf 9 7 837 1116 bf 9 7 854 1116 bf 9 7 863 1116 bf 8 7 872 1116 bf 9 7 880 1116 bf 8 7 907 1116 bf 9 7 915 1116 bf 9 7 924 1116 bf 8 7 933 1116 bf 9 7 950 1116
bf 9 7 967 1116 bf 9 7 985 1116 bf 9 6 201 1123 bf 9 6 210 1123 bf 9 6 297 1123 bf 9 6 419 1123 bf 9 6 480 1123 bf 8 6 489 1123 bf 9 6 497 1123 bf 9 6 506 1123 bf 8 6 515 1123 bf 9 6 523 1123 bf 9 6 532 1123 bf 9 6 541 1123 bf 8 6 550 1123 bf 9 6
558 1123 bf 9 6 567 1123 bf 8 6 576 1123 bf 9 6 584 1123 bf 9 6 593 1123 bf 8 6 602 1123 bf 9 6 610 1123 bf 9 6 619 1123 bf 9 6 628 1123 bf 8 6 637 1123 bf 9 6 645 1123 bf 9 6 654 1123 bf 8 6 663 1123 bf 9 6 671 1123 bf 9 6 680 1123 bf 9 6 689 1123
bf 8 6 698 1123 bf 9 6 706 1123 bf 9 6 715 1123 bf 8 6 724 1123 bf 9 6 732 1123 bf 9 6 741 1123 bf 9 6 750 1123 bf 8 6 759 1123 bf 9 6 767 1123 bf 8 6 785 1123 bf 8 6 811 1123 bf 9 6 819 1123 bf 9 6 828 1123 bf 9 6 837 1123 bf 8 6 846 1123 bf 9 6
854 1123 bf 9 6 863 1123 bf 8 6 872 1123 bf 9 6 889 1123 bf 9 6 898 1123 bf 8 6 907 1123 bf 9 6 924 1123 bf 9 6 941 1123 bf 9 6 950 1123 bf 9 6 976 1123 bf 9 6 985 1123 bf 9 7 210 1129 bf 8 7 245 1129 bf 9 7 253 1129 bf 9 7 288 1129 bf 9 7 323 1129
bf 8 7 341 1129 bf 8 7 454 1129 bf 9 7 462 1129 bf 9 7 471 1129 bf 8 7 489 1129 bf 9 7 497 1129 bf 9 7 506 1129 bf 8 7 515 1129 bf 9 7 523 1129 bf 9 7 532 1129 bf 9 7 541 1129 bf 8 7 550 1129 bf 9 7 558 1129 bf 9 7 567 1129 bf 8 7 576 1129 bf 9 7
584 1129 bf 9 7 593 1129 bf 8 7 602 1129 bf 9 7 610 1129 bf 9 7 619 1129 bf 9 7 628 1129 bf 8 7 637 1129 bf 9 7 645 1129 bf 9 7 654 1129 bf 8 7 663 1129 bf 9 7 671 1129 bf 9 7 680 1129 bf 9 7 689 1129 bf 8 7 698 1129 bf 9 7 706 1129 bf 9 7 715 1129
bf 8 7 724 1129 bf 9 7 732 1129 bf 9 7 741 1129 bf 9 7 750 1129 bf 9 7 776 1129 bf 8 7 785 1129 bf 8 7 811 1129 bf 9 7 828 1129 bf 8 7 846 1129 bf 9 7 854 1129 bf 9 7 863 1129 bf 9 7 889 1129 bf 9 7 915 1129 bf 9 7 924 1129 bf 8 7 959 1129 bf 9 7
967 1129 bf 9 7 976 1129 bf 8 7 994 1129 bf 9 7 210 1136 bf 8 7 219 1136 bf 9 7 262 1136 bf 8 7 280 1136 bf 9 7 445 1136 bf 8 7 454 1136 bf 9 7 462 1136 bf 9 7 471 1136 bf 9 7 480 1136 bf 8 7 489 1136 bf 9 7 497 1136 bf 9 7 506 1136 bf 8 7 515 1136
bf 9 7 523 1136 bf 9 7 532 1136 bf 9 7 541 1136 bf 8 7 550 1136 bf 9 7 558 1136 bf 9 7 567 1136 bf 8 7 576 1136 bf 9 7 584 1136 bf 9 7 593 1136 bf 8 7 602 1136 bf 9 7 610 1136 bf 9 7 619 1136 bf 9 7 628 1136 bf 8 7 637 1136 bf 9 7 645 1136 bf 9 7
654 1136 bf 8 7 663 1136 bf 9 7 671 1136 bf 9 7 680 1136 bf 9 7 689 1136 bf 8 7 698 1136 bf 9 7 706 1136 bf 9 7 715 1136 bf 8 7 724 1136 bf 9 7 741 1136 bf 9 7 750 1136 bf 8 7 759 1136 bf 9 7 767 1136 bf 9 7 776 1136 bf 9 7 793 1136 bf 9 7 802 1136
bf 8 7 811 1136 bf 9 7 819 1136 bf 9 7 828 1136 bf 9 7 837 1136 bf 9 7 854 1136 bf 9 7 863 1136 bf 8 7 872 1136 bf 9 7 889 1136 bf 8 7 907 1136 bf 9 7 915 1136 bf 9 7 924 1136 bf 8 7 933 1136 bf 9 7 985 1136 bf 9 7 210 1143 bf 8 7 219 1143 bf 9 7
236 1143 bf 9 7 410 1143 bf 9 7 419 1143 bf 9 7 436 1143 bf 9 7 445 1143 bf 8 7 454 1143 bf 9 7 462 1143 bf 9 7 471 1143 bf 9 7 480 1143 bf 8 7 489 1143 bf 9 7 506 1143 bf 8 7 515 1143 bf 9 7 523 1143 bf 9 7 532 1143 bf 9 7 541 1143 bf 8 7 550 1143
bf 9 7 558 1143 bf 9 7 567 1143 bf 8 7 576 1143 bf 9 7 584 1143 bf 9 7 593 1143 bf 8 7 602 1143 bf 9 7 610 1143 bf 9 7 619 1143 bf 9 7 628 1143 bf 8 7 637 1143 bf 9 7 645 1143 bf 9 7 654 1143 bf 8 7 663 1143 bf 9 7 680 1143 bf 9 7 689 1143 bf 8 7
698 1143 bf 9 7 706 1143 bf 9 7 715 1143 bf 8 7 724 1143 bf 9 7 741 1143 bf 9 7 750 1143 bf 8 7 759 1143 bf 9 7 793 1143 bf 8 7 811 1143 bf 9 7 837 1143 bf 8 7 846 1143 bf 9 7 854 1143 bf 9 7 863 1143 bf 8 7 872 1143 bf 9 7 880 1143 bf 9 7 898 1143
bf 8 7 907 1143 bf 9 7 924 1143 bf 9 7 941 1143 bf 9 7 950 1143 bf 8 7 959 1143 bf 9 7 967 1143 bf 9 7 976 1143 bf 8 6 219 1150 bf 9 6 227 1150 bf 8 6 245 1150 bf 9 6 436 1150 bf 9 6 445 1150 bf 8 6 454 1150 bf 9 6 462 1150 bf 9 6 471 1150 bf 9 6
480 1150 bf 8 6 489 1150 bf 9 6 497 1150 bf 9 6 506 1150 bf 8 6 515 1150 bf 9 6 523 1150 bf 9 6 532 1150 bf 9 6 541 1150 bf 8 6 550 1150 bf 9 6 558 1150 bf 9 6 567 1150 bf 8 6 576 1150 bf 9 6 584 1150 bf 9 6 593 1150 bf 8 6 602 1150 bf 9 6 610 1150
bf 9 6 619 1150 bf 9 6 628 1150 bf 8 6 637 1150 bf 9 6 645 1150 bf 9 6 654 1150 bf 8 6 663 1150 bf 9 6 671 1150 bf 9 6 680 1150 bf 9 6 689 1150 bf 8 6 698 1150 bf 9 6 715 1150 bf 9 6 732 1150 bf 9 6 741 1150 bf 9 6 750 1150 bf 9 6 776 1150 bf 8 6
785 1150 bf 9 6 793 1150 bf 9 6 802 1150 bf 8 6 811 1150 bf 9 6 828 1150 bf 9 6 837 1150 bf 9 6 854 1150 bf 8 6 872 1150 bf 9 6 880 1150 bf 9 6 889 1150 bf 9 6 898 1150 bf 8 6 907 1150 bf 8 7 219 1156 bf 9 7 227 1156 bf 9 7 401 1156 bf 9 7 419 1156
bf 9 7 445 1156 bf 8 7 454 1156 bf 9 7 462 1156 bf 9 7 471 1156 bf 9 7 480 1156 bf 8 7 489 1156 bf 9 7 497 1156 bf 9 7 506 1156 bf 8 7 515 1156 bf 9 7 523 1156 bf 9 7 532 1156 bf 9 7 541 1156 bf 8 7 550 1156 bf 9 7 558 1156 bf 9 7 567 1156 bf 8 7
576 1156 bf 9 7 584 1156 bf 9 7 593 1156 bf 8 7 602 1156 bf 9 7 610 1156 bf 9 7 619 1156 bf 9 7 628 1156 bf 8 7 637 1156 bf 9 7 645 1156 bf 8 7 663 1156 bf 9 7 671 1156 bf 9 7 680 1156 bf 8 7 698 1156 bf 9 7 715 1156 bf 8 7 724 1156 bf 9 7 732 1156
bf 8 7 759 1156 bf 9 7 776 1156 bf 8 7 785 1156 bf 8 7 811 1156 bf 9 7 828 1156 bf 8 7 846 1156 bf 9 7 854 1156 bf 9 7 863 1156 bf 8 7 872 1156 bf 9 7 880 1156 bf 9 7 889 1156 bf 9 7 898 1156 bf 9 7 924 1156 bf 9 7 941 1156 bf 9 7 976 1156 bf 9 7
985 1156 bf 9 7 227 1163 bf 9 7 262 1163 bf 9 7 419 1163 bf 8 7 428 1163 bf 9 7 436 1163 bf 9 7 445 1163 bf 8 7 454 1163 bf 9 7 462 1163 bf 9 7 471 1163 bf 9 7 480 1163 bf 8 7 489 1163 bf 9 7 497 1163 bf 9 7 506 1163 bf 8 7 515 1163 bf 9 7 523 1163
bf 9 7 532 1163 bf 9 7 541 1163 bf 8 7 550 1163 bf 9 7 558 1163 bf 9 7 567 1163 bf 8 7 576 1163 bf 9 7 584 1163 bf 9 7 593 1163 bf 9 7 610 1163 bf 9 7 619 1163 bf 9 7 628 1163 bf 9 7 671 1163 bf 9 7 689 1163 bf 9 7 706 1163 bf 9 7 715 1163 bf 9 7
732 1163 bf 9 7 741 1163 bf 9 7 750 1163 bf 9 7 767 1163 bf 9 7 776 1163 bf 8 7 785 1163 bf 9 7 802 1163 bf 9 7 828 1163 bf 9 7 837 1163 bf 8 7 846 1163 bf 9 7 854 1163 bf 9 7 863 1163 bf 9 7 898 1163 bf 8 7 907 1163 bf 9 7 915 1163 bf 8 7 959 1163
bf 8 7 994 1163 bf 9 7 227 1170 bf 9 7 236 1170 bf 9 7 271 1170 bf 9 7 384 1170 bf 8 7 393 1170 bf 9 7 401 1170 bf 9 7 410 1170 bf 9 7 419 1170 bf 8 7 428 1170 bf 9 7 436 1170 bf 9 7 445 1170 bf 8 7 454 1170 bf 9 7 462 1170 bf 9 7 471 1170 bf 9 7
480 1170 bf 8 7 489 1170 bf 9 7 497 1170 bf 9 7 506 1170 bf 8 7 515 1170 bf 9 7 523 1170 bf 9 7 532 1170 bf 9 7 541 1170 bf 8 7 550 1170 bf 9 7 558 1170 bf 9 7 567 1170 bf 8 7 576 1170 bf 9 7 584 1170 bf 9 7 593 1170 bf 8 7 602 1170 bf 9 7 610 1170
bf 9 7 619 1170 bf 9 7 628 1170 bf 9 7 671 1170 bf 9 7 689 1170 bf 8 7 698 1170 bf 9 7 715 1170 bf 8 7 724 1170 bf 9 7 732 1170 bf 9 7 741 1170 bf 9 7 750 1170 bf 8 7 759 1170 bf 9 7 776 1170 bf 8 7 785 1170 bf 8 7 811 1170 bf 9 7 837 1170 bf 8 7
846 1170 bf 9 7 854 1170 bf 9 7 889 1170 bf 8 7 907 1170 bf 9 7 915 1170 bf 9 7 924 1170 bf 9 7 950 1170 bf 9 7 967 1170 bf 9 6 227 1177 bf 9 6 236 1177 bf 9 6 401 1177 bf 9 6 410 1177 bf 9 6 419 1177 bf 8 6 428 1177 bf 9 6 436 1177 bf 9 6 445 1177
bf 8 6 454 1177 bf 9 6 462 1177 bf 9 6 471 1177 bf 9 6 480 1177 bf 8 6 489 1177 bf 9 6 497 1177 bf 9 6 506 1177 bf 8 6 515 1177 bf 9 6 523 1177 bf 9 6 532 1177 bf 9 6 541 1177 bf 9 6 558 1177 bf 9 6 567 1177 bf 9 6 584 1177 bf 9 6 610 1177 bf 9 6
619 1177 bf 9 6 628 1177 bf 8 6 637 1177 bf 9 6 654 1177 bf 8 6 663 1177 bf 9 6 671 1177 bf 9 6 689 1177 bf 8 6 698 1177 bf 9 6 706 1177 bf 8 6 724 1177 bf 9 6 732 1177 bf 9 6 741 1177 bf 9 6 750 1177 bf 8 6 759 1177 bf 9 6 767 1177 bf 9 6 776 1177
bf 8 6 785 1177 bf 8 6 811 1177 bf 9 6 828 1177 bf 9 6 837 1177 bf 9 6 915 1177 bf 9 6 924 1177 bf 8 6 959 1177 bf 9 6 976 1177 bf 9 6 985 1177 bf 8 6 994 1177 bf 9 7 236 1183 bf 8 7 245 1183 bf 9 7 375 1183 bf 9 7 384 1183 bf 8 7 393 1183 bf 9 7
401 1183 bf 9 7 410 1183 bf 9 7 419 1183 bf 8 7 428 1183 bf 9 7 436 1183 bf 9 7 445 1183 bf 8 7 454 1183 bf 9 7 462 1183 bf 9 7 471 1183 bf 9 7 480 1183 bf 8 7 489 1183 bf 9 7 497 1183 bf 9 7 506 1183 bf 8 7 515 1183 bf 9 7 523 1183 bf 9 7 541 1183
bf 9 7 558 1183 bf 9 7 567 1183 bf 9 7 584 1183 bf 9 7 593 1183 bf 8 7 602 1183 bf 8 7 637 1183 bf 9 7 645 1183 bf 9 7 654 1183 bf 8 7 663 1183 bf 9 7 671 1183 bf 9 7 680 1183 bf 9 7 689 1183 bf 8 7 698 1183 bf 9 7 706 1183 bf 8 7 724 1183 bf 9 7
741 1183 bf 9 7 750 1183 bf 8 7 759 1183 bf 9 7 767 1183 bf 9 7 776 1183 bf 8 7 785 1183 bf 9 7 802 1183 bf 8 7 811 1183 bf 9 7 819 1183 bf 8 7 846 1183 bf 9 7 854 1183 bf 9 7 915 1183 bf 9 7 941 1183 bf 9 7 950 1183 bf 9 7 985 1183 bf 9 7 236 1190
bf 8 7 245 1190 bf 8 7 367 1190 bf 9 7 375 1190 bf 9 7 384 1190 bf 8 7 393 1190 bf 9 7 401 1190 bf 9 7 410 1190 bf 9 7 419 1190 bf 8 7 428 1190 bf 9 7 436 1190 bf 9 7 445 1190 bf 8 7 454 1190 bf 9 7 462 1190 bf 9 7 471 1190 bf 9 7 480 1190 bf 8 7
489 1190 bf 9 7 497 1190 bf 9 7 506 1190 bf 8 7 515 1190 bf 9 7 523 1190 bf 9 7 532 1190 bf 9 7 541 1190 bf 8 7 550 1190 bf 9 7 558 1190 bf 9 7 584 1190 bf 9 7 593 1190 bf 9 7 610 1190 bf 9 7 619 1190 bf 9 7 628 1190 bf 9 7 654 1190 bf 8 7 663 1190
bf 9 7 680 1190 bf 9 7 706 1190 bf 9 7 715 1190 bf 8 7 724 1190 bf 9 7 732 1190 bf 9 7 741 1190 bf 9 7 750 1190 bf 9 7 776 1190 bf 8 7 785 1190 bf 9 7 793 1190 bf 9 7 802 1190 bf 8 7 811 1190 bf 9 7 854 1190 bf 9 7 863 1190 bf 9 7 880 1190 bf 9 7
985 1190 bf 8 7 994 1190 bf 8 7 245 1197 bf 9 7 358 1197 bf 9 7 375 1197 bf 8 7 393 1197 bf 9 7 401 1197 bf 9 7 410 1197 bf 9 7 419 1197 bf 8 7 428 1197 bf 9 7 436 1197 bf 9 7 445 1197 bf 8 7 454 1197 bf 9 7 462 1197 bf 9 7 480 1197 bf 8 7 489 1197
bf 9 7 497 1197 bf 9 7 506 1197 bf 8 7 515 1197 bf 9 7 523 1197 bf 9 7 541 1197 bf 9 7 558 1197 bf 8 7 576 1197 bf 9 7 610 1197 bf 9 7 619 1197 bf 9 7 628 1197 bf 8 7 637 1197 bf 9 7 645 1197 bf 8 7 663 1197 bf 9 7 680 1197 bf 9 7 689 1197 bf 8 7
698 1197 bf 9 7 715 1197 bf 8 7 724 1197 bf 9 7 741 1197 bf 8 7 759 1197 bf 9 7 776 1197 bf 8 7 811 1197 bf 9 7 828 1197 bf 9 7 898 1197 bf 9 7 950 1197 bf 8 6 245 1204 bf 9 6 253 1204 bf 9 6 358 1204 bf 9 6 375 1204 bf 9 6 384 1204 bf 9 6 401 1204
bf 9 6 410 1204 bf 9 6 419 1204 bf 8 6 428 1204 bf 9 6 436 1204 bf 9 6 445 1204 bf 8 6 454 1204 bf 9 6 462 1204 bf 9 6 471 1204 bf 9 6 480 1204 bf 8 6 489 1204 bf 9 6 497 1204 bf 9 6 506 1204 bf 8 6 515 1204 bf 9 6 523 1204 bf 9 6 532 1204 bf 9 6
541 1204 bf 8 6 550 1204 bf 8 6 576 1204 bf 9 6 584 1204 bf 8 6 602 1204 bf 9 6 619 1204 bf 9 6 628 1204 bf 8 6 637 1204 bf 9 6 645 1204 bf 8 6 663 1204 bf 9 6 680 1204 bf 9 6 689 1204 bf 9 6 715 1204 bf 8 6 724 1204 bf 8 6 759 1204 bf 9 6 767 1204
bf 8 6 785 1204 bf 9 6 828 1204 bf 9 6 837 1204 bf 8 6 872 1204 bf 9 6 898 1204 bf 8 6 907 1204 bf 9 6 915 1204 bf 9 6 924 1204 bf 8 7 245 1210 bf 9 7 253 1210 bf 8 7 367 1210 bf 9 7 384 1210 bf 8 7 393 1210 bf 9 7 401 1210 bf 9 7 410 1210 bf 9 7
419 1210 bf 8 7 428 1210 bf 9 7 436 1210 bf 9 7 445 1210 bf 8 7 454 1210 bf 9 7 462 1210 bf 9 7 471 1210 bf 9 7 480 1210 bf 8 7 489 1210 bf 9 7 497 1210 bf 9 7 506 1210 bf 9 7 523 1210 bf 8 7 550 1210 bf 9 7 567 1210 bf 8 7 602 1210 bf 9 7 610 1210
bf 9 7 619 1210 bf 9 7 628 1210 bf 8 7 637 1210 bf 9 7 645 1210 bf 9 7 671 1210 bf 9 7 706 1210 bf 9 7 715 1210 bf 8 7 724 1210 bf 9 7 741 1210 bf 9 7 750 1210 bf 9 7 767 1210 bf 8 7 811 1210 bf 8 7 846 1210 bf 9 7 854 1210 bf 9 7 863 1210 bf 8 7
872 1210 bf 9 7 898 1210 bf 8 7 933 1210 bf 9 7 253 1217 bf 9 7 262 1217 bf 9 7 349 1217 bf 8 7 367 1217 bf 9 7 375 1217 bf 9 7 384 1217 bf 8 7 393 1217 bf 9 7 401 1217 bf 9 7 410 1217 bf 9 7 419 1217 bf 8 7 428 1217 bf 9 7 436 1217 bf 9 7 445 1217
bf 8 7 454 1217 bf 9 7 462 1217 bf 9 7 471 1217 bf 9 7 497 1217 bf 8 7 515 1217 bf 9 7 532 1217 bf 8 7 550 1217 bf 9 7 567 1217 bf 8 7 576 1217 bf 9 7 584 1217 bf 8 7 602 1217 bf 9 7 610 1217 bf 9 7 619 1217 bf 9 7 628 1217 bf 8 7 637 1217 bf 9 7
645 1217 bf 9 7 654 1217 bf 8 7 663 1217 bf 8 7 698 1217 bf 9 7 706 1217 bf 8 7 724 1217 bf 9 7 750 1217 bf 8 7 811 1217 bf 9 7 828 1217 bf 9 7 837 1217 bf 9 7 854 1217 bf 9 7 898 1217 bf 9 7 924 1217 bf 9 7 950 1217 bf 9 7 253 1224 bf 9 7 262 1224
bf 9 7 358 1224 bf 8 7 367 1224 bf 9 7 375 1224 bf 9 7 384 1224 bf 8 7 393 1224 bf 9 7 401 1224 bf 9 7 410 1224 bf 9 7 419 1224 bf 8 7 428 1224 bf 9 7 436 1224 bf 9 7 445 1224 bf 8 7 454 1224 bf 9 7 462 1224 bf 9 7 471 1224 bf 9 7 480 1224 bf 9 7
506 1224 bf 8 7 515 1224 bf 9 7 523 1224 bf 8 7 550 1224 bf 9 7 558 1224 bf 9 7 567 1224 bf 8 7 576 1224 bf 8 7 637 1224 bf 9 7 654 1224 bf 8 7 663 1224 bf 9 7 671 1224 bf 9 7 689 1224 bf 8 7 698 1224 bf 9 7 715 1224 bf 8 7 724 1224 bf 9 7 750 1224
bf 8 7 785 1224 bf 8 7 811 1224 bf 9 7 967 1224 bf 9 6 262 1231 bf 9 6 271 1231 bf 9 6 349 1231 bf 9 6 358 1231 bf 8 6 367 1231 bf 9 6 375 1231 bf 9 6 384 1231 bf 8 6 393 1231 bf 9 6 401 1231 bf 9 6 410 1231 bf 9 6 419 1231 bf 8 6 428 1231 bf 9 6
436 1231 bf 9 6 445 1231 bf 8 6 454 1231 bf 9 6 462 1231 bf 9 6 471 1231 bf 9 6 480 1231 bf 8 6 515 1231 bf 8 6 550 1231 bf 9 6 558 1231 bf 9 6 567 1231 bf 9 6 593 1231 bf 8 6 602 1231 bf 9 6 619 1231 bf 9 6 645 1231 bf 9 6 654 1231 bf 8 6 663 1231
bf 8 6 724 1231 bf 8 6 759 1231 bf 9 6 802 1231 bf 8 6 811 1231 bf 9 6 819 1231 bf 9 6 837 1231 bf 9 6 854 1231 bf 8 6 872 1231 bf 9 6 967 1231 bf 9 7 262 1237 bf 9 7 271 1237 bf 9 7 349 1237 bf 8 7 367 1237 bf 9 7 375 1237 bf 9 7 384 1237 bf 8 7
393 1237 bf 9 7 401 1237 bf 9 7 410 1237 bf 9 7 419 1237 bf 8 7 428 1237 bf 9 7 436 1237 bf 9 7 445 1237 bf 8 7 454 1237 bf 9 7 462 1237 bf 8 7 489 1237 bf 9 7 532 1237 bf 9 7 558 1237 bf 9 7 567 1237 bf 8 7 576 1237 bf 9 7 593 1237 bf 8 7 602 1237
bf 9 7 610 1237 bf 9 7 628 1237 bf 8 7 637 1237 bf 9 7 645 1237 bf 9 7 671 1237 bf 9 7 689 1237 bf 8 7 698 1237 bf 9 7 715 1237 bf 9 7 767 1237 bf 9 7 776 1237 bf 8 7 785 1237 bf 9 7 802 1237 bf 9 7 271 1244 bf 9 7 297 1244 bf 9 7 349 1244 bf 9 7
358 1244 bf 8 7 367 1244 bf 9 7 375 1244 bf 9 7 384 1244 bf 8 7 393 1244 bf 9 7 401 1244 bf 9 7 410 1244 bf 9 7 419 1244 bf 8 7 428 1244 bf 9 7 436 1244 bf 9 7 471 1244 bf 9 7 480 1244 bf 9 7 497 1244 bf 9 7 523 1244 bf 9 7 532 1244 bf 9 7 567 1244
bf 8 7 576 1244 bf 9 7 584 1244 bf 9 7 593 1244 bf 8 7 602 1244 bf 9 7 610 1244 bf 9 7 628 1244 bf 8 7 637 1244 bf 9 7 645 1244 bf 9 7 671 1244 bf 9 7 680 1244 bf 9 7 689 1244 bf 8 7 698 1244 bf 9 7 706 1244 bf 8 7 724 1244 bf 9 7 767 1244 bf 9 7
776 1244 bf 9 7 828 1244 bf 9 7 271 1251 bf 8 7 280 1251 bf 9 7 358 1251 bf 8 7 367 1251 bf 9 7 375 1251 bf 9 7 384 1251 bf 8 7 393 1251 bf 9 7 401 1251 bf 9 7 410 1251 bf 9 7 419 1251 bf 8 7 428 1251 bf 9 7 445 1251 bf 8 7 454 1251 bf 9 7 462 1251
bf 9 7 471 1251 bf 9 7 480 1251 bf 8 7 489 1251 bf 9 7 506 1251 bf 9 7 523 1251 bf 9 7 532 1251 bf 9 7 558 1251 bf 9 7 567 1251 bf 8 7 576 1251 bf 9 7 584 1251 bf 9 7 593 1251 bf 9 7 619 1251 bf 9 7 628 1251 bf 9 7 645 1251 bf 8 7 663 1251 bf 9 7
680 1251 bf 9 7 732 1251 bf 9 7 741 1251 bf 9 7 750 1251 bf 9 7 767 1251 bf 9 7 776 1251 bf 9 7 854 1251 bf 9 6 271 1258 bf 8 6 280 1258 bf 9 6 314 1258 bf 9 6 332 1258 bf 8 6 341 1258 bf 9 6 349 1258 bf 8 6 367 1258 bf 9 6 375 1258 bf 9 6 384 1258
bf 8 6 393 1258 bf 9 6 401 1258 bf 9 6 410 1258 bf 9 6 419 1258 bf 8 6 428 1258 bf 9 6 445 1258 bf 8 6 454 1258 bf 9 6 462 1258 bf 9 6 480 1258 bf 9 6 497 1258 bf 9 6 506 1258 bf 9 6 532 1258 bf 9 6 541 1258 bf 8 6 550 1258 bf 9 6 558 1258 bf 8 6
576 1258 bf 9 6 584 1258 bf 9 6 619 1258 bf 9 6 628 1258 bf 8 6 663 1258 bf 9 6 680 1258 bf 9 6 689 1258 bf 8 6 698 1258 bf 9 6 715 1258 bf 9 6 750 1258 bf 8 6 785 1258 bf 9 6 837 1258 bf 8 7 280 1264 bf 9 7 288 1264 bf 9 7 349 1264 bf 9 7 358 1264
bf 8 7 367 1264 bf 9 7 375 1264 bf 9 7 384 1264 bf 8 7 393 1264 bf 9 7 401 1264 bf 9 7 410 1264 bf 9 7 419 1264 bf 8 7 428 1264 bf 9 7 462 1264 bf 9 7 497 1264 bf 9 7 506 1264 bf 8 7 515 1264 bf 9 7 523 1264 bf 9 7 532 1264 bf 9 7 541 1264 bf 8 7
550 1264 bf 9 7 558 1264 bf 9 7 567 1264 bf 9 7 584 1264 bf 9 7 593 1264 bf 9 7 671 1264 bf 9 7 689 1264 bf 8 7 698 1264 bf 9 7 706 1264 bf 8 7 724 1264 bf 9 7 741 1264 bf 9 7 750 1264 bf 8 7 759 1264 bf 9 7 767 1264 bf 8 7 785 1264 bf 9 7 288 1271
bf 9 7 349 1271 bf 9 7 358 1271 bf 8 7 367 1271 bf 9 7 375 1271 bf 9 7 384 1271 bf 8 7 393 1271 bf 9 7 401 1271 bf 9 7 410 1271 bf 9 7 419 1271 bf 9 7 497 1271 bf 8 7 515 1271 bf 9 7 523 1271 bf 9 7 541 1271 bf 8 7 550 1271 bf 9 7 567 1271 bf 8 7
602 1271 bf 9 7 610 1271 bf 8 7 698 1271 bf 9 7 750 1271 bf 8 7 759 1271 bf 9 7 288 1278 bf 9 7 297 1278 bf 8 7 341 1278 bf 9 7 349 1278 bf 9 7 358 1278 bf 8 7 367 1278 bf 9 7 384 1278 bf 8 7 393 1278 bf 9 7 401 1278 bf 9 7 419 1278 bf 8 7 428 1278
bf 8 7 454 1278 bf 9 7 471 1278 bf 9 7 497 1278 bf 8 7 515 1278 bf 9 7 532 1278 bf 9 7 541 1278 bf 8 7 550 1278 bf 8 7 576 1278 bf 8 7 637 1278 bf 9 7 645 1278 bf 9 7 654 1278 bf 8 7 663 1278 bf 9 7 706 1278 bf 8 7 724 1278 bf 9 7 750 1278 bf 9 6
288 1285 bf 9 6 297 1285 bf 9 6 314 1285 bf 9 6 332 1285 bf 9 6 349 1285 bf 9 6 358 1285 bf 8 6 367 1285 bf 9 6 375 1285 bf 9 6 384 1285 bf 8 6 393 1285 bf 8 6 454 1285 bf 9 6 462 1285 bf 9 6 471 1285 bf 9 6 480 1285 bf 9 6 497 1285 bf 8 6 515 1285
bf 9 6 532 1285 bf 9 6 541 1285 bf 8 6 602 1285 bf 9 6 654 1285 bf 9 6 680 1285 bf 9 6 689 1285 bf 9 6 706 1285 bf 9 6 715 1285 bf 8 6 759 1285 bf 8 6 811 1285 bf 9 7 297 1291 bf 8 7 306 1291 bf 9 7 332 1291 bf 8 7 341 1291 bf 9 7 349 1291 bf 9 7
358 1291 bf 8 7 367 1291 bf 9 7 375 1291 bf 9 7 384 1291 bf 9 7 401 1291 bf 9 7 471 1291 bf 9 7 480 1291 bf 8 7 489 1291 bf 9 7 497 1291 bf 9 7 506 1291 bf 8 7 515 1291 bf 9 7 523 1291 bf 9 7 532 1291 bf 8 7 550 1291 bf 9 7 567 1291 bf 8 7 576 1291
bf 9 7 584 1291 bf 9 7 619 1291 bf 8 7 663 1291 bf 9 7 671 1291 bf 9 7 689 1291 bf 8 7 698 1291 bf 9 7 706 1291 bf 9 7 732 1291 bf 8 7 759 1291 bf 9 7 297 1298 bf 8 7 306 1298 bf 8 7 341 1298 bf 9 7 358 1298 bf 8 7 367 1298 bf 9 7 375 1298 bf 9 7
384 1298 bf 8 7 393 1298 bf 9 7 401 1298 bf 9 7 471 1298 bf 9 7 480 1298 bf 8 7 489 1298 bf 9 7 497 1298 bf 8 7 515 1298 bf 9 7 523 1298 bf 9 7 532 1298 bf 9 7 558 1298 bf 9 7 584 1298 bf 9 7 610 1298 bf 9 7 645 1298 bf 9 7 654 1298 bf 9 7 706 1298
bf 9 7 297 1305 bf 8 7 306 1305 bf 9 7 323 1305 bf 9 7 332 1305 bf 8 7 341 1305 bf 9 7 349 1305 bf 9 7 358 1305 bf 8 7 367 1305 bf 9 7 375 1305 bf 9 7 384 1305 bf 9 7 401 1305 bf 9 7 410 1305 bf 9 7 419 1305 bf 9 7 436 1305 bf 9 7 462 1305 bf 9 7
471 1305 bf 9 7 480 1305 bf 8 7 489 1305 bf 9 7 497 1305 bf 8 7 515 1305 bf 9 7 523 1305 bf 9 7 541 1305 bf 8 7 550 1305 bf 9 7 558 1305 bf 8 7 602 1305 bf 8 7 637 1305 bf 9 7 645 1305 bf 9 7 671 1305 bf 9 7 767 1305 bf 8 6 306 1312 bf 9 6 314 1312
bf 9 6 332 1312 bf 8 6 341 1312 bf 9 6 349 1312 bf 9 6 358 1312 bf 8 6 367 1312 bf 9 6 375 1312 bf 9 6 384 1312 bf 8 6 393 1312 bf 9 6 419 1312 bf 9 6 445 1312 bf 9 6 471 1312 bf 9 6 480 1312 bf 8 6 489 1312 bf 9 6 497 1312 bf 9 6 506 1312 bf 8 6
515 1312 bf 9 6 558 1312 bf 9 6 567 1312 bf 8 6 576 1312 bf 8 6 602 1312 bf 9 6 619 1312 bf 9 6 628 1312 bf 8 7 306 1318 bf 9 7 314 1318 bf 9 7 332 1318 bf 8 7 341 1318 bf 9 7 349 1318 bf 9 7 358 1318 bf 8 7 367 1318 bf 9 7 375 1318 bf 8 7 454 1318
bf 9 7 462 1318 bf 9 7 471 1318 bf 9 7 480 1318 bf 8 7 489 1318 bf 9 7 506 1318 bf 8 7 515 1318 bf 8 7 550 1318 bf 9 7 610 1318 bf 9 7 619 1318 bf 8 7 637 1318 bf 9 7 654 1318 bf 8 7 724 1318 bf 8 7 785 1318 bf 9 7 314 1325 bf 9 7 323 1325 bf 9 7
332 1325 bf 8 7 341 1325 bf 9 7 349 1325 bf 9 7 358 1325 bf 8 7 367 1325 bf 9 7 375 1325 bf 9 7 384 1325 bf 8 7 393 1325 bf 9 7 401 1325 bf 8 7 428 1325 bf 9 7 436 1325 bf 8 7 454 1325 bf 9 7 471 1325 bf 9 7 480 1325 bf 8 7 489 1325 bf 9 7 497 1325
bf 9 7 506 1325 bf 8 7 515 1325 bf 9 7 523 1325 bf 9 7 584 1325 bf 9 7 671 1325 bf 9 7 314 1332 bf 9 7 323 1332 bf 9 7 332 1332 bf 8 7 341 1332 bf 9 7 349 1332 bf 9 7 358 1332 bf 8 7 367 1332 bf 9 7 384 1332 bf 9 7 401 1332 bf 9 7 445 1332 bf 8 7
454 1332 bf 9 7 471 1332 bf 8 7 489 1332 bf 9 7 497 1332 bf 9 6 323 1339 bf 9 6 332 1339 bf 8 6 341 1339 bf 9 6 349 1339 bf 9 6 358 1339 bf 8 6 367 1339 bf 9 6 375 1339 bf 9 6 384 1339 bf 9 6 419 1339 bf 9 6 436 1339 bf 9 6 445 1339 bf 8 6 454 1339
bf 9 6 462 1339 bf 9 6 471 1339 bf 9 6 480 1339 bf 9 6 532 1339 bf 9 6 680 1339 bf 9 7 323 1345 bf 9 7 332 1345 bf 8 7 341 1345 bf 9 7 349 1345 bf 9 7 358 1345 bf 8 7 367 1345 bf 9 7 375 1345 bf 9 7 384 1345 bf 8 7 454 1345 bf 9 7 462 1345 bf 8 7
489 1345 bf 9 7 506 1345 bf 8 7 602 1345 bf 9 7 619 1345 bf 9 7 323 1352 bf 9 7 332 1352 bf 8 7 341 1352 bf 9 7 349 1352 bf 9 7 358 1352 bf 8 7 367 1352 bf 9 7 384 1352 bf 8 7 393 1352 bf 9 7 410 1352 bf 9 7 419 1352 bf 8 7 428 1352 bf 9 7 436 1352
bf 9 7 445 1352 bf 8 7 454 1352 bf 9 7 462 1352 bf 8 7 489 1352 bf 9 7 497 1352 bf 9 7 506 1352 bf 9 7 541 1352 bf 8 7 550 1352 bf 8 7 576 1352 bf 9 7 584 1352 bf 8 7 602 1352 bf 9 7 332 1359 bf 8 7 341 1359 bf 9 7 349 1359 bf 9 7 358 1359 bf 8 7
367 1359 bf 9 7 436 1359 bf 8 7 454 1359 bf 9 7 462 1359 bf 8 7 550 1359 bf 9 7 584 1359 bf 9 6 332 1366 bf 8 6 341 1366 bf 9 6 349 1366 bf 9 6 358 1366 bf 9 6 384 1366 bf 9 6 419 1366 bf 8 6 428 1366 bf 9 6 445 1366 bf 8 6 454 1366 bf 9 6 497 1366
bf 9 6 541 1366 bf 9 6 567 1366 bf 8 6 576 1366 bf 9 6 584 1366 bf 8 6 602 1366 bf 9 6 828 1366 bf 8 7 341 1372 bf 9 7 349 1372 bf 9 7 358 1372 bf 9 7 375 1372 bf 9 7 384 1372 bf 8 7 393 1372 bf 8 7 428 1372 bf 9 7 445 1372 bf 8 7 454 1372 bf 9 7
471 1372 bf 9 7 541 1372 bf 8 7 341 1379 bf 9 7 349 1379 bf 8 7 367 1379 bf 9 7 384 1379 bf 9 7 401 1379 bf 9 7 419 1379 bf 8 7 428 1379 bf 9 7 445 1379 bf 8 7 454 1379 bf 9 7 462 1379 bf 9 7 471 1379 bf 9 7 480 1379 bf 9 7 497 1379 bf 9 7 523 1379
bf 9 7 532 1379 bf 9 7 567 1379 bf 8 7 576 1379 bf 9 7 610 1379 bf 9 7 349 1386 bf 9 7 358 1386 bf 8 7 367 1386 bf 9 7 384 1386 bf 9 7 419 1386 bf 8 7 428 1386 bf 9 7 445 1386 bf 8 7 454 1386 bf 9 7 471 1386 bf 9 7 497 1386 bf 9 7 506 1386 bf 9 6
349 1393 bf 9 6 358 1393 bf 8 6 367 1393 bf 9 6 375 1393 bf 8 6 428 1393 bf 9 6 436 1393 bf 9 6 445 1393 bf 9 6 584 1393 bf 9 7 349 1399 bf 9 7 358 1399 bf 8 7 367 1399 bf 9 7 410 1399 bf 9 7 419 1399 bf 8 7 428 1399 bf 9 7 436 1399 bf 9 7 445 1399
bf 8 7 454 1399 bf 8 7 515 1399 bf 9 7 532 1399 bf 9 7 558 1399 bf 9 7 358 1406 bf 8 7 367 1406 bf 9 7 401 1406 bf 9 7 410 1406 bf 9 7 419 1406 bf 8 7 428 1406 bf 9 7 445 1406 bf 8 7 454 1406 bf 9 7 480 1406 bf 8 7 489 1406 bf 9 7 506 1406 bf 8 7
550 1406 bf 9 7 358 1413 bf 8 7 367 1413 bf 9 7 375 1413 bf 9 7 419 1413 bf 8 7 428 1413 bf 9 7 445 1413 bf 8 7 489 1413 bf 9 7 506 1413 bf 8 7 515 1413 bf 9 7 532 1413 bf 9 7 541 1413 bf 8 6 367 1420 bf 9 6 375 1420 bf 9 6 401 1420 bf 9 6 419 1420
bf 9 6 436 1420 bf 8 7 367 1426 bf 9 7 375 1426 bf 8 7 393 1426 bf 9 7 401 1426 bf 9 7 419 1426 bf 8 7 428 1426 bf 9 7 436 1426 bf 8 7 489 1426 bf 9 7 523 1426 bf 9 7 802 1426 bf 9 7 375 1433 bf 9 7 401 1433 bf 9 7 410 1433 bf 9 7 462 1433 bf 8 7
489 1433 bf 9 7 497 1433 bf 9 7 506 1433 bf 8 7 515 1433 bf 9 7 532 1433 bf 9 7 375 1440 bf 9 7 384 1440 bf 8 7 393 1440 bf 9 7 401 1440 bf 9 7 410 1440 bf 8 7 428 1440 bf 9 7 480 1440 bf 8 7 489 1440 bf 9 6 375 1447 bf 9 6 384 1447 bf 9 6 401 1447
bf 9 6 410 1447 bf 9 6 419 1447 bf 9 6 436 1447 bf 9 7 384 1453 bf 8 7 393 1453 bf 9 7 445 1453 bf 9 7 462 1453 bf 9 7 480 1453 bf 9 7 384 1460 bf 8 7 393 1460 bf 9 7 401 1460 bf 8 7 428 1460 bf 9 7 462 1460 bf 9 7 497 1460 bf 8 7 393 1467 bf 9 7
410 1467 bf 9 7 419 1467 bf 8 6 393 1474 bf 9 6 401 1474 bf 9 6 410 1474 bf 8 7 393 1480 bf 9 7 401 1480 bf 9 7 410 1480 bf 9 7 462 1480 bf 9 7 819 1480 bf 9 7 401 1487 bf 9 7 410 1487 bf 9 7 419 1487 bf 9 7 471 1487 bf 9 7 480 1487 bf 9 7 410 1494
bf 9 7 462 1494 bf 8 7 602 1494 bf 9 6 410 1501 bf 8 6 489 1501 bf 9 7 410 1507 bf 9 7 419 1507 bf 9 7 471 1507 bf 9 7 480 1507 bf 9 7 419 1514 bf 9 7 436 1514 bf 9 7 462 1514 bf 9 7 480 1514 bf 9 7 419 1521 bf 8 7 428 1521 bf 9 7 436 1521 bf 9 7
462 1521 bf 9 6 419 1528 bf 8 6 428 1528 bf 9 6 462 1528 bf 8 7 428 1534 bf 9 7 436 1534 bf 8 7 454 1534 bf 9 7 471 1534 bf 8 7 428 1541 bf 9 7 436 1541 bf 9 7 471 1541 bf 9 7 436 1548 bf 8 7 454 1548 bf 9 7 471 1548 bf 9 6 436 1555 bf 9 6 445 1555
bf 9 7 445 1561 bf 8 7 454 1561 bf 9 7 462 1561 bf 9 7 445 1568 bf 8 7 454 1568 bf 8 7 454 1575 bf 9 7 462 1575 bf 8 6 454 1582 bf 8 7 454 1588 bf 9 7 462 1588 bf 8 7 454 1595 bf 9 7 462 1595 bf 9 7 471 1595 bf 9 7 462 1602 bf 9 7 471 1602 bf 9 6
471 1609 bf 9 7 471 1622 bf 9 7 480 1622 bf 9 7 480 1629 bf 9 7 506 1629 bf 8 6 489 1636 bf 8 7 489 1642 bf 8 7 489 1649 bf 1 1 1 c black 132 981 m 870 X s
gsave 1088 844 23 896 C 569.206 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 1001 m -20 Y s 149 991 m -10 Y s 166 991 m -10 Y s 184 991 m -10 Y s 201 991 m -10 Y s 219 1001 m -20 Y s 236 991 m
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gsave 1088 844 23 896 C 790.058 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
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gsave 1088 844 1157 896 C 1703.06 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 1265 1001 m -20 Y s 1283 991 m -10 Y s 1300 991 m -10 Y s 1318 991 m -10 Y s 1335 991 m -10 Y s 1352 1001 m -20 Y s 1370
991 m -10 Y s 1387 991 m -10 Y s 1405 991 m -10 Y s 1422 991 m -10 Y s 1440 1001 m -20 Y s 1457 991 m -10 Y s 1474 991 m -10 Y s 1492 991 m -10 Y s 1509 991 m -10 Y s 1527 1001 m -20 Y s 1544 991 m -10 Y s 1561 991 m -10 Y s 1579 991 m -10 Y s 1596
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1001 m -20 Y s 2067 991 m -10 Y s 2084 991 m -10 Y s 2101 991 m -10 Y s 2119 991 m -10 Y s 2136 1001 m -20 Y s
gsave 1088 844 1157 896 C 1254.53 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 1157 896 C 1316 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 1157 896 C 1402.52 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 1157 896 C 1489.04 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 1157 896 C 1575.56 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 1157 896 C 1664.36 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 1157 896 C 1750.88 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 1157 896 C 1837.4 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 1157 896 C 1923.92 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 1157 896 C 2010.44 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 1157 896 C 2090.12 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 1265 1656 m 871 X s 1265 1636 m 20 Y s 1283 1646 m 10 Y s 1300 1646 m 10 Y s 1318 1646 m 10 Y s 1335 1646 m 10 Y s 1352 1636 m 20 Y s 1370
1646 m 10 Y s 1387 1646 m 10 Y s 1405 1646 m 10 Y s 1422 1646 m 10 Y s 1440 1636 m 20 Y s 1457 1646 m 10 Y s 1474 1646 m 10 Y s 1492 1646 m 10 Y s 1509 1646 m 10 Y s 1527 1636 m 20 Y s 1544 1646 m 10 Y s 1561 1646 m 10 Y s 1579 1646 m 10 Y s 1596
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gsave 1088 844 1157 896 C 1188.5 1400.25 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 1292 981 m -27 X s 1278 997 m -13 X s 1278 1013 m -13 X s 1278 1029 m -13 X s 1278 1045 m -13 X s 1292 1061 m -27 X s 1278 1077
m -13 X s 1278 1093 m -13 X s 1278 1109 m -13 X s 1278 1125 m -13 X s 1292 1142 m -27 X s 1278 1158 m -13 X s 1278 1174 m -13 X s 1278 1190 m -13 X s 1278 1206 m -13 X s 1292 1222 m -27 X s 1278 1238 m -13 X s 1278 1254 m -13 X s 1278 1270 m -13 X s
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gsave 1088 844 1157 896 C 1240.87 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 1157 896 C 1206.72 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 844 1157 896 C 1188.5 1129.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 1157 896 C 1188.5 1208.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 844 1157 896 C 1188.5 1288.68 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 1157 896 C 1188.5 1370.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 844 1157 896 C 1188.5 1450.34 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 1157 896 C 1188.5 1530.03 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
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gsave 1088 844 1157 896 C 2194.86 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 1157 896 C 2194.86 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5) show NC gr
gsave 1088 844 1157 896 C 2194.86 1124.75 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 844 1157 896 C 2194.86 1204.44 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (15) show NC gr
gsave 1088 844 1157 896 C 2194.86 1281.85 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (20) show NC gr
gsave 1088 844 1157 896 C 2194.86 1361.54 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (25) show NC gr
gsave 1088 844 1157 896 C 2194.86 1438.95 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (30) show NC gr
gsave 1088 844 1157 896 C 2194.86 1518.64 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (35) show NC gr
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gsave 1088 843 23 18 C 569.206 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 122 m -20 Y s 149 112 m -10 Y s 166 112 m -10 Y s 184 112 m -10 Y s 201 112 m -10 Y s 219 122 m -20 Y s 236 112 m -10 Y
s 253 112 m -10 Y s 271 112 m -10 Y s 288 112 m -10 Y s 306 122 m -20 Y s 323 112 m -10 Y s 341 112 m -10 Y s 358 112 m -10 Y s 375 112 m -10 Y s 393 122 m -20 Y s 410 112 m -10 Y s 428 112 m -10 Y s 445 112 m -10 Y s 462 112 m -10 Y s 480 122 m -20
Y s 497 112 m -10 Y s 515 112 m -10 Y s 532 112 m -10 Y s 550 112 m -10 Y s 567 122 m -20 Y s 584 112 m -10 Y s 602 112 m -10 Y s 619 112 m -10 Y s 637 112 m -10 Y s 654 122 m -20 Y s 671 112 m -10 Y s 689 112 m -10 Y s 706 112 m -10 Y s 724 112 m
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m -10 Y s 985 112 m -10 Y s 1002 122 m -20 Y s
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gsave 1088 843 23 18 C 182.146 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 23 18 C 268.665 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 23 18 C 355.185 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 23 18 C 441.704 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
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gsave 1088 843 23 18 C 617.019 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 843 23 18 C 703.539 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 843 23 18 C 790.058 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 843 23 18 C 876.577 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 843 23 18 C 956.266 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 777 m 870 X s 132 757 m 20 Y s 149 767 m 10 Y s 166 767 m 10 Y s 184 767 m 10 Y s 201 767 m 10 Y s 219 757 m 20 Y s 236 767 m 10 Y s 253
767 m 10 Y s 271 767 m 10 Y s 288 767 m 10 Y s 306 757 m 20 Y s 323 767 m 10 Y s 341 767 m 10 Y s 358 767 m 10 Y s 375 767 m 10 Y s 393 757 m 20 Y s 410 767 m 10 Y s 428 767 m 10 Y s 445 767 m 10 Y s 462 767 m 10 Y s 480 757 m 20 Y s 497 767 m 10 Y
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102 m 675 Y s
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214 m -13 X s 145 231 m -13 X s 145 247 m -13 X s 158 263 m -26 X s 145 279 m -13 X s 145 295 m -13 X s 145 311 m -13 X s 145 327 m -13 X s 158 343 m -26 X s 145 359 m -13 X s 145 375 m -13 X s 145 391 m -13 X s 145 407 m -13 X s 158 423 m -26 X s
145 439 m -13 X s 145 455 m -13 X s 145 472 m -13 X s 145 488 m -13 X s 158 504 m -26 X s 145 520 m -13 X s 145 536 m -13 X s 145 552 m -13 X s 145 568 m -13 X s 158 584 m -26 X s 145 600 m -13 X s 145 616 m -13 X s 145 632 m -13 X s 145 648 m -13 X
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gsave 1088 843 23 18 C 54.6438 330.139 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
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214 m 13 X s 989 231 m 13 X s 989 247 m 13 X s 976 263 m 26 X s 989 279 m 13 X s 989 295 m 13 X s 989 311 m 13 X s 989 327 m 13 X s 976 343 m 26 X s 989 359 m 13 X s 989 375 m 13 X s 989 391 m 13 X s 989 407 m 13 X s 976 423 m 26 X s 989 439 m 13 X
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13 X s 989 697 m 13 X s 989 713 m 13 X s 989 729 m 13 X s 976 745 m 26 X s 976 745 m 26 X s 989 761 m 13 X s 989 777 m 13 X s 0.386667 0 1 c 49 34 1008 102 bf 0.2 0 1 c 49 33 1008 136 bf 0 0.0800001 1 c 49 34 1008 169 bf 0 0.266667 1 c 49 34 1008
203 bf 0 0.546666 1 c 49 34 1008 237 bf 0 0.733333 1 c 49 33 1008 271 bf 0 1 0.986667 c 49 34 1008 304 bf 0 1 0.8 c 49 34 1008 338 bf 0 1 0.52 c 49 34 1008 372 bf 0 1 0.333333 c 49 33 1008 406 bf 0 1 0.0533333 c 49 34 1008 439 bf 0.133333 1 0 c 49
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gsave 1088 843 23 18 C 1061 161.654 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5) show NC gr
gsave 1088 843 23 18 C 1061 229.959 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 843 23 18 C 1061 300.541 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (15) show NC gr
gsave 1088 843 23 18 C 1061 371.122 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (20) show NC gr
gsave 1088 843 23 18 C 1061 441.704 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (25) show NC gr
gsave 1088 843 23 18 C 1061 512.285 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (30) show NC gr
gsave 1088 843 23 18 C 1061 580.59 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (35) show NC gr
gsave 1088 843 23 18 C 1061 651.172 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (40) show NC gr
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675 1265 102 bl 1 1 1 c 0 0.0800001 1 c 9 7 1265 102 bf 9 6 1265 109 bf 0.386667 0 1 c 9 6 1274 109 bf 8 6 1292 109 bf 9 6 1788 109 bf 8 6 2006 109 bf 0.2 0 1 c 9 7 1265 115 bf 0 0.546666 1 c 9 7 1274 115 bf 0.386667 0 1 c 9 7 2110 115 bf 0 1
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bf 0 0.266667 1 c 8 7 1318 210 bf 0.386667 0 1 c 9 7 1326 210 bf 9 7 1474 210 bf 9 7 1692 210 bf 8 7 1701 210 bf 9 7 1718 210 bf 8 7 1736 210 bf 9 7 1744 210 bf 9 7 1753 210 bf 0.2 0 1 c 8 7 1762 210 bf 0.386667 0 1 c 9 7 1770 210 bf 9 7 1779 210 bf
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1028 bf 9 7 166 1028 bf 9 7 175 1028 bf 8 7 184 1028 bf 9 7 192 1028 bf 9 7 210 1028 bf 8 7 219 1028 bf 9 7 227 1028 bf 9 7 236 1028 bf 8 7 245 1028 bf 9 7 262 1028 bf 9 7 271 1028 bf 8 7 367 1028 bf 9 7 375 1028 bf 9 7 384 1028 bf 8 7 550 1028 bf 8
7 576 1028 bf 9 7 828 1028 bf 9 7 863 1028 bf 9 7 898 1028 bf 9 7 967 1028 bf 8 7 994 1028 bf 8 7 158 1035 bf 9 7 166 1035 bf 9 7 192 1035 bf 9 7 201 1035 bf 9 7 227 1035 bf 8 7 341 1035 bf 9 7 358 1035 bf 9 7 384 1035 bf 8 7 393 1035 bf 9 7 401
1035 bf 9 7 628 1035 bf 9 7 828 1035 bf 8 6 158 1042 bf 9 6 166 1042 bf 9 6 175 1042 bf 8 6 184 1042 bf 9 6 192 1042 bf 9 6 201 1042 bf 8 6 219 1042 bf 8 6 245 1042 bf 9 6 253 1042 bf 9 6 271 1042 bf 8 6 280 1042 bf 9 6 297 1042 bf 8 6 306 1042 bf 9
6 314 1042 bf 9 6 323 1042 bf 9 6 332 1042 bf 9 6 349 1042 bf 8 6 515 1042 bf 9 6 941 1042 bf 9 7 166 1048 bf 8 7 184 1048 bf 9 7 253 1048 bf 9 7 262 1048 bf 9 7 271 1048 bf 8 7 280 1048 bf 9 7 288 1048 bf 8 7 306 1048 bf 9 7 323 1048 bf 8 7 341
1048 bf 9 7 541 1048 bf 8 7 698 1048 bf 8 7 846 1048 bf 8 7 933 1048 bf 9 7 941 1048 bf 9 7 985 1048 bf 8 7 994 1048 bf 9 7 166 1055 bf 9 7 175 1055 bf 9 7 210 1055 bf 8 7 245 1055 bf 9 7 253 1055 bf 9 7 262 1055 bf 9 7 271 1055 bf 9 7 297 1055 bf 8
7 306 1055 bf 9 7 323 1055 bf 9 7 332 1055 bf 8 7 785 1055 bf 9 7 837 1055 bf 8 7 872 1055 bf 9 7 880 1055 bf 9 7 889 1055 bf 9 7 898 1055 bf 9 7 915 1055 bf 9 7 941 1055 bf 9 7 950 1055 bf 8 7 959 1055 bf 9 7 967 1055 bf 9 7 976 1055 bf 9 7 985
1055 bf 8 7 994 1055 bf 9 7 166 1062 bf 9 7 175 1062 bf 9 7 192 1062 bf 9 7 227 1062 bf 8 7 245 1062 bf 9 7 253 1062 bf 9 7 262 1062 bf 8 7 280 1062 bf 9 7 297 1062 bf 8 7 306 1062 bf 9 7 314 1062 bf 8 7 393 1062 bf 8 7 428 1062 bf 8 7 602 1062 bf 9
7 706 1062 bf 9 7 793 1062 bf 8 7 811 1062 bf 9 7 828 1062 bf 8 7 872 1062 bf 9 7 880 1062 bf 9 7 889 1062 bf 9 7 898 1062 bf 8 7 907 1062 bf 9 7 915 1062 bf 9 7 924 1062 bf 8 7 933 1062 bf 9 7 941 1062 bf 9 7 950 1062 bf 8 7 959 1062 bf 9 7 967
1062 bf 9 7 976 1062 bf 9 7 985 1062 bf 8 7 994 1062 bf 9 6 175 1069 bf 8 6 184 1069 bf 9 6 192 1069 bf 8 6 245 1069 bf 9 6 253 1069 bf 9 6 271 1069 bf 9 6 288 1069 bf 8 6 306 1069 bf 9 6 384 1069 bf 9 6 715 1069 bf 9 6 741 1069 bf 9 6 776 1069 bf 9
6 837 1069 bf 9 6 854 1069 bf 9 6 863 1069 bf 8 6 872 1069 bf 9 6 880 1069 bf 9 6 889 1069 bf 9 6 898 1069 bf 8 6 907 1069 bf 9 6 915 1069 bf 9 6 924 1069 bf 8 6 933 1069 bf 9 6 941 1069 bf 9 6 950 1069 bf 8 6 959 1069 bf 9 6 967 1069 bf 9 6 976
1069 bf 9 6 985 1069 bf 8 6 994 1069 bf 9 7 175 1075 bf 8 7 184 1075 bf 8 7 245 1075 bf 9 7 262 1075 bf 9 7 271 1075 bf 9 7 323 1075 bf 9 7 567 1075 bf 8 7 759 1075 bf 9 7 767 1075 bf 9 7 776 1075 bf 9 7 793 1075 bf 9 7 802 1075 bf 8 7 811 1075 bf 9
7 819 1075 bf 9 7 828 1075 bf 9 7 837 1075 bf 8 7 846 1075 bf 9 7 854 1075 bf 9 7 863 1075 bf 8 7 872 1075 bf 9 7 880 1075 bf 9 7 889 1075 bf 9 7 898 1075 bf 8 7 907 1075 bf 9 7 915 1075 bf 9 7 924 1075 bf 8 7 933 1075 bf 9 7 941 1075 bf 9 7 950
1075 bf 8 7 959 1075 bf 9 7 967 1075 bf 9 7 976 1075 bf 9 7 985 1075 bf 8 7 994 1075 bf 8 7 184 1082 bf 9 7 192 1082 bf 9 7 236 1082 bf 9 7 253 1082 bf 9 7 262 1082 bf 8 7 280 1082 bf 8 7 306 1082 bf 9 7 332 1082 bf 9 7 349 1082 bf 8 7 367 1082 bf 8
7 393 1082 bf 9 7 567 1082 bf 9 7 689 1082 bf 8 7 698 1082 bf 9 7 715 1082 bf 8 7 724 1082 bf 9 7 732 1082 bf 9 7 741 1082 bf 9 7 750 1082 bf 8 7 759 1082 bf 9 7 767 1082 bf 9 7 776 1082 bf 8 7 785 1082 bf 9 7 793 1082 bf 9 7 802 1082 bf 8 7 811
1082 bf 9 7 819 1082 bf 9 7 828 1082 bf 9 7 837 1082 bf 8 7 846 1082 bf 9 7 854 1082 bf 9 7 863 1082 bf 8 7 872 1082 bf 9 7 880 1082 bf 9 7 889 1082 bf 9 7 898 1082 bf 8 7 907 1082 bf 9 7 915 1082 bf 9 7 924 1082 bf 8 7 933 1082 bf 9 7 941 1082 bf 9
7 950 1082 bf 8 7 959 1082 bf 9 7 976 1082 bf 9 7 985 1082 bf 8 7 994 1082 bf 8 7 184 1089 bf 9 7 192 1089 bf 9 7 227 1089 bf 8 7 245 1089 bf 9 7 271 1089 bf 9 7 297 1089 bf 9 7 349 1089 bf 9 7 523 1089 bf 9 7 628 1089 bf 9 7 689 1089 bf 8 7 698
1089 bf 9 7 706 1089 bf 9 7 715 1089 bf 8 7 724 1089 bf 9 7 732 1089 bf 9 7 741 1089 bf 9 7 750 1089 bf 8 7 759 1089 bf 9 7 767 1089 bf 9 7 776 1089 bf 8 7 785 1089 bf 9 7 793 1089 bf 9 7 802 1089 bf 8 7 811 1089 bf 9 7 819 1089 bf 9 7 828 1089 bf 9
7 837 1089 bf 8 7 846 1089 bf 9 7 854 1089 bf 9 7 863 1089 bf 8 7 872 1089 bf 9 7 880 1089 bf 9 7 889 1089 bf 9 7 898 1089 bf 8 7 907 1089 bf 9 7 915 1089 bf 8 7 933 1089 bf 9 7 941 1089 bf 9 7 950 1089 bf 8 7 959 1089 bf 9 7 976 1089 bf 9 7 985
1089 bf 8 6 184 1096 bf 9 6 192 1096 bf 9 6 201 1096 bf 9 6 227 1096 bf 9 6 236 1096 bf 8 6 245 1096 bf 8 6 280 1096 bf 9 6 332 1096 bf 8 6 393 1096 bf 9 6 645 1096 bf 9 6 654 1096 bf 8 6 663 1096 bf 9 6 671 1096 bf 9 6 680 1096 bf 9 6 689 1096 bf 8
6 698 1096 bf 9 6 706 1096 bf 9 6 715 1096 bf 8 6 724 1096 bf 9 6 732 1096 bf 9 6 741 1096 bf 9 6 750 1096 bf 8 6 759 1096 bf 9 6 767 1096 bf 9 6 776 1096 bf 8 6 785 1096 bf 9 6 793 1096 bf 9 6 802 1096 bf 8 6 811 1096 bf 9 6 819 1096 bf 9 6 828
1096 bf 9 6 837 1096 bf 8 6 846 1096 bf 9 6 854 1096 bf 9 6 863 1096 bf 8 6 872 1096 bf 9 6 880 1096 bf 9 6 889 1096 bf 9 6 898 1096 bf 8 6 907 1096 bf 9 6 915 1096 bf 9 6 924 1096 bf 9 6 941 1096 bf 8 6 959 1096 bf 9 7 192 1102 bf 9 7 201 1102 bf 9
7 227 1102 bf 8 7 341 1102 bf 9 7 462 1102 bf 8 7 576 1102 bf 9 7 584 1102 bf 8 7 602 1102 bf 9 7 619 1102 bf 9 7 628 1102 bf 8 7 637 1102 bf 9 7 645 1102 bf 9 7 654 1102 bf 8 7 663 1102 bf 9 7 671 1102 bf 9 7 680 1102 bf 9 7 689 1102 bf 8 7 698
1102 bf 9 7 706 1102 bf 9 7 715 1102 bf 8 7 724 1102 bf 9 7 732 1102 bf 9 7 741 1102 bf 9 7 750 1102 bf 8 7 759 1102 bf 9 7 767 1102 bf 9 7 776 1102 bf 8 7 785 1102 bf 9 7 793 1102 bf 9 7 802 1102 bf 8 7 811 1102 bf 9 7 819 1102 bf 9 7 828 1102 bf 9
7 854 1102 bf 9 7 863 1102 bf 9 7 898 1102 bf 9 7 985 1102 bf 9 7 192 1109 bf 9 7 201 1109 bf 8 7 219 1109 bf 9 7 262 1109 bf 9 7 332 1109 bf 9 7 410 1109 bf 9 7 567 1109 bf 9 7 584 1109 bf 9 7 593 1109 bf 8 7 602 1109 bf 9 7 610 1109 bf 9 7 619
1109 bf 9 7 628 1109 bf 8 7 637 1109 bf 9 7 645 1109 bf 9 7 654 1109 bf 8 7 663 1109 bf 9 7 671 1109 bf 9 7 680 1109 bf 9 7 689 1109 bf 8 7 698 1109 bf 9 7 706 1109 bf 9 7 715 1109 bf 8 7 724 1109 bf 9 7 732 1109 bf 9 7 741 1109 bf 9 7 750 1109 bf 8
7 759 1109 bf 9 7 767 1109 bf 9 7 776 1109 bf 9 7 793 1109 bf 9 7 802 1109 bf 9 7 819 1109 bf 9 7 837 1109 bf 9 7 889 1109 bf 9 7 201 1116 bf 9 7 210 1116 bf 9 7 253 1116 bf 9 7 314 1116 bf 9 7 401 1116 bf 8 7 550 1116 bf 9 7 567 1116 bf 8 7 576
1116 bf 9 7 584 1116 bf 9 7 593 1116 bf 8 7 602 1116 bf 9 7 610 1116 bf 9 7 619 1116 bf 9 7 628 1116 bf 8 7 637 1116 bf 9 7 645 1116 bf 9 7 654 1116 bf 8 7 663 1116 bf 9 7 671 1116 bf 9 7 680 1116 bf 9 7 689 1116 bf 8 7 698 1116 bf 9 7 706 1116 bf 9
7 715 1116 bf 8 7 724 1116 bf 9 7 732 1116 bf 9 7 741 1116 bf 9 7 750 1116 bf 8 7 759 1116 bf 9 7 767 1116 bf 9 7 776 1116 bf 9 7 793 1116 bf 9 7 802 1116 bf 8 7 811 1116 bf 9 7 819 1116 bf 9 7 828 1116 bf 9 7 837 1116 bf 9 7 985 1116 bf 9 6 201
1123 bf 9 6 210 1123 bf 8 6 219 1123 bf 9 6 227 1123 bf 9 6 253 1123 bf 8 6 280 1123 bf 9 6 288 1123 bf 9 6 532 1123 bf 8 6 550 1123 bf 9 6 558 1123 bf 9 6 567 1123 bf 8 6 576 1123 bf 9 6 584 1123 bf 9 6 593 1123 bf 8 6 602 1123 bf 9 6 610 1123 bf 9
6 619 1123 bf 9 6 628 1123 bf 8 6 637 1123 bf 9 6 645 1123 bf 9 6 654 1123 bf 8 6 663 1123 bf 9 6 671 1123 bf 9 6 680 1123 bf 9 6 689 1123 bf 8 6 698 1123 bf 9 6 706 1123 bf 8 6 724 1123 bf 9 6 732 1123 bf 9 6 741 1123 bf 9 6 750 1123 bf 8 6 785
1123 bf 8 6 907 1123 bf 8 6 933 1123 bf 9 6 967 1123 bf 9 6 976 1123 bf 9 6 985 1123 bf 8 6 994 1123 bf 9 7 210 1129 bf 9 7 227 1129 bf 8 7 245 1129 bf 9 7 253 1129 bf 9 7 323 1129 bf 9 7 523 1129 bf 9 7 532 1129 bf 8 7 550 1129 bf 9 7 558 1129 bf 9
7 567 1129 bf 8 7 576 1129 bf 9 7 584 1129 bf 9 7 593 1129 bf 8 7 602 1129 bf 9 7 610 1129 bf 9 7 619 1129 bf 9 7 628 1129 bf 8 7 637 1129 bf 9 7 645 1129 bf 9 7 654 1129 bf 8 7 663 1129 bf 9 7 671 1129 bf 9 7 680 1129 bf 9 7 689 1129 bf 9 7 715
1129 bf 9 7 741 1129 bf 8 7 846 1129 bf 9 7 889 1129 bf 9 7 898 1129 bf 9 7 915 1129 bf 9 7 924 1129 bf 9 7 950 1129 bf 8 7 959 1129 bf 9 7 967 1129 bf 9 7 985 1129 bf 8 7 994 1129 bf 9 7 210 1136 bf 8 7 219 1136 bf 9 7 297 1136 bf 8 7 489 1136 bf 9
7 506 1136 bf 8 7 515 1136 bf 9 7 523 1136 bf 9 7 532 1136 bf 9 7 541 1136 bf 8 7 550 1136 bf 9 7 558 1136 bf 9 7 567 1136 bf 8 7 576 1136 bf 9 7 584 1136 bf 9 7 593 1136 bf 8 7 602 1136 bf 9 7 610 1136 bf 9 7 619 1136 bf 9 7 628 1136 bf 8 7 637
1136 bf 9 7 645 1136 bf 9 7 654 1136 bf 8 7 663 1136 bf 9 7 671 1136 bf 9 7 680 1136 bf 9 7 689 1136 bf 9 7 706 1136 bf 9 7 715 1136 bf 9 7 750 1136 bf 9 7 767 1136 bf 9 7 828 1136 bf 9 7 854 1136 bf 9 7 863 1136 bf 9 7 889 1136 bf 9 7 898 1136 bf 9
7 915 1136 bf 9 7 924 1136 bf 9 7 941 1136 bf 9 7 950 1136 bf 9 7 967 1136 bf 9 7 976 1136 bf 9 7 985 1136 bf 9 7 210 1143 bf 8 7 219 1143 bf 9 7 236 1143 bf 9 7 349 1143 bf 8 7 454 1143 bf 9 7 480 1143 bf 8 7 489 1143 bf 9 7 497 1143 bf 9 7 506
1143 bf 8 7 515 1143 bf 9 7 523 1143 bf 9 7 532 1143 bf 9 7 541 1143 bf 8 7 550 1143 bf 9 7 558 1143 bf 9 7 567 1143 bf 8 7 576 1143 bf 9 7 584 1143 bf 9 7 593 1143 bf 8 7 602 1143 bf 9 7 610 1143 bf 9 7 619 1143 bf 9 7 628 1143 bf 9 7 645 1143 bf 9
7 654 1143 bf 8 7 698 1143 bf 9 7 802 1143 bf 9 7 828 1143 bf 9 7 854 1143 bf 9 7 863 1143 bf 8 7 872 1143 bf 9 7 880 1143 bf 9 7 898 1143 bf 8 7 907 1143 bf 9 7 915 1143 bf 8 7 933 1143 bf 9 7 950 1143 bf 8 7 994 1143 bf 8 6 219 1150 bf 9 6 227
1150 bf 8 6 245 1150 bf 9 6 471 1150 bf 9 6 480 1150 bf 8 6 489 1150 bf 9 6 497 1150 bf 9 6 506 1150 bf 8 6 515 1150 bf 9 6 523 1150 bf 9 6 532 1150 bf 9 6 541 1150 bf 8 6 550 1150 bf 9 6 558 1150 bf 9 6 567 1150 bf 8 6 576 1150 bf 9 6 584 1150 bf 9
6 593 1150 bf 8 6 602 1150 bf 9 6 610 1150 bf 9 6 619 1150 bf 9 6 628 1150 bf 8 6 637 1150 bf 9 6 654 1150 bf 9 6 689 1150 bf 9 6 767 1150 bf 8 6 785 1150 bf 9 6 819 1150 bf 9 6 828 1150 bf 9 6 837 1150 bf 8 6 846 1150 bf 9 6 854 1150 bf 9 6 863
1150 bf 8 6 872 1150 bf 9 6 880 1150 bf 9 6 889 1150 bf 9 6 898 1150 bf 9 6 915 1150 bf 9 6 924 1150 bf 8 6 933 1150 bf 8 6 959 1150 bf 9 6 967 1150 bf 8 7 219 1156 bf 9 7 227 1156 bf 9 7 262 1156 bf 9 7 462 1156 bf 9 7 471 1156 bf 9 7 480 1156 bf 8
7 489 1156 bf 9 7 497 1156 bf 9 7 506 1156 bf 8 7 515 1156 bf 9 7 523 1156 bf 9 7 532 1156 bf 9 7 541 1156 bf 8 7 550 1156 bf 9 7 558 1156 bf 9 7 567 1156 bf 8 7 576 1156 bf 9 7 584 1156 bf 9 7 593 1156 bf 8 7 602 1156 bf 9 7 610 1156 bf 9 7 619
1156 bf 9 7 645 1156 bf 8 7 663 1156 bf 9 7 671 1156 bf 9 7 741 1156 bf 9 7 750 1156 bf 9 7 776 1156 bf 8 7 785 1156 bf 9 7 802 1156 bf 8 7 811 1156 bf 9 7 819 1156 bf 9 7 828 1156 bf 9 7 837 1156 bf 9 7 854 1156 bf 8 7 872 1156 bf 9 7 880 1156 bf 9
7 889 1156 bf 9 7 898 1156 bf 8 7 933 1156 bf 9 7 967 1156 bf 9 7 227 1163 bf 9 7 253 1163 bf 8 7 454 1163 bf 9 7 462 1163 bf 9 7 471 1163 bf 9 7 480 1163 bf 8 7 489 1163 bf 9 7 497 1163 bf 9 7 506 1163 bf 8 7 515 1163 bf 9 7 523 1163 bf 9 7 532
1163 bf 9 7 541 1163 bf 8 7 550 1163 bf 9 7 558 1163 bf 9 7 567 1163 bf 8 7 576 1163 bf 9 7 593 1163 bf 8 7 637 1163 bf 9 7 654 1163 bf 8 7 663 1163 bf 9 7 689 1163 bf 9 7 732 1163 bf 9 7 750 1163 bf 8 7 759 1163 bf 9 7 767 1163 bf 8 7 785 1163 bf 9
7 793 1163 bf 9 7 802 1163 bf 8 7 811 1163 bf 9 7 819 1163 bf 9 7 828 1163 bf 9 7 837 1163 bf 8 7 846 1163 bf 9 7 854 1163 bf 8 7 872 1163 bf 9 7 880 1163 bf 8 7 907 1163 bf 9 7 227 1170 bf 9 7 236 1170 bf 9 7 436 1170 bf 9 7 445 1170 bf 8 7 454
1170 bf 9 7 462 1170 bf 9 7 471 1170 bf 9 7 480 1170 bf 8 7 489 1170 bf 9 7 497 1170 bf 9 7 506 1170 bf 8 7 515 1170 bf 9 7 523 1170 bf 9 7 532 1170 bf 9 7 541 1170 bf 8 7 550 1170 bf 8 7 576 1170 bf 9 7 584 1170 bf 9 7 610 1170 bf 8 7 637 1170 bf 9
7 645 1170 bf 9 7 689 1170 bf 8 7 698 1170 bf 9 7 715 1170 bf 8 7 724 1170 bf 9 7 732 1170 bf 9 7 741 1170 bf 9 7 750 1170 bf 8 7 759 1170 bf 9 7 767 1170 bf 9 7 776 1170 bf 8 7 785 1170 bf 9 7 793 1170 bf 9 7 819 1170 bf 9 7 828 1170 bf 8 7 846
1170 bf 8 7 994 1170 bf 9 6 227 1177 bf 9 6 236 1177 bf 9 6 419 1177 bf 8 6 428 1177 bf 9 6 436 1177 bf 9 6 445 1177 bf 8 6 454 1177 bf 9 6 462 1177 bf 9 6 471 1177 bf 9 6 480 1177 bf 8 6 489 1177 bf 9 6 497 1177 bf 9 6 506 1177 bf 8 6 515 1177 bf 9
6 523 1177 bf 9 6 532 1177 bf 9 6 541 1177 bf 8 6 550 1177 bf 9 6 567 1177 bf 9 6 593 1177 bf 9 6 680 1177 bf 8 6 698 1177 bf 9 6 706 1177 bf 9 6 715 1177 bf 8 6 724 1177 bf 9 6 732 1177 bf 9 6 741 1177 bf 9 6 750 1177 bf 8 6 759 1177 bf 9 6 767
1177 bf 9 6 776 1177 bf 8 6 785 1177 bf 9 6 793 1177 bf 9 6 802 1177 bf 8 6 811 1177 bf 9 6 950 1177 bf 8 6 959 1177 bf 9 7 236 1183 bf 8 7 245 1183 bf 9 7 419 1183 bf 8 7 428 1183 bf 9 7 436 1183 bf 9 7 445 1183 bf 8 7 454 1183 bf 9 7 462 1183 bf 9
7 471 1183 bf 9 7 480 1183 bf 8 7 489 1183 bf 9 7 497 1183 bf 9 7 506 1183 bf 8 7 515 1183 bf 9 7 523 1183 bf 9 7 532 1183 bf 8 7 550 1183 bf 8 7 637 1183 bf 9 7 689 1183 bf 8 7 698 1183 bf 9 7 706 1183 bf 9 7 715 1183 bf 8 7 724 1183 bf 9 7 732
1183 bf 9 7 741 1183 bf 9 7 750 1183 bf 9 7 767 1183 bf 9 7 802 1183 bf 8 7 811 1183 bf 9 7 828 1183 bf 9 7 915 1183 bf 9 7 941 1183 bf 9 7 950 1183 bf 9 7 976 1183 bf 9 7 985 1183 bf 8 7 994 1183 bf 9 7 236 1190 bf 8 7 245 1190 bf 9 7 410 1190 bf 9
7 419 1190 bf 8 7 428 1190 bf 9 7 436 1190 bf 9 7 445 1190 bf 8 7 454 1190 bf 9 7 462 1190 bf 9 7 471 1190 bf 9 7 480 1190 bf 8 7 489 1190 bf 9 7 497 1190 bf 9 7 506 1190 bf 8 7 515 1190 bf 9 7 523 1190 bf 9 7 532 1190 bf 9 7 558 1190 bf 8 7 576
1190 bf 8 7 637 1190 bf 8 7 663 1190 bf 9 7 671 1190 bf 9 7 680 1190 bf 9 7 689 1190 bf 8 7 698 1190 bf 9 7 706 1190 bf 9 7 715 1190 bf 8 7 724 1190 bf 9 7 732 1190 bf 9 7 750 1190 bf 8 7 759 1190 bf 9 7 767 1190 bf 9 7 776 1190 bf 9 7 793 1190 bf 9
7 915 1190 bf 9 7 941 1190 bf 9 7 985 1190 bf 8 7 245 1197 bf 9 7 401 1197 bf 9 7 410 1197 bf 9 7 419 1197 bf 8 7 428 1197 bf 9 7 436 1197 bf 9 7 445 1197 bf 8 7 454 1197 bf 9 7 462 1197 bf 9 7 471 1197 bf 9 7 480 1197 bf 8 7 489 1197 bf 9 7 497
1197 bf 9 7 506 1197 bf 9 7 523 1197 bf 9 7 558 1197 bf 9 7 628 1197 bf 8 7 637 1197 bf 9 7 645 1197 bf 9 7 654 1197 bf 8 7 663 1197 bf 9 7 671 1197 bf 9 7 680 1197 bf 9 7 689 1197 bf 8 7 698 1197 bf 9 7 706 1197 bf 9 7 715 1197 bf 9 7 732 1197 bf 9
7 750 1197 bf 9 7 837 1197 bf 8 7 907 1197 bf 9 7 915 1197 bf 8 7 933 1197 bf 8 6 245 1204 bf 9 6 253 1204 bf 8 6 393 1204 bf 9 6 401 1204 bf 9 6 410 1204 bf 9 6 419 1204 bf 8 6 428 1204 bf 9 6 436 1204 bf 9 6 445 1204 bf 8 6 454 1204 bf 9 6 462
1204 bf 9 6 480 1204 bf 8 6 489 1204 bf 9 6 497 1204 bf 9 6 506 1204 bf 9 6 610 1204 bf 9 6 619 1204 bf 9 6 628 1204 bf 8 6 637 1204 bf 9 6 645 1204 bf 9 6 654 1204 bf 8 6 663 1204 bf 9 6 671 1204 bf 9 6 689 1204 bf 8 6 698 1204 bf 9 6 863 1204 bf 8
6 872 1204 bf 9 6 889 1204 bf 8 6 907 1204 bf 9 6 924 1204 bf 9 6 950 1204 bf 8 6 959 1204 bf 8 7 245 1210 bf 9 7 253 1210 bf 8 7 393 1210 bf 9 7 401 1210 bf 9 7 410 1210 bf 9 7 419 1210 bf 8 7 428 1210 bf 9 7 436 1210 bf 9 7 445 1210 bf 8 7 454
1210 bf 9 7 462 1210 bf 9 7 480 1210 bf 8 7 489 1210 bf 8 7 515 1210 bf 9 7 593 1210 bf 8 7 602 1210 bf 9 7 610 1210 bf 9 7 619 1210 bf 9 7 628 1210 bf 8 7 637 1210 bf 9 7 645 1210 bf 9 7 654 1210 bf 8 7 663 1210 bf 9 7 671 1210 bf 9 7 680 1210 bf 9
7 689 1210 bf 9 7 715 1210 bf 9 7 741 1210 bf 9 7 828 1210 bf 8 7 846 1210 bf 9 7 854 1210 bf 9 7 863 1210 bf 8 7 907 1210 bf 9 7 924 1210 bf 9 7 253 1217 bf 9 7 262 1217 bf 9 7 384 1217 bf 8 7 393 1217 bf 9 7 401 1217 bf 9 7 410 1217 bf 9 7 419
1217 bf 8 7 428 1217 bf 9 7 445 1217 bf 8 7 454 1217 bf 9 7 462 1217 bf 9 7 480 1217 bf 9 7 497 1217 bf 8 7 515 1217 bf 9 7 584 1217 bf 9 7 593 1217 bf 8 7 602 1217 bf 9 7 610 1217 bf 9 7 619 1217 bf 9 7 628 1217 bf 8 7 637 1217 bf 9 7 645 1217 bf 9
7 654 1217 bf 8 7 663 1217 bf 9 7 671 1217 bf 9 7 689 1217 bf 9 7 776 1217 bf 9 7 802 1217 bf 9 7 828 1217 bf 9 7 889 1217 bf 9 7 253 1224 bf 9 7 262 1224 bf 9 7 384 1224 bf 8 7 393 1224 bf 9 7 401 1224 bf 9 7 410 1224 bf 9 7 419 1224 bf 9 7 436
1224 bf 9 7 445 1224 bf 8 7 454 1224 bf 9 7 462 1224 bf 9 7 480 1224 bf 9 7 506 1224 bf 9 7 593 1224 bf 8 7 602 1224 bf 9 7 610 1224 bf 9 7 619 1224 bf 9 7 628 1224 bf 8 7 637 1224 bf 9 7 645 1224 bf 9 7 654 1224 bf 8 7 663 1224 bf 9 7 715 1224 bf 9
7 767 1224 bf 8 7 785 1224 bf 9 7 793 1224 bf 9 7 819 1224 bf 9 7 863 1224 bf 9 6 262 1231 bf 9 6 271 1231 bf 9 6 375 1231 bf 9 6 384 1231 bf 8 6 393 1231 bf 9 6 401 1231 bf 9 6 410 1231 bf 9 6 419 1231 bf 9 6 445 1231 bf 8 6 454 1231 bf 9 6 471
1231 bf 9 6 480 1231 bf 9 6 497 1231 bf 8 6 576 1231 bf 9 6 584 1231 bf 9 6 593 1231 bf 8 6 602 1231 bf 9 6 610 1231 bf 9 6 619 1231 bf 9 6 628 1231 bf 8 6 637 1231 bf 9 6 767 1231 bf 9 6 802 1231 bf 8 6 811 1231 bf 8 6 846 1231 bf 9 7 262 1237 bf 9
7 271 1237 bf 8 7 367 1237 bf 9 7 375 1237 bf 9 7 384 1237 bf 8 7 393 1237 bf 9 7 401 1237 bf 9 7 410 1237 bf 9 7 419 1237 bf 9 7 436 1237 bf 9 7 445 1237 bf 9 7 462 1237 bf 9 7 471 1237 bf 8 7 489 1237 bf 9 7 532 1237 bf 9 7 558 1237 bf 9 7 567
1237 bf 8 7 576 1237 bf 9 7 584 1237 bf 9 7 593 1237 bf 8 7 602 1237 bf 9 7 610 1237 bf 9 7 628 1237 bf 9 7 671 1237 bf 9 7 715 1237 bf 8 7 724 1237 bf 9 7 741 1237 bf 9 7 776 1237 bf 8 7 785 1237 bf 9 7 793 1237 bf 9 7 802 1237 bf 9 7 819 1237 bf 9
7 828 1237 bf 9 7 271 1244 bf 9 7 297 1244 bf 8 7 367 1244 bf 9 7 375 1244 bf 9 7 384 1244 bf 8 7 393 1244 bf 9 7 401 1244 bf 9 7 410 1244 bf 9 7 419 1244 bf 8 7 428 1244 bf 9 7 436 1244 bf 8 7 454 1244 bf 9 7 471 1244 bf 8 7 489 1244 bf 9 7 523
1244 bf 8 7 550 1244 bf 9 7 558 1244 bf 9 7 567 1244 bf 8 7 576 1244 bf 9 7 584 1244 bf 9 7 593 1244 bf 9 7 610 1244 bf 9 7 619 1244 bf 9 7 645 1244 bf 8 7 698 1244 bf 8 7 724 1244 bf 9 7 732 1244 bf 9 7 741 1244 bf 8 7 759 1244 bf 9 7 767 1244 bf 8
7 785 1244 bf 9 7 793 1244 bf 9 7 802 1244 bf 9 7 271 1251 bf 8 7 280 1251 bf 9 7 358 1251 bf 8 7 367 1251 bf 9 7 375 1251 bf 9 7 384 1251 bf 8 7 393 1251 bf 9 7 401 1251 bf 9 7 410 1251 bf 9 7 419 1251 bf 9 7 436 1251 bf 9 7 532 1251 bf 9 7 541
1251 bf 8 7 550 1251 bf 9 7 558 1251 bf 9 7 567 1251 bf 8 7 576 1251 bf 9 7 584 1251 bf 8 7 602 1251 bf 8 7 698 1251 bf 9 7 706 1251 bf 9 7 715 1251 bf 8 7 724 1251 bf 9 7 732 1251 bf 9 7 750 1251 bf 9 7 767 1251 bf 8 7 785 1251 bf 8 6 280 1258 bf 8
6 367 1258 bf 9 6 375 1258 bf 9 6 384 1258 bf 8 6 393 1258 bf 9 6 401 1258 bf 9 6 410 1258 bf 8 6 428 1258 bf 8 6 454 1258 bf 9 6 523 1258 bf 9 6 532 1258 bf 9 6 541 1258 bf 8 6 550 1258 bf 9 6 567 1258 bf 8 6 576 1258 bf 9 6 584 1258 bf 9 6 628
1258 bf 9 6 680 1258 bf 9 6 689 1258 bf 8 6 698 1258 bf 9 6 732 1258 bf 9 6 741 1258 bf 8 7 280 1264 bf 9 7 288 1264 bf 9 7 358 1264 bf 8 7 367 1264 bf 9 7 375 1264 bf 9 7 384 1264 bf 8 7 393 1264 bf 9 7 401 1264 bf 9 7 419 1264 bf 8 7 428 1264 bf 9
7 436 1264 bf 9 7 445 1264 bf 9 7 480 1264 bf 8 7 489 1264 bf 8 7 515 1264 bf 9 7 523 1264 bf 9 7 532 1264 bf 9 7 558 1264 bf 9 7 567 1264 bf 9 7 584 1264 bf 9 7 689 1264 bf 8 7 698 1264 bf 9 7 706 1264 bf 9 7 715 1264 bf 8 7 724 1264 bf 9 7 741
1264 bf 8 7 759 1264 bf 8 7 280 1271 bf 9 7 288 1271 bf 8 7 306 1271 bf 9 7 358 1271 bf 8 7 367 1271 bf 9 7 375 1271 bf 9 7 384 1271 bf 8 7 393 1271 bf 9 7 410 1271 bf 9 7 419 1271 bf 8 7 428 1271 bf 9 7 471 1271 bf 9 7 497 1271 bf 9 7 506 1271 bf 8
7 515 1271 bf 9 7 523 1271 bf 9 7 532 1271 bf 9 7 541 1271 bf 8 7 550 1271 bf 9 7 584 1271 bf 9 7 654 1271 bf 8 7 663 1271 bf 9 7 671 1271 bf 9 7 680 1271 bf 9 7 689 1271 bf 8 7 698 1271 bf 9 7 715 1271 bf 8 7 724 1271 bf 9 7 741 1271 bf 9 7 288
1278 bf 9 7 297 1278 bf 9 7 349 1278 bf 9 7 358 1278 bf 8 7 367 1278 bf 9 7 375 1278 bf 8 7 393 1278 bf 9 7 401 1278 bf 8 7 428 1278 bf 9 7 506 1278 bf 8 7 515 1278 bf 9 7 532 1278 bf 9 7 541 1278 bf 9 7 567 1278 bf 9 7 654 1278 bf 8 7 663 1278 bf 9
7 671 1278 bf 9 7 689 1278 bf 8 7 698 1278 bf 9 7 706 1278 bf 9 7 750 1278 bf 9 6 288 1285 bf 9 6 297 1285 bf 9 6 349 1285 bf 9 6 358 1285 bf 8 6 367 1285 bf 9 6 375 1285 bf 9 6 384 1285 bf 8 6 393 1285 bf 9 6 410 1285 bf 9 6 419 1285 bf 9 6 497
1285 bf 9 6 506 1285 bf 8 6 515 1285 bf 9 6 523 1285 bf 9 6 541 1285 bf 9 6 558 1285 bf 9 6 654 1285 bf 9 6 680 1285 bf 8 6 698 1285 bf 9 7 297 1291 bf 9 7 349 1291 bf 9 7 358 1291 bf 8 7 367 1291 bf 9 7 375 1291 bf 9 7 384 1291 bf 8 7 393 1291 bf 9
7 401 1291 bf 9 7 410 1291 bf 8 7 428 1291 bf 9 7 480 1291 bf 8 7 489 1291 bf 9 7 497 1291 bf 9 7 506 1291 bf 8 7 515 1291 bf 9 7 523 1291 bf 9 7 532 1291 bf 9 7 654 1291 bf 9 7 671 1291 bf 9 7 706 1291 bf 9 7 297 1298 bf 8 7 306 1298 bf 9 7 349
1298 bf 9 7 358 1298 bf 8 7 367 1298 bf 9 7 375 1298 bf 9 7 384 1298 bf 8 7 393 1298 bf 9 7 401 1298 bf 9 7 480 1298 bf 8 7 489 1298 bf 9 7 506 1298 bf 9 7 523 1298 bf 8 7 602 1298 bf 9 7 610 1298 bf 9 7 619 1298 bf 9 7 628 1298 bf 8 7 637 1298 bf 9
7 645 1298 bf 8 7 663 1298 bf 9 7 297 1305 bf 8 7 306 1305 bf 8 7 341 1305 bf 9 7 349 1305 bf 9 7 358 1305 bf 8 7 367 1305 bf 9 7 375 1305 bf 9 7 384 1305 bf 8 7 393 1305 bf 9 7 401 1305 bf 8 7 454 1305 bf 9 7 471 1305 bf 9 7 480 1305 bf 8 7 489
1305 bf 9 7 497 1305 bf 9 7 506 1305 bf 9 7 541 1305 bf 8 7 550 1305 bf 8 7 602 1305 bf 9 7 619 1305 bf 9 7 628 1305 bf 9 7 645 1305 bf 8 6 306 1312 bf 9 6 314 1312 bf 9 6 349 1312 bf 9 6 358 1312 bf 8 6 367 1312 bf 9 6 375 1312 bf 9 6 384 1312 bf 9
6 436 1312 bf 9 6 462 1312 bf 9 6 471 1312 bf 9 6 480 1312 bf 8 6 489 1312 bf 9 6 497 1312 bf 9 6 506 1312 bf 9 6 593 1312 bf 9 6 610 1312 bf 9 6 619 1312 bf 9 6 628 1312 bf 9 6 645 1312 bf 8 7 306 1318 bf 9 7 314 1318 bf 8 7 341 1318 bf 9 7 349
1318 bf 9 7 358 1318 bf 8 7 367 1318 bf 9 7 462 1318 bf 9 7 471 1318 bf 9 7 480 1318 bf 8 7 489 1318 bf 8 7 515 1318 bf 8 7 576 1318 bf 8 7 602 1318 bf 9 7 610 1318 bf 8 7 637 1318 bf 9 7 654 1318 bf 9 7 314 1325 bf 9 7 323 1325 bf 8 7 341 1325 bf 9
7 349 1325 bf 9 7 358 1325 bf 9 7 375 1325 bf 9 7 384 1325 bf 9 7 401 1325 bf 9 7 471 1325 bf 9 7 480 1325 bf 8 7 489 1325 bf 9 7 497 1325 bf 9 7 523 1325 bf 9 7 593 1325 bf 9 7 610 1325 bf 9 7 628 1325 bf 9 7 671 1325 bf 9 7 776 1325 bf 9 7 793
1325 bf 9 7 802 1325 bf 9 7 314 1332 bf 9 7 323 1332 bf 8 7 341 1332 bf 9 7 349 1332 bf 9 7 358 1332 bf 8 7 367 1332 bf 9 7 375 1332 bf 9 7 384 1332 bf 8 7 393 1332 bf 9 7 445 1332 bf 9 7 462 1332 bf 9 7 471 1332 bf 9 7 480 1332 bf 8 7 489 1332 bf 9
7 497 1332 bf 9 7 593 1332 bf 9 6 314 1339 bf 9 6 323 1339 bf 8 6 341 1339 bf 9 6 349 1339 bf 9 6 358 1339 bf 8 6 454 1339 bf 9 6 462 1339 bf 8 6 489 1339 bf 8 6 576 1339 bf 9 6 584 1339 bf 9 6 619 1339 bf 9 7 323 1345 bf 9 7 332 1345 bf 8 7 341
1345 bf 9 7 349 1345 bf 9 7 358 1345 bf 9 7 375 1345 bf 9 7 384 1345 bf 8 7 393 1345 bf 9 7 419 1345 bf 8 7 454 1345 bf 9 7 462 1345 bf 9 7 471 1345 bf 9 7 558 1345 bf 9 7 567 1345 bf 8 7 576 1345 bf 9 7 584 1345 bf 9 7 593 1345 bf 8 7 602 1345 bf 9
7 323 1352 bf 9 7 332 1352 bf 8 7 341 1352 bf 9 7 349 1352 bf 9 7 358 1352 bf 8 7 367 1352 bf 9 7 375 1352 bf 8 7 393 1352 bf 9 7 445 1352 bf 8 7 454 1352 bf 9 7 462 1352 bf 9 7 471 1352 bf 8 7 489 1352 bf 9 7 584 1352 bf 9 7 593 1352 bf 9 7 332
1359 bf 8 7 341 1359 bf 9 7 349 1359 bf 8 7 367 1359 bf 9 7 375 1359 bf 9 7 419 1359 bf 9 7 436 1359 bf 9 7 445 1359 bf 8 7 454 1359 bf 9 7 462 1359 bf 9 7 558 1359 bf 8 7 576 1359 bf 9 7 584 1359 bf 9 7 593 1359 bf 9 6 332 1366 bf 8 6 341 1366 bf 9
6 349 1366 bf 9 6 375 1366 bf 9 6 384 1366 bf 9 6 436 1366 bf 9 6 445 1366 bf 8 6 454 1366 bf 9 6 462 1366 bf 8 6 550 1366 bf 8 7 341 1372 bf 9 7 349 1372 bf 9 7 358 1372 bf 8 7 367 1372 bf 8 7 428 1372 bf 9 7 436 1372 bf 9 7 445 1372 bf 9 7 462
1372 bf 9 7 558 1372 bf 8 7 341 1379 bf 9 7 349 1379 bf 8 7 367 1379 bf 8 7 393 1379 bf 9 7 419 1379 bf 8 7 428 1379 bf 9 7 436 1379 bf 9 7 445 1379 bf 9 7 462 1379 bf 9 7 532 1379 bf 9 7 541 1379 bf 8 7 341 1386 bf 9 7 349 1386 bf 9 7 358 1386 bf 8
7 367 1386 bf 9 7 384 1386 bf 8 7 393 1386 bf 9 7 436 1386 bf 9 7 445 1386 bf 9 7 532 1386 bf 8 7 550 1386 bf 9 6 349 1393 bf 9 6 358 1393 bf 9 6 375 1393 bf 8 6 428 1393 bf 9 6 436 1393 bf 9 6 445 1393 bf 9 7 349 1399 bf 9 7 358 1399 bf 8 7 367
1399 bf 9 7 419 1399 bf 8 7 428 1399 bf 9 7 436 1399 bf 9 7 506 1399 bf 9 7 523 1399 bf 9 7 558 1399 bf 9 7 358 1406 bf 8 7 367 1406 bf 9 7 410 1406 bf 8 7 428 1406 bf 9 7 445 1406 bf 9 7 506 1406 bf 8 7 515 1406 bf 9 7 358 1413 bf 8 7 367 1413 bf 9
7 375 1413 bf 9 7 384 1413 bf 9 7 401 1413 bf 9 7 410 1413 bf 9 7 419 1413 bf 8 7 428 1413 bf 9 7 436 1413 bf 9 7 462 1413 bf 9 7 506 1413 bf 8 7 515 1413 bf 9 7 584 1413 bf 8 6 367 1420 bf 9 6 401 1420 bf 9 6 419 1420 bf 8 6 428 1420 bf 9 6 436
1420 bf 8 6 489 1420 bf 9 6 497 1420 bf 8 6 515 1420 bf 9 6 523 1420 bf 8 7 367 1426 bf 9 7 375 1426 bf 9 7 410 1426 bf 9 7 419 1426 bf 8 7 428 1426 bf 9 7 793 1426 bf 9 7 375 1433 bf 8 7 393 1433 bf 8 7 489 1433 bf 9 7 497 1433 bf 9 7 506 1433 bf 9
7 523 1433 bf 9 7 375 1440 bf 9 7 384 1440 bf 9 7 410 1440 bf 9 7 419 1440 bf 9 7 480 1440 bf 8 7 489 1440 bf 9 7 497 1440 bf 9 6 375 1447 bf 9 6 384 1447 bf 9 6 401 1447 bf 9 6 410 1447 bf 9 6 419 1447 bf 9 7 384 1453 bf 9 7 497 1453 bf 8 7 576
1453 bf 9 7 384 1460 bf 8 7 393 1460 bf 9 7 401 1460 bf 9 7 410 1460 bf 9 7 419 1460 bf 9 7 462 1460 bf 8 7 393 1467 bf 9 7 401 1467 bf 9 7 410 1467 bf 9 7 471 1467 bf 8 7 489 1467 bf 8 6 393 1474 bf 9 6 401 1474 bf 9 6 462 1474 bf 9 6 471 1474 bf 9
6 480 1474 bf 9 7 401 1480 bf 9 7 410 1480 bf 9 7 462 1480 bf 9 7 480 1480 bf 9 7 401 1487 bf 9 7 410 1487 bf 9 7 419 1487 bf 9 7 462 1487 bf 9 7 401 1494 bf 9 7 410 1494 bf 9 7 462 1494 bf 9 7 480 1494 bf 9 7 828 1494 bf 9 6 410 1501 bf 8 6 454
1501 bf 9 7 410 1507 bf 9 7 419 1507 bf 9 7 471 1507 bf 9 7 419 1514 bf 8 7 454 1514 bf 9 7 480 1514 bf 9 7 419 1521 bf 8 7 428 1521 bf 9 7 436 1521 bf 9 7 462 1521 bf 9 7 471 1521 bf 8 6 428 1528 bf 8 6 454 1528 bf 9 6 462 1528 bf 8 7 428 1534 bf 9
7 436 1534 bf 9 7 445 1534 bf 8 7 454 1534 bf 9 7 462 1534 bf 8 7 428 1541 bf 9 7 436 1541 bf 9 7 436 1548 bf 9 7 445 1548 bf 8 7 454 1548 bf 9 6 436 1555 bf 9 6 445 1555 bf 9 7 436 1561 bf 9 7 445 1561 bf 8 7 454 1561 bf 9 7 462 1561 bf 9 7 445
1568 bf 8 7 454 1568 bf 9 7 445 1575 bf 8 7 454 1575 bf 8 6 454 1582 bf 8 7 454 1588 bf 9 7 462 1588 bf 9 7 462 1595 bf 9 7 471 1602 bf 9 6 471 1609 bf 9 7 471 1615 bf 9 7 480 1629 bf 8 6 489 1636 bf 8 7 489 1642 bf 8 7 515 1642 bf 8 7 489 1649 bf 1
1 1 c black 132 981 m 870 X s
gsave 1088 844 23 896 C 569.206 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 1001 m -20 Y s 149 991 m -10 Y s 166 991 m -10 Y s 184 991 m -10 Y s 201 991 m -10 Y s 219 1001 m -20 Y s 236 991 m
-10 Y s 253 991 m -10 Y s 271 991 m -10 Y s 288 991 m -10 Y s 306 1001 m -20 Y s 323 991 m -10 Y s 341 991 m -10 Y s 358 991 m -10 Y s 375 991 m -10 Y s 393 1001 m -20 Y s 410 991 m -10 Y s 428 991 m -10 Y s 445 991 m -10 Y s 462 991 m -10 Y s 480
1001 m -20 Y s 497 991 m -10 Y s 515 991 m -10 Y s 532 991 m -10 Y s 550 991 m -10 Y s 567 1001 m -20 Y s 584 991 m -10 Y s 602 991 m -10 Y s 619 991 m -10 Y s 637 991 m -10 Y s 654 1001 m -20 Y s 671 991 m -10 Y s 689 991 m -10 Y s 706 991 m -10 Y
s 724 991 m -10 Y s 741 1001 m -20 Y s 759 991 m -10 Y s 776 991 m -10 Y s 793 991 m -10 Y s 811 991 m -10 Y s 828 1001 m -20 Y s 846 991 m -10 Y s 863 991 m -10 Y s 880 991 m -10 Y s 898 991 m -10 Y s 915 1001 m -20 Y s 933 991 m -10 Y s 950 991 m
-10 Y s 967 991 m -10 Y s 985 991 m -10 Y s 1002 1001 m -20 Y s
gsave 1088 844 23 896 C 120.672 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 182.146 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 268.665 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 355.185 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 441.704 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 23 896 C 530.5 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 23 896 C 617.019 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 23 896 C 703.539 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 23 896 C 790.058 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 23 896 C 876.577 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 23 896 C 956.266 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 1656 m 870 X s 132 1636 m 20 Y s 149 1646 m 10 Y s 166 1646 m 10 Y s 184 1646 m 10 Y s 201 1646 m 10 Y s 219 1636 m 20 Y s 236 1646 m 10
Y s 253 1646 m 10 Y s 271 1646 m 10 Y s 288 1646 m 10 Y s 306 1636 m 20 Y s 323 1646 m 10 Y s 341 1646 m 10 Y s 358 1646 m 10 Y s 375 1646 m 10 Y s 393 1636 m 20 Y s 410 1646 m 10 Y s 428 1646 m 10 Y s 445 1646 m 10 Y s 462 1646 m 10 Y s 480 1636 m
20 Y s 497 1646 m 10 Y s 515 1646 m 10 Y s 532 1646 m 10 Y s 550 1646 m 10 Y s 567 1636 m 20 Y s 584 1646 m 10 Y s 602 1646 m 10 Y s 619 1646 m 10 Y s 637 1646 m 10 Y s 654 1636 m 20 Y s 671 1646 m 10 Y s 689 1646 m 10 Y s 706 1646 m 10 Y s 724 1646
m 10 Y s 741 1636 m 20 Y s 759 1646 m 10 Y s 776 1646 m 10 Y s 793 1646 m 10 Y s 811 1646 m 10 Y s 828 1636 m 20 Y s 846 1646 m 10 Y s 863 1646 m 10 Y s 880 1646 m 10 Y s 898 1646 m 10 Y s 915 1636 m 20 Y s 933 1646 m 10 Y s 950 1646 m 10 Y s 967
1646 m 10 Y s 985 1646 m 10 Y s 1002 1636 m 20 Y s 132 981 m 675 Y s
gsave 1088 844 23 896 C 54.6438 1400.25 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 158 981 m -26 X s 145 997 m -13 X s 145 1013 m -13 X s 145 1029 m -13 X s 145 1045 m -13 X s 158 1061 m -26 X s 145 1077 m -13 X
s 145 1093 m -13 X s 145 1109 m -13 X s 145 1125 m -13 X s 158 1142 m -26 X s 145 1158 m -13 X s 145 1174 m -13 X s 145 1190 m -13 X s 145 1206 m -13 X s 158 1222 m -26 X s 145 1238 m -13 X s 145 1254 m -13 X s 145 1270 m -13 X s 145 1286 m -13 X s
158 1302 m -26 X s 145 1318 m -13 X s 145 1334 m -13 X s 145 1350 m -13 X s 145 1366 m -13 X s 158 1383 m -26 X s 145 1399 m -13 X s 145 1415 m -13 X s 145 1431 m -13 X s 145 1447 m -13 X s 158 1463 m -26 X s 145 1479 m -13 X s 145 1495 m -13 X s
145 1511 m -13 X s 145 1527 m -13 X s 158 1543 m -26 X s 145 1559 m -13 X s 145 1575 m -13 X s 145 1591 m -13 X s 145 1608 m -13 X s 158 1624 m -26 X s 158 1624 m -26 X s 145 1640 m -13 X s 145 1656 m -13 X s
gsave 1088 844 23 896 C 107.011 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 72.8584 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 844 23 896 C 54.6438 1129.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 54.6438 1208.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 844 23 896 C 54.6438 1288.68 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 54.6438 1370.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 844 23 896 C 54.6438 1450.34 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 54.6438 1530.03 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 844 23 896 C 54.6438 1611.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 1002 981 m 675 Y s 976 981 m 26 X s 989 997 m 13 X s 989 1013 m 13 X s 989 1029 m 13 X s 989 1045 m 13 X s 976 1061 m 26 X s 989 1077 m 13 X
s 989 1093 m 13 X s 989 1109 m 13 X s 989 1125 m 13 X s 976 1142 m 26 X s 989 1158 m 13 X s 989 1174 m 13 X s 989 1190 m 13 X s 989 1206 m 13 X s 976 1222 m 26 X s 989 1238 m 13 X s 989 1254 m 13 X s 989 1270 m 13 X s 989 1286 m 13 X s 976 1302 m 26
X s 989 1318 m 13 X s 989 1334 m 13 X s 989 1350 m 13 X s 989 1366 m 13 X s 976 1383 m 26 X s 989 1399 m 13 X s 989 1415 m 13 X s 989 1431 m 13 X s 989 1447 m 13 X s 976 1463 m 26 X s 989 1479 m 13 X s 989 1495 m 13 X s 989 1511 m 13 X s 989 1527 m
13 X s 976 1543 m 26 X s 989 1559 m 13 X s 989 1575 m 13 X s 989 1591 m 13 X s 989 1608 m 13 X s 976 1624 m 26 X s 976 1624 m 26 X s 989 1640 m 13 X s 989 1656 m 13 X s 0.386667 0 1 c 49 34 1008 981 bf 0.2 0 1 c 49 33 1008 1015 bf 0 0.0800001 1 c 49
34 1008 1048 bf 0 0.266667 1 c 49 34 1008 1082 bf 0 0.546666 1 c 49 34 1008 1116 bf 0 0.733333 1 c 49 33 1008 1150 bf 0 1 0.986667 c 49 34 1008 1183 bf 0 1 0.8 c 49 34 1008 1217 bf 0 1 0.52 c 49 34 1008 1251 bf 0 1 0.333333 c 49 33 1008 1285 bf 0 1
0.0533333 c 49 34 1008 1318 bf 0.133333 1 0 c 49 34 1008 1352 bf 0.413333 1 0 c 49 34 1008 1386 bf 0.6 1 0 c 49 33 1008 1420 bf 0.88 1 0 c 49 34 1008 1453 bf 1 0.933333 0 c 49 34 1008 1487 bf 1 0.653333 0 c 49 34 1008 1521 bf 1 0.466667 0 c 49 33
1008 1555 bf 1 0.186667 0 c 49 34 1008 1588 bf 1 0 0 c 49 34 1008 1622 bf black 1057 981 m 675 Y s 1031 981 m 26 X s 1031 1095 m 26 X s 1031 1208 m 26 X s 1031 1322 m 26 X s 1031 1436 m 26 X s 1031 1549 m 26 X s 1031 1549 m 26 X s
gsave 1088 844 23 896 C 1061 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 1061 1081.49 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 1061 1195.33 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 1061 1309.17 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 1061 1423.01 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 23 896 C 1061 1536.86 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 23 896 C 1108.81 1678.02 t 0 r /Helvetica-Bold findfont 20.5224 sf 0 0 m (3) show NC gr
gsave 1088 844 23 896 C 1074.66 1659.8 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 844 23 896 C 1056.45 1659.8 t 0 r /Symbol findfont 31.9238 sf 0 0 m (<EFBFBD>) show NC gr 1 1 1 c 240 47 34 1689 bf black 34 1689 m 240 X s 274 1689 m 47 Y s 274 1736 m -240 X s 34 1736 m -47 Y s 1 1 1 c black
gsave 1088 844 23 896 C 47.8133 1703.06 t 0 r /Helvetica-Bold findfont 36.4843 sf 0 0 m (All particles) show NC gr 1 1 1 c 1088 844 1157 896 bf black 1 1 1 c 871 675 1265 981 bf black 871 675 1265 981 bl 1 1 1 c 871 675 1265 981 bf black 871 675
1265 981 bl 1 1 1 c 0 0.0800001 1 c 9 7 1265 981 bf 0 0.733333 1 c 9 6 1265 988 bf 0.2 0 1 c 9 7 1265 994 bf 0 0.0800001 1 c 9 7 1274 994 bf 0 1 0.8 c 9 7 1274 1001 bf 0 0.0800001 1 c 9 7 1274 1008 bf 9 7 1283 1008 bf 0.386667 0 1 c 9 7 1814 1008 bf
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991 m -10 Y s 1387 991 m -10 Y s 1405 991 m -10 Y s 1422 991 m -10 Y s 1440 1001 m -20 Y s 1457 991 m -10 Y s 1474 991 m -10 Y s 1492 991 m -10 Y s 1509 991 m -10 Y s 1527 1001 m -20 Y s 1544 991 m -10 Y s 1561 991 m -10 Y s 1579 991 m -10 Y s 1596
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gsave 1088 844 1157 896 C 1254.53 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 1157 896 C 1316 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 1157 896 C 1402.52 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 1157 896 C 1489.04 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 1157 896 C 1575.56 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 1157 896 C 1664.36 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 1157 896 C 1750.88 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 1157 896 C 1837.4 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 1157 896 C 1923.92 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 1157 896 C 2010.44 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 1157 896 C 2090.12 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 1265 1656 m 871 X s 1265 1636 m 20 Y s 1283 1646 m 10 Y s 1300 1646 m 10 Y s 1318 1646 m 10 Y s 1335 1646 m 10 Y s 1352 1636 m 20 Y s 1370
1646 m 10 Y s 1387 1646 m 10 Y s 1405 1646 m 10 Y s 1422 1646 m 10 Y s 1440 1636 m 20 Y s 1457 1646 m 10 Y s 1474 1646 m 10 Y s 1492 1646 m 10 Y s 1509 1646 m 10 Y s 1527 1636 m 20 Y s 1544 1646 m 10 Y s 1561 1646 m 10 Y s 1579 1646 m 10 Y s 1596
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gsave 1088 844 1157 896 C 1188.5 1400.25 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 1292 981 m -27 X s 1278 997 m -13 X s 1278 1013 m -13 X s 1278 1029 m -13 X s 1278 1045 m -13 X s 1292 1061 m -27 X s 1278 1077
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gsave 1088 844 1157 896 C 1188.5 1288.68 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
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gsave 1088 844 1157 896 C 2194.86 1067.83 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5) show NC gr
gsave 1088 844 1157 896 C 2194.86 1161.18 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
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615 bf 0.2 0 1 c 9 6 410 622 bf 0.386667 0 1 c 9 7 410 628 bf 9 7 445 682 bf 1 1 1 c black 132 102 m 870 X s
gsave 1088 843 23 18 C 569.206 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 122 m -20 Y s 149 112 m -10 Y s 166 112 m -10 Y s 184 112 m -10 Y s 201 112 m -10 Y s 219 122 m -20 Y s 236 112 m -10 Y
s 253 112 m -10 Y s 271 112 m -10 Y s 288 112 m -10 Y s 306 122 m -20 Y s 323 112 m -10 Y s 341 112 m -10 Y s 358 112 m -10 Y s 375 112 m -10 Y s 393 122 m -20 Y s 410 112 m -10 Y s 428 112 m -10 Y s 445 112 m -10 Y s 462 112 m -10 Y s 480 122 m -20
Y s 497 112 m -10 Y s 515 112 m -10 Y s 532 112 m -10 Y s 550 112 m -10 Y s 567 122 m -20 Y s 584 112 m -10 Y s 602 112 m -10 Y s 619 112 m -10 Y s 637 112 m -10 Y s 654 122 m -20 Y s 671 112 m -10 Y s 689 112 m -10 Y s 706 112 m -10 Y s 724 112 m
-10 Y s 741 122 m -20 Y s 759 112 m -10 Y s 776 112 m -10 Y s 793 112 m -10 Y s 811 112 m -10 Y s 828 122 m -20 Y s 846 112 m -10 Y s 863 112 m -10 Y s 880 112 m -10 Y s 898 112 m -10 Y s 915 122 m -20 Y s 933 112 m -10 Y s 950 112 m -10 Y s 967 112
m -10 Y s 985 112 m -10 Y s 1002 122 m -20 Y s
gsave 1088 843 23 18 C 120.672 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 23 18 C 182.146 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 23 18 C 268.665 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 23 18 C 355.185 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 23 18 C 441.704 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 843 23 18 C 530.5 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 843 23 18 C 617.019 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 843 23 18 C 703.539 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 843 23 18 C 790.058 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 843 23 18 C 876.577 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 843 23 18 C 956.266 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 777 m 870 X s 132 757 m 20 Y s 149 767 m 10 Y s 166 767 m 10 Y s 184 767 m 10 Y s 201 767 m 10 Y s 219 757 m 20 Y s 236 767 m 10 Y s 253
767 m 10 Y s 271 767 m 10 Y s 288 767 m 10 Y s 306 757 m 20 Y s 323 767 m 10 Y s 341 767 m 10 Y s 358 767 m 10 Y s 375 767 m 10 Y s 393 757 m 20 Y s 410 767 m 10 Y s 428 767 m 10 Y s 445 767 m 10 Y s 462 767 m 10 Y s 480 757 m 20 Y s 497 767 m 10 Y
s 515 767 m 10 Y s 532 767 m 10 Y s 550 767 m 10 Y s 567 757 m 20 Y s 584 767 m 10 Y s 602 767 m 10 Y s 619 767 m 10 Y s 637 767 m 10 Y s 654 757 m 20 Y s 671 767 m 10 Y s 689 767 m 10 Y s 706 767 m 10 Y s 724 767 m 10 Y s 741 757 m 20 Y s 759 767 m
10 Y s 776 767 m 10 Y s 793 767 m 10 Y s 811 767 m 10 Y s 828 757 m 20 Y s 846 767 m 10 Y s 863 767 m 10 Y s 880 767 m 10 Y s 898 767 m 10 Y s 915 757 m 20 Y s 933 767 m 10 Y s 950 767 m 10 Y s 967 767 m 10 Y s 985 767 m 10 Y s 1002 757 m 20 Y s 132
102 m 675 Y s
gsave 1088 843 23 18 C 54.6438 521.393 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 158 102 m -26 X s 145 118 m -13 X s 145 134 m -13 X s 145 150 m -13 X s 145 166 m -13 X s 158 182 m -26 X s 145 198 m -13 X s 145
214 m -13 X s 145 231 m -13 X s 145 247 m -13 X s 158 263 m -26 X s 145 279 m -13 X s 145 295 m -13 X s 145 311 m -13 X s 145 327 m -13 X s 158 343 m -26 X s 145 359 m -13 X s 145 375 m -13 X s 145 391 m -13 X s 145 407 m -13 X s 158 423 m -26 X s
145 439 m -13 X s 145 455 m -13 X s 145 472 m -13 X s 145 488 m -13 X s 158 504 m -26 X s 145 520 m -13 X s 145 536 m -13 X s 145 552 m -13 X s 145 568 m -13 X s 158 584 m -26 X s 145 600 m -13 X s 145 616 m -13 X s 145 632 m -13 X s 145 648 m -13 X
s 158 664 m -26 X s 145 680 m -13 X s 145 697 m -13 X s 145 713 m -13 X s 145 729 m -13 X s 158 745 m -26 X s 158 745 m -26 X s 145 761 m -13 X s 145 777 m -13 X s
gsave 1088 843 23 18 C 107.011 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
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428 994 bf 9 7 436 994 bf 9 7 471 994 bf 9 7 480 994 bf 9 7 506 994 bf 8 7 550 994 bf 9 7 567 994 bf 8 7 811 994 bf 9 7 140 1001 bf 9 7 149 1001 bf 8 7 158 1001 bf 9 7 166 1001 bf 9 7 175 1001 bf 8 7 184 1001 bf 9 7 192 1001 bf 9 7 201 1001 bf 9 7
210 1001 bf 8 7 219 1001 bf 9 7 227 1001 bf 9 7 236 1001 bf 8 7 245 1001 bf 9 7 253 1001 bf 9 7 262 1001 bf 9 7 271 1001 bf 8 7 280 1001 bf 9 7 288 1001 bf 9 7 297 1001 bf 9 7 323 1001 bf 9 7 332 1001 bf 9 7 349 1001 bf 9 7 358 1001 bf 9 7 375 1001
bf 9 7 445 1001 bf 9 7 506 1001 bf 9 7 541 1001 bf 9 7 567 1001 bf 9 7 593 1001 bf 9 7 750 1001 bf 9 7 140 1008 bf 9 7 149 1008 bf 8 7 158 1008 bf 9 7 166 1008 bf 9 7 175 1008 bf 8 7 184 1008 bf 9 7 192 1008 bf 9 7 201 1008 bf 9 7 210 1008 bf 8 7
219 1008 bf 9 7 227 1008 bf 9 7 236 1008 bf 8 7 245 1008 bf 9 7 253 1008 bf 9 7 262 1008 bf 9 7 271 1008 bf 8 7 280 1008 bf 9 7 288 1008 bf 9 7 297 1008 bf 8 7 306 1008 bf 9 7 323 1008 bf 9 7 332 1008 bf 8 7 428 1008 bf 9 7 462 1008 bf 9 7 541 1008
bf 9 7 593 1008 bf 9 7 645 1008 bf 8 7 663 1008 bf 9 7 750 1008 bf 9 6 149 1015 bf 8 6 158 1015 bf 9 6 166 1015 bf 9 6 175 1015 bf 8 6 184 1015 bf 9 6 192 1015 bf 9 6 201 1015 bf 9 6 210 1015 bf 8 6 219 1015 bf 9 6 227 1015 bf 9 6 236 1015 bf 8 6
245 1015 bf 9 6 253 1015 bf 9 6 271 1015 bf 9 6 288 1015 bf 8 6 341 1015 bf 9 6 358 1015 bf 9 6 462 1015 bf 9 6 471 1015 bf 9 6 680 1015 bf 9 6 706 1015 bf 9 6 889 1015 bf 9 7 149 1021 bf 8 7 158 1021 bf 9 7 166 1021 bf 9 7 175 1021 bf 9 7 192 1021
bf 9 7 201 1021 bf 9 7 210 1021 bf 8 7 219 1021 bf 9 7 227 1021 bf 9 7 236 1021 bf 9 7 253 1021 bf 9 7 262 1021 bf 9 7 288 1021 bf 8 7 306 1021 bf 9 7 314 1021 bf 9 7 323 1021 bf 9 7 349 1021 bf 9 7 375 1021 bf 9 7 471 1021 bf 9 7 767 1021 bf 9 7
819 1021 bf 9 7 837 1021 bf 9 7 854 1021 bf 9 7 863 1021 bf 9 7 880 1021 bf 9 7 889 1021 bf 9 7 924 1021 bf 8 7 933 1021 bf 8 7 994 1021 bf 9 7 149 1028 bf 8 7 158 1028 bf 9 7 166 1028 bf 8 7 184 1028 bf 9 7 192 1028 bf 9 7 201 1028 bf 9 7 210 1028
bf 8 7 219 1028 bf 9 7 227 1028 bf 8 7 245 1028 bf 8 7 280 1028 bf 9 7 332 1028 bf 9 7 349 1028 bf 8 7 367 1028 bf 9 7 375 1028 bf 9 7 401 1028 bf 8 7 550 1028 bf 8 7 576 1028 bf 9 7 837 1028 bf 9 7 889 1028 bf 8 7 959 1028 bf 9 7 967 1028 bf 9 7
976 1028 bf 8 7 994 1028 bf 8 7 158 1035 bf 9 7 166 1035 bf 8 7 184 1035 bf 9 7 210 1035 bf 9 7 227 1035 bf 8 7 306 1035 bf 9 7 323 1035 bf 8 7 341 1035 bf 9 7 375 1035 bf 8 7 393 1035 bf 9 7 828 1035 bf 8 7 933 1035 bf 8 6 158 1042 bf 9 6 166 1042
bf 8 6 184 1042 bf 9 6 192 1042 bf 8 6 219 1042 bf 8 6 245 1042 bf 9 6 253 1042 bf 9 6 262 1042 bf 9 6 271 1042 bf 8 6 280 1042 bf 9 6 288 1042 bf 9 6 297 1042 bf 9 6 349 1042 bf 9 6 384 1042 bf 8 6 515 1042 bf 9 6 532 1042 bf 9 6 628 1042 bf 9 7
166 1048 bf 9 7 201 1048 bf 9 7 253 1048 bf 8 7 280 1048 bf 9 7 323 1048 bf 9 7 332 1048 bf 9 7 349 1048 bf 8 7 393 1048 bf 9 7 837 1048 bf 8 7 846 1048 bf 9 7 166 1055 bf 9 7 175 1055 bf 9 7 192 1055 bf 9 7 210 1055 bf 9 7 262 1055 bf 9 7 271 1055
bf 8 7 280 1055 bf 9 7 297 1055 bf 8 7 306 1055 bf 9 7 323 1055 bf 9 7 384 1055 bf 9 7 419 1055 bf 8 7 698 1055 bf 9 7 793 1055 bf 9 7 941 1055 bf 8 7 959 1055 bf 9 7 967 1055 bf 9 7 976 1055 bf 8 7 994 1055 bf 9 7 175 1062 bf 8 7 184 1062 bf 9 7
236 1062 bf 8 7 245 1062 bf 9 7 253 1062 bf 9 7 271 1062 bf 9 7 288 1062 bf 9 7 297 1062 bf 8 7 306 1062 bf 9 7 384 1062 bf 8 7 602 1062 bf 9 7 706 1062 bf 8 7 785 1062 bf 8 7 872 1062 bf 9 7 880 1062 bf 9 7 889 1062 bf 9 7 898 1062 bf 8 7 907 1062
bf 9 7 915 1062 bf 9 7 924 1062 bf 9 7 941 1062 bf 9 7 950 1062 bf 8 7 959 1062 bf 9 7 967 1062 bf 9 7 976 1062 bf 9 7 985 1062 bf 8 7 994 1062 bf 9 6 175 1069 bf 9 6 227 1069 bf 8 6 245 1069 bf 9 6 253 1069 bf 9 6 262 1069 bf 9 6 288 1069 bf 8 6
306 1069 bf 9 6 323 1069 bf 9 6 706 1069 bf 8 6 846 1069 bf 9 6 854 1069 bf 9 6 863 1069 bf 8 6 872 1069 bf 9 6 880 1069 bf 9 6 889 1069 bf 9 6 898 1069 bf 8 6 907 1069 bf 9 6 915 1069 bf 9 6 924 1069 bf 8 6 933 1069 bf 9 6 941 1069 bf 9 6 950 1069
bf 8 6 959 1069 bf 9 6 967 1069 bf 9 6 976 1069 bf 9 6 985 1069 bf 8 6 994 1069 bf 9 7 175 1075 bf 8 7 184 1075 bf 9 7 236 1075 bf 9 7 253 1075 bf 9 7 262 1075 bf 9 7 271 1075 bf 9 7 297 1075 bf 9 7 567 1075 bf 9 7 776 1075 bf 8 7 785 1075 bf 9 7
793 1075 bf 9 7 802 1075 bf 8 7 811 1075 bf 9 7 819 1075 bf 9 7 828 1075 bf 9 7 837 1075 bf 8 7 846 1075 bf 9 7 854 1075 bf 9 7 863 1075 bf 8 7 872 1075 bf 9 7 880 1075 bf 9 7 889 1075 bf 9 7 898 1075 bf 8 7 907 1075 bf 9 7 915 1075 bf 9 7 924 1075
bf 8 7 933 1075 bf 9 7 941 1075 bf 9 7 950 1075 bf 8 7 959 1075 bf 9 7 967 1075 bf 9 7 976 1075 bf 9 7 985 1075 bf 8 7 994 1075 bf 8 7 184 1082 bf 9 7 236 1082 bf 9 7 253 1082 bf 9 7 297 1082 bf 8 7 341 1082 bf 8 7 367 1082 bf 8 7 393 1082 bf 9 7
715 1082 bf 8 7 724 1082 bf 9 7 732 1082 bf 9 7 741 1082 bf 9 7 750 1082 bf 8 7 759 1082 bf 9 7 767 1082 bf 9 7 776 1082 bf 8 7 785 1082 bf 9 7 793 1082 bf 9 7 802 1082 bf 8 7 811 1082 bf 9 7 819 1082 bf 9 7 828 1082 bf 9 7 837 1082 bf 8 7 846 1082
bf 9 7 854 1082 bf 9 7 863 1082 bf 8 7 872 1082 bf 9 7 880 1082 bf 9 7 889 1082 bf 9 7 898 1082 bf 8 7 907 1082 bf 9 7 915 1082 bf 9 7 924 1082 bf 8 7 933 1082 bf 9 7 941 1082 bf 9 7 950 1082 bf 8 7 959 1082 bf 9 7 967 1082 bf 9 7 985 1082 bf 8 7
994 1082 bf 8 7 184 1089 bf 9 7 192 1089 bf 9 7 227 1089 bf 9 7 236 1089 bf 8 7 245 1089 bf 9 7 253 1089 bf 8 7 280 1089 bf 8 7 306 1089 bf 8 7 341 1089 bf 9 7 523 1089 bf 9 7 567 1089 bf 9 7 689 1089 bf 8 7 698 1089 bf 9 7 706 1089 bf 9 7 715 1089
bf 8 7 724 1089 bf 9 7 732 1089 bf 9 7 741 1089 bf 9 7 750 1089 bf 8 7 759 1089 bf 9 7 767 1089 bf 9 7 776 1089 bf 8 7 785 1089 bf 9 7 793 1089 bf 9 7 802 1089 bf 8 7 811 1089 bf 9 7 819 1089 bf 9 7 828 1089 bf 9 7 837 1089 bf 8 7 846 1089 bf 9 7
854 1089 bf 9 7 863 1089 bf 8 7 872 1089 bf 9 7 880 1089 bf 9 7 889 1089 bf 9 7 898 1089 bf 9 7 915 1089 bf 9 7 924 1089 bf 8 7 933 1089 bf 9 7 941 1089 bf 8 7 959 1089 bf 9 7 976 1089 bf 9 6 192 1096 bf 9 6 201 1096 bf 9 6 227 1096 bf 9 6 271 1096
bf 9 6 323 1096 bf 9 6 654 1096 bf 8 6 663 1096 bf 9 6 671 1096 bf 9 6 680 1096 bf 9 6 689 1096 bf 8 6 698 1096 bf 9 6 706 1096 bf 9 6 715 1096 bf 8 6 724 1096 bf 9 6 732 1096 bf 9 6 741 1096 bf 9 6 750 1096 bf 8 6 759 1096 bf 9 6 767 1096 bf 9 6
776 1096 bf 8 6 785 1096 bf 9 6 793 1096 bf 9 6 802 1096 bf 8 6 811 1096 bf 9 6 819 1096 bf 9 6 828 1096 bf 9 6 837 1096 bf 8 6 846 1096 bf 9 6 854 1096 bf 9 6 863 1096 bf 9 6 880 1096 bf 9 6 889 1096 bf 9 6 898 1096 bf 8 6 907 1096 bf 9 6 915 1096
bf 8 6 933 1096 bf 9 6 985 1096 bf 9 7 192 1102 bf 8 7 280 1102 bf 9 7 332 1102 bf 8 7 341 1102 bf 8 7 393 1102 bf 9 7 462 1102 bf 9 7 584 1102 bf 9 7 619 1102 bf 8 7 637 1102 bf 9 7 654 1102 bf 8 7 663 1102 bf 9 7 671 1102 bf 9 7 680 1102 bf 9 7
689 1102 bf 8 7 698 1102 bf 9 7 706 1102 bf 9 7 715 1102 bf 8 7 724 1102 bf 9 7 732 1102 bf 9 7 741 1102 bf 9 7 750 1102 bf 8 7 759 1102 bf 9 7 767 1102 bf 9 7 776 1102 bf 8 7 785 1102 bf 9 7 793 1102 bf 9 7 802 1102 bf 8 7 811 1102 bf 9 7 819 1102
bf 9 7 828 1102 bf 9 7 837 1102 bf 8 7 846 1102 bf 9 7 854 1102 bf 9 7 863 1102 bf 8 7 872 1102 bf 9 7 898 1102 bf 9 7 192 1109 bf 9 7 201 1109 bf 9 7 236 1109 bf 8 7 602 1109 bf 9 7 610 1109 bf 9 7 619 1109 bf 9 7 628 1109 bf 8 7 637 1109 bf 9 7
645 1109 bf 9 7 654 1109 bf 8 7 663 1109 bf 9 7 671 1109 bf 9 7 680 1109 bf 9 7 689 1109 bf 8 7 698 1109 bf 9 7 706 1109 bf 9 7 715 1109 bf 8 7 724 1109 bf 9 7 732 1109 bf 9 7 741 1109 bf 9 7 750 1109 bf 8 7 759 1109 bf 9 7 767 1109 bf 9 7 776 1109
bf 9 7 793 1109 bf 8 7 811 1109 bf 9 7 828 1109 bf 9 7 837 1109 bf 9 7 898 1109 bf 9 7 201 1116 bf 8 7 219 1116 bf 9 7 227 1116 bf 9 7 253 1116 bf 9 7 271 1116 bf 9 7 314 1116 bf 9 7 401 1116 bf 9 7 410 1116 bf 8 7 550 1116 bf 9 7 567 1116 bf 8 7
576 1116 bf 9 7 584 1116 bf 9 7 593 1116 bf 8 7 602 1116 bf 9 7 610 1116 bf 9 7 619 1116 bf 9 7 628 1116 bf 8 7 637 1116 bf 9 7 645 1116 bf 9 7 654 1116 bf 8 7 663 1116 bf 9 7 671 1116 bf 9 7 680 1116 bf 9 7 689 1116 bf 8 7 698 1116 bf 9 7 706 1116
bf 9 7 715 1116 bf 8 7 724 1116 bf 9 7 732 1116 bf 9 7 741 1116 bf 9 7 750 1116 bf 8 7 759 1116 bf 9 7 767 1116 bf 9 7 776 1116 bf 8 7 785 1116 bf 9 7 793 1116 bf 9 7 802 1116 bf 8 7 811 1116 bf 9 7 967 1116 bf 9 6 201 1123 bf 9 6 210 1123 bf 8 6
245 1123 bf 8 6 280 1123 bf 9 6 297 1123 bf 9 6 532 1123 bf 8 6 550 1123 bf 9 6 558 1123 bf 9 6 567 1123 bf 8 6 576 1123 bf 9 6 584 1123 bf 9 6 593 1123 bf 8 6 602 1123 bf 9 6 610 1123 bf 9 6 619 1123 bf 9 6 628 1123 bf 8 6 637 1123 bf 9 6 645 1123
bf 9 6 654 1123 bf 8 6 663 1123 bf 9 6 671 1123 bf 9 6 680 1123 bf 9 6 689 1123 bf 8 6 698 1123 bf 9 6 706 1123 bf 9 6 715 1123 bf 9 6 732 1123 bf 9 6 741 1123 bf 9 6 750 1123 bf 9 6 802 1123 bf 8 6 811 1123 bf 8 6 907 1123 bf 8 6 959 1123 bf 8 6
994 1123 bf 9 7 210 1129 bf 9 7 227 1129 bf 9 7 262 1129 bf 9 7 297 1129 bf 9 7 323 1129 bf 9 7 523 1129 bf 9 7 532 1129 bf 9 7 541 1129 bf 8 7 550 1129 bf 9 7 558 1129 bf 9 7 567 1129 bf 8 7 576 1129 bf 9 7 584 1129 bf 9 7 593 1129 bf 8 7 602 1129
bf 9 7 610 1129 bf 9 7 619 1129 bf 9 7 628 1129 bf 8 7 637 1129 bf 9 7 645 1129 bf 9 7 654 1129 bf 8 7 663 1129 bf 9 7 680 1129 bf 9 7 706 1129 bf 9 7 715 1129 bf 9 7 767 1129 bf 9 7 828 1129 bf 9 7 915 1129 bf 9 7 924 1129 bf 8 7 933 1129 bf 9 7
941 1129 bf 9 7 950 1129 bf 8 7 959 1129 bf 9 7 976 1129 bf 9 7 985 1129 bf 8 7 994 1129 bf 9 7 210 1136 bf 8 7 219 1136 bf 8 7 515 1136 bf 9 7 523 1136 bf 9 7 532 1136 bf 9 7 541 1136 bf 8 7 550 1136 bf 9 7 558 1136 bf 9 7 567 1136 bf 8 7 576 1136
bf 9 7 584 1136 bf 9 7 593 1136 bf 8 7 602 1136 bf 9 7 610 1136 bf 9 7 619 1136 bf 9 7 628 1136 bf 9 7 645 1136 bf 9 7 654 1136 bf 8 7 663 1136 bf 9 7 671 1136 bf 9 7 680 1136 bf 9 7 689 1136 bf 8 7 698 1136 bf 8 7 846 1136 bf 9 7 863 1136 bf 8 7
872 1136 bf 9 7 889 1136 bf 9 7 898 1136 bf 8 7 907 1136 bf 9 7 915 1136 bf 8 7 933 1136 bf 9 7 950 1136 bf 8 7 959 1136 bf 9 7 967 1136 bf 9 7 985 1136 bf 8 7 994 1136 bf 8 7 219 1143 bf 9 7 236 1143 bf 9 7 349 1143 bf 9 7 445 1143 bf 9 7 480 1143
bf 9 7 497 1143 bf 9 7 506 1143 bf 8 7 515 1143 bf 9 7 523 1143 bf 9 7 532 1143 bf 9 7 541 1143 bf 8 7 550 1143 bf 9 7 558 1143 bf 9 7 567 1143 bf 8 7 576 1143 bf 9 7 584 1143 bf 9 7 593 1143 bf 8 7 602 1143 bf 9 7 610 1143 bf 9 7 628 1143 bf 8 7
637 1143 bf 9 7 645 1143 bf 9 7 654 1143 bf 8 7 663 1143 bf 9 7 689 1143 bf 8 7 724 1143 bf 9 7 837 1143 bf 9 7 854 1143 bf 9 7 863 1143 bf 8 7 872 1143 bf 9 7 880 1143 bf 9 7 898 1143 bf 8 7 907 1143 bf 9 7 915 1143 bf 9 7 924 1143 bf 8 7 933 1143
bf 9 7 950 1143 bf 8 7 959 1143 bf 9 7 967 1143 bf 8 6 219 1150 bf 9 6 236 1150 bf 9 6 262 1150 bf 9 6 480 1150 bf 8 6 489 1150 bf 9 6 497 1150 bf 9 6 506 1150 bf 8 6 515 1150 bf 9 6 523 1150 bf 9 6 532 1150 bf 9 6 541 1150 bf 8 6 550 1150 bf 9 6
558 1150 bf 9 6 567 1150 bf 8 6 576 1150 bf 9 6 584 1150 bf 9 6 593 1150 bf 8 6 602 1150 bf 9 6 610 1150 bf 9 6 619 1150 bf 9 6 628 1150 bf 8 6 637 1150 bf 9 6 645 1150 bf 8 6 663 1150 bf 9 6 750 1150 bf 9 6 802 1150 bf 9 6 828 1150 bf 9 6 837 1150
bf 8 6 846 1150 bf 9 6 854 1150 bf 9 6 863 1150 bf 8 6 872 1150 bf 9 6 880 1150 bf 9 6 889 1150 bf 9 6 898 1150 bf 8 6 907 1150 bf 9 6 915 1150 bf 8 6 933 1150 bf 8 7 219 1156 bf 9 7 227 1156 bf 9 7 471 1156 bf 9 7 480 1156 bf 8 7 489 1156 bf 9 7
497 1156 bf 9 7 506 1156 bf 8 7 515 1156 bf 9 7 523 1156 bf 9 7 532 1156 bf 9 7 541 1156 bf 8 7 550 1156 bf 9 7 558 1156 bf 9 7 567 1156 bf 8 7 576 1156 bf 9 7 584 1156 bf 9 7 593 1156 bf 8 7 602 1156 bf 9 7 628 1156 bf 9 7 645 1156 bf 9 7 671 1156
bf 9 7 689 1156 bf 9 7 776 1156 bf 8 7 785 1156 bf 9 7 793 1156 bf 9 7 802 1156 bf 8 7 811 1156 bf 9 7 819 1156 bf 9 7 828 1156 bf 9 7 837 1156 bf 8 7 846 1156 bf 9 7 854 1156 bf 9 7 880 1156 bf 9 7 898 1156 bf 9 7 227 1163 bf 9 7 253 1163 bf 9 7
462 1163 bf 9 7 471 1163 bf 9 7 480 1163 bf 8 7 489 1163 bf 9 7 497 1163 bf 9 7 506 1163 bf 8 7 515 1163 bf 9 7 523 1163 bf 9 7 532 1163 bf 9 7 541 1163 bf 8 7 550 1163 bf 9 7 558 1163 bf 9 7 567 1163 bf 8 7 576 1163 bf 9 7 584 1163 bf 9 7 593 1163
bf 9 7 610 1163 bf 8 7 637 1163 bf 9 7 732 1163 bf 9 7 741 1163 bf 9 7 750 1163 bf 8 7 759 1163 bf 9 7 767 1163 bf 9 7 776 1163 bf 8 7 785 1163 bf 9 7 793 1163 bf 9 7 802 1163 bf 8 7 811 1163 bf 9 7 828 1163 bf 9 7 837 1163 bf 8 7 846 1163 bf 9 7
854 1163 bf 8 7 872 1163 bf 9 7 227 1170 bf 9 7 236 1170 bf 9 7 253 1170 bf 9 7 436 1170 bf 9 7 445 1170 bf 8 7 454 1170 bf 9 7 462 1170 bf 9 7 471 1170 bf 9 7 480 1170 bf 8 7 489 1170 bf 9 7 497 1170 bf 9 7 506 1170 bf 8 7 515 1170 bf 9 7 523 1170
bf 9 7 532 1170 bf 9 7 541 1170 bf 9 7 558 1170 bf 9 7 567 1170 bf 9 7 584 1170 bf 9 7 593 1170 bf 8 7 637 1170 bf 8 7 698 1170 bf 8 7 724 1170 bf 9 7 732 1170 bf 9 7 741 1170 bf 9 7 750 1170 bf 8 7 759 1170 bf 9 7 767 1170 bf 9 7 776 1170 bf 8 7
785 1170 bf 9 7 793 1170 bf 8 7 811 1170 bf 9 7 819 1170 bf 9 7 828 1170 bf 9 7 837 1170 bf 8 7 846 1170 bf 9 6 236 1177 bf 9 6 436 1177 bf 9 6 445 1177 bf 8 6 454 1177 bf 9 6 462 1177 bf 9 6 471 1177 bf 9 6 480 1177 bf 8 6 489 1177 bf 9 6 497 1177
bf 9 6 506 1177 bf 8 6 515 1177 bf 9 6 523 1177 bf 9 6 532 1177 bf 8 6 550 1177 bf 9 6 567 1177 bf 9 6 593 1177 bf 9 6 645 1177 bf 8 6 698 1177 bf 9 6 706 1177 bf 9 6 715 1177 bf 8 6 724 1177 bf 9 6 732 1177 bf 9 6 741 1177 bf 9 6 750 1177 bf 8 6
759 1177 bf 9 6 767 1177 bf 9 6 776 1177 bf 8 6 785 1177 bf 9 6 802 1177 bf 9 6 828 1177 bf 8 6 933 1177 bf 9 6 976 1177 bf 8 6 994 1177 bf 9 7 236 1183 bf 8 7 245 1183 bf 8 7 428 1183 bf 9 7 436 1183 bf 9 7 445 1183 bf 8 7 454 1183 bf 9 7 462 1183
bf 9 7 471 1183 bf 9 7 480 1183 bf 9 7 497 1183 bf 8 7 515 1183 bf 9 7 523 1183 bf 9 7 532 1183 bf 9 7 541 1183 bf 9 7 689 1183 bf 8 7 698 1183 bf 9 7 706 1183 bf 9 7 715 1183 bf 8 7 724 1183 bf 9 7 732 1183 bf 9 7 741 1183 bf 9 7 750 1183 bf 9 7
776 1183 bf 9 7 802 1183 bf 8 7 811 1183 bf 9 7 924 1183 bf 9 7 941 1183 bf 9 7 950 1183 bf 9 7 967 1183 bf 8 7 245 1190 bf 9 7 419 1190 bf 8 7 428 1190 bf 9 7 436 1190 bf 9 7 445 1190 bf 8 7 454 1190 bf 9 7 462 1190 bf 9 7 471 1190 bf 8 7 489 1190
bf 9 7 497 1190 bf 9 7 506 1190 bf 8 7 515 1190 bf 9 7 523 1190 bf 9 7 558 1190 bf 8 7 576 1190 bf 8 7 637 1190 bf 9 7 671 1190 bf 9 7 689 1190 bf 8 7 698 1190 bf 9 7 706 1190 bf 9 7 715 1190 bf 8 7 724 1190 bf 9 7 732 1190 bf 9 7 750 1190 bf 9 7
767 1190 bf 9 7 793 1190 bf 9 7 915 1190 bf 8 7 933 1190 bf 9 7 941 1190 bf 9 7 950 1190 bf 9 7 985 1190 bf 8 7 994 1190 bf 8 7 245 1197 bf 9 7 410 1197 bf 9 7 419 1197 bf 8 7 428 1197 bf 9 7 436 1197 bf 9 7 445 1197 bf 8 7 454 1197 bf 9 7 462 1197
bf 9 7 471 1197 bf 9 7 480 1197 bf 9 7 497 1197 bf 8 7 515 1197 bf 9 7 523 1197 bf 9 7 532 1197 bf 8 7 637 1197 bf 9 7 645 1197 bf 9 7 654 1197 bf 9 7 671 1197 bf 9 7 680 1197 bf 9 7 689 1197 bf 8 7 698 1197 bf 9 7 706 1197 bf 9 7 715 1197 bf 9 7
732 1197 bf 9 7 741 1197 bf 8 7 846 1197 bf 9 7 880 1197 bf 8 7 907 1197 bf 9 7 915 1197 bf 9 7 924 1197 bf 8 7 994 1197 bf 8 6 245 1204 bf 9 6 253 1204 bf 9 6 401 1204 bf 9 6 410 1204 bf 9 6 419 1204 bf 8 6 428 1204 bf 9 6 436 1204 bf 9 6 445 1204
bf 8 6 454 1204 bf 9 6 462 1204 bf 8 6 489 1204 bf 9 6 497 1204 bf 9 6 506 1204 bf 9 6 558 1204 bf 9 6 628 1204 bf 8 6 637 1204 bf 9 6 645 1204 bf 9 6 654 1204 bf 8 6 663 1204 bf 9 6 671 1204 bf 9 6 680 1204 bf 9 6 689 1204 bf 9 6 715 1204 bf 9 6
863 1204 bf 8 6 872 1204 bf 9 6 898 1204 bf 8 6 907 1204 bf 9 6 924 1204 bf 9 6 950 1204 bf 8 6 959 1204 bf 9 7 253 1210 bf 8 7 393 1210 bf 9 7 401 1210 bf 9 7 410 1210 bf 9 7 419 1210 bf 8 7 428 1210 bf 9 7 436 1210 bf 9 7 445 1210 bf 8 7 454 1210
bf 9 7 462 1210 bf 9 7 471 1210 bf 9 7 480 1210 bf 8 7 489 1210 bf 9 7 523 1210 bf 9 7 593 1210 bf 8 7 602 1210 bf 9 7 610 1210 bf 9 7 619 1210 bf 9 7 628 1210 bf 8 7 637 1210 bf 9 7 645 1210 bf 9 7 654 1210 bf 8 7 663 1210 bf 9 7 671 1210 bf 9 7
680 1210 bf 9 7 689 1210 bf 9 7 828 1210 bf 9 7 837 1210 bf 8 7 846 1210 bf 9 7 863 1210 bf 9 7 880 1210 bf 9 7 889 1210 bf 8 7 907 1210 bf 9 7 924 1210 bf 9 7 253 1217 bf 9 7 262 1217 bf 8 7 393 1217 bf 9 7 401 1217 bf 9 7 410 1217 bf 9 7 419 1217
bf 8 7 428 1217 bf 9 7 436 1217 bf 9 7 445 1217 bf 8 7 454 1217 bf 9 7 462 1217 bf 8 7 489 1217 bf 9 7 506 1217 bf 8 7 515 1217 bf 9 7 584 1217 bf 9 7 593 1217 bf 8 7 602 1217 bf 9 7 610 1217 bf 9 7 619 1217 bf 9 7 628 1217 bf 8 7 637 1217 bf 9 7
645 1217 bf 9 7 654 1217 bf 9 7 776 1217 bf 9 7 828 1217 bf 9 7 863 1217 bf 9 7 262 1224 bf 9 7 384 1224 bf 8 7 393 1224 bf 9 7 401 1224 bf 9 7 410 1224 bf 9 7 419 1224 bf 8 7 428 1224 bf 9 7 436 1224 bf 9 7 445 1224 bf 8 7 454 1224 bf 9 7 462 1224
bf 9 7 471 1224 bf 9 7 480 1224 bf 8 7 576 1224 bf 9 7 584 1224 bf 9 7 593 1224 bf 8 7 602 1224 bf 9 7 610 1224 bf 9 7 619 1224 bf 9 7 628 1224 bf 8 7 637 1224 bf 9 7 645 1224 bf 8 7 663 1224 bf 9 7 715 1224 bf 9 7 802 1224 bf 8 7 811 1224 bf 9 7
819 1224 bf 8 7 846 1224 bf 9 6 262 1231 bf 9 6 384 1231 bf 8 6 393 1231 bf 9 6 401 1231 bf 9 6 410 1231 bf 9 6 419 1231 bf 9 6 436 1231 bf 9 6 445 1231 bf 8 6 454 1231 bf 9 6 462 1231 bf 8 6 489 1231 bf 8 6 515 1231 bf 9 6 567 1231 bf 9 6 584 1231
bf 9 6 593 1231 bf 8 6 602 1231 bf 9 6 610 1231 bf 9 6 619 1231 bf 8 6 637 1231 bf 9 6 776 1231 bf 9 6 802 1231 bf 8 6 811 1231 bf 9 6 819 1231 bf 9 7 262 1237 bf 9 7 271 1237 bf 9 7 375 1237 bf 9 7 384 1237 bf 8 7 393 1237 bf 9 7 401 1237 bf 9 7
410 1237 bf 9 7 419 1237 bf 8 7 428 1237 bf 9 7 462 1237 bf 9 7 471 1237 bf 9 7 532 1237 bf 9 7 558 1237 bf 9 7 567 1237 bf 8 7 576 1237 bf 9 7 584 1237 bf 9 7 593 1237 bf 9 7 610 1237 bf 9 7 628 1237 bf 9 7 645 1237 bf 9 7 671 1237 bf 9 7 689 1237
bf 8 7 724 1237 bf 9 7 741 1237 bf 9 7 750 1237 bf 9 7 767 1237 bf 9 7 776 1237 bf 8 7 785 1237 bf 9 7 802 1237 bf 9 7 828 1237 bf 9 7 271 1244 bf 9 7 297 1244 bf 8 7 367 1244 bf 9 7 375 1244 bf 9 7 384 1244 bf 8 7 393 1244 bf 9 7 401 1244 bf 9 7
410 1244 bf 9 7 419 1244 bf 9 7 436 1244 bf 8 7 454 1244 bf 9 7 471 1244 bf 8 7 489 1244 bf 9 7 523 1244 bf 8 7 550 1244 bf 9 7 558 1244 bf 9 7 567 1244 bf 8 7 576 1244 bf 9 7 584 1244 bf 9 7 593 1244 bf 8 7 602 1244 bf 8 7 724 1244 bf 9 7 732 1244
bf 8 7 759 1244 bf 9 7 767 1244 bf 9 7 776 1244 bf 9 7 793 1244 bf 9 7 271 1251 bf 8 7 280 1251 bf 8 7 367 1251 bf 9 7 375 1251 bf 9 7 384 1251 bf 8 7 393 1251 bf 9 7 401 1251 bf 9 7 410 1251 bf 9 7 419 1251 bf 9 7 436 1251 bf 8 7 454 1251 bf 8 7
550 1251 bf 9 7 558 1251 bf 9 7 567 1251 bf 8 7 576 1251 bf 9 7 584 1251 bf 9 7 619 1251 bf 9 7 628 1251 bf 8 7 724 1251 bf 9 7 732 1251 bf 9 7 741 1251 bf 9 7 750 1251 bf 9 7 767 1251 bf 8 7 785 1251 bf 8 6 280 1258 bf 8 6 367 1258 bf 9 6 375 1258
bf 9 6 384 1258 bf 8 6 393 1258 bf 9 6 401 1258 bf 9 6 410 1258 bf 9 6 419 1258 bf 8 6 428 1258 bf 9 6 445 1258 bf 9 6 462 1258 bf 9 6 480 1258 bf 9 6 532 1258 bf 9 6 541 1258 bf 8 6 550 1258 bf 9 6 558 1258 bf 9 6 567 1258 bf 8 6 576 1258 bf 9 6
584 1258 bf 9 6 619 1258 bf 9 6 680 1258 bf 9 6 689 1258 bf 8 6 698 1258 bf 9 6 706 1258 bf 9 6 715 1258 bf 8 6 724 1258 bf 9 6 732 1258 bf 9 6 741 1258 bf 8 7 280 1264 bf 9 7 288 1264 bf 9 7 297 1264 bf 9 7 358 1264 bf 8 7 367 1264 bf 9 7 375 1264
bf 9 7 384 1264 bf 8 7 393 1264 bf 9 7 401 1264 bf 9 7 410 1264 bf 8 7 428 1264 bf 9 7 436 1264 bf 9 7 506 1264 bf 9 7 523 1264 bf 9 7 532 1264 bf 9 7 541 1264 bf 8 7 550 1264 bf 9 7 558 1264 bf 8 7 576 1264 bf 9 7 680 1264 bf 9 7 689 1264 bf 8 7
698 1264 bf 8 7 759 1264 bf 9 7 288 1271 bf 9 7 358 1271 bf 8 7 367 1271 bf 9 7 375 1271 bf 9 7 384 1271 bf 8 7 393 1271 bf 9 7 410 1271 bf 9 7 419 1271 bf 8 7 428 1271 bf 9 7 471 1271 bf 9 7 506 1271 bf 8 7 515 1271 bf 9 7 523 1271 bf 9 7 532 1271
bf 9 7 541 1271 bf 8 7 550 1271 bf 9 7 567 1271 bf 8 7 663 1271 bf 9 7 671 1271 bf 9 7 680 1271 bf 8 7 698 1271 bf 9 7 706 1271 bf 9 7 715 1271 bf 9 7 732 1271 bf 9 7 750 1271 bf 9 7 288 1278 bf 9 7 349 1278 bf 9 7 358 1278 bf 8 7 367 1278 bf 9 7
375 1278 bf 8 7 393 1278 bf 9 7 401 1278 bf 9 7 497 1278 bf 9 7 506 1278 bf 8 7 515 1278 bf 9 7 532 1278 bf 8 7 550 1278 bf 9 7 654 1278 bf 9 7 671 1278 bf 9 7 689 1278 bf 8 7 698 1278 bf 9 7 706 1278 bf 9 7 750 1278 bf 9 6 288 1285 bf 9 6 297 1285
bf 9 6 349 1285 bf 9 6 358 1285 bf 8 6 367 1285 bf 9 6 375 1285 bf 9 6 384 1285 bf 9 6 419 1285 bf 8 6 428 1285 bf 9 6 436 1285 bf 9 6 506 1285 bf 8 6 515 1285 bf 9 6 523 1285 bf 9 6 532 1285 bf 9 6 541 1285 bf 9 6 645 1285 bf 9 6 654 1285 bf 8 6
663 1285 bf 9 6 671 1285 bf 9 6 680 1285 bf 9 7 297 1291 bf 9 7 349 1291 bf 9 7 358 1291 bf 8 7 367 1291 bf 9 7 375 1291 bf 9 7 384 1291 bf 9 7 401 1291 bf 9 7 410 1291 bf 8 7 489 1291 bf 9 7 497 1291 bf 9 7 506 1291 bf 8 7 515 1291 bf 9 7 523 1291
bf 9 7 541 1291 bf 8 7 550 1291 bf 9 7 619 1291 bf 8 7 637 1291 bf 8 7 663 1291 bf 8 7 698 1291 bf 9 7 297 1298 bf 8 7 306 1298 bf 9 7 349 1298 bf 9 7 358 1298 bf 8 7 367 1298 bf 9 7 375 1298 bf 9 7 384 1298 bf 9 7 410 1298 bf 8 7 454 1298 bf 9 7
480 1298 bf 8 7 489 1298 bf 9 7 497 1298 bf 9 7 506 1298 bf 8 7 515 1298 bf 9 7 541 1298 bf 9 7 619 1298 bf 9 7 628 1298 bf 8 7 637 1298 bf 9 7 645 1298 bf 8 7 663 1298 bf 8 7 306 1305 bf 8 7 341 1305 bf 9 7 349 1305 bf 9 7 358 1305 bf 8 7 367 1305
bf 9 7 375 1305 bf 8 7 393 1305 bf 9 7 401 1305 bf 9 7 471 1305 bf 9 7 480 1305 bf 8 7 489 1305 bf 9 7 497 1305 bf 9 7 506 1305 bf 9 7 523 1305 bf 8 7 602 1305 bf 9 7 610 1305 bf 9 7 619 1305 bf 9 7 628 1305 bf 8 6 306 1312 bf 9 6 349 1312 bf 9 6
358 1312 bf 8 6 367 1312 bf 9 6 384 1312 bf 8 6 393 1312 bf 9 6 436 1312 bf 9 6 471 1312 bf 9 6 480 1312 bf 8 6 489 1312 bf 9 6 497 1312 bf 9 6 506 1312 bf 8 6 602 1312 bf 9 6 610 1312 bf 9 6 619 1312 bf 8 6 637 1312 bf 9 6 654 1312 bf 9 7 314 1318
bf 8 7 341 1318 bf 9 7 349 1318 bf 9 7 358 1318 bf 9 7 375 1318 bf 9 7 462 1318 bf 9 7 471 1318 bf 9 7 480 1318 bf 8 7 489 1318 bf 9 7 497 1318 bf 8 7 515 1318 bf 9 7 584 1318 bf 9 7 593 1318 bf 8 7 602 1318 bf 9 7 628 1318 bf 9 7 645 1318 bf 9 7
776 1318 bf 8 7 785 1318 bf 9 7 314 1325 bf 8 7 341 1325 bf 9 7 349 1325 bf 9 7 358 1325 bf 9 7 375 1325 bf 9 7 384 1325 bf 9 7 471 1325 bf 9 7 480 1325 bf 9 7 497 1325 bf 9 7 523 1325 bf 8 7 602 1325 bf 9 7 610 1325 bf 9 7 628 1325 bf 9 7 314 1332
bf 9 7 323 1332 bf 8 7 341 1332 bf 9 7 349 1332 bf 9 7 358 1332 bf 9 7 375 1332 bf 9 7 384 1332 bf 8 7 393 1332 bf 9 7 401 1332 bf 8 7 454 1332 bf 9 7 471 1332 bf 9 7 480 1332 bf 8 7 489 1332 bf 8 7 576 1332 bf 9 7 584 1332 bf 9 7 593 1332 bf 9 7
680 1332 bf 8 7 811 1332 bf 9 6 323 1339 bf 9 6 332 1339 bf 8 6 341 1339 bf 9 6 349 1339 bf 9 6 358 1339 bf 9 6 419 1339 bf 9 6 445 1339 bf 9 6 462 1339 bf 9 6 471 1339 bf 8 6 489 1339 bf 8 6 576 1339 bf 9 6 593 1339 bf 9 6 619 1339 bf 9 7 323 1345
bf 9 7 332 1345 bf 8 7 341 1345 bf 9 7 349 1345 bf 8 7 367 1345 bf 9 7 384 1345 bf 8 7 454 1345 bf 9 7 462 1345 bf 9 7 558 1345 bf 9 7 567 1345 bf 8 7 576 1345 bf 9 7 593 1345 bf 9 7 332 1352 bf 8 7 341 1352 bf 9 7 349 1352 bf 9 7 358 1352 bf 8 7
367 1352 bf 9 7 375 1352 bf 9 7 445 1352 bf 8 7 454 1352 bf 9 7 462 1352 bf 8 7 489 1352 bf 9 7 567 1352 bf 8 7 576 1352 bf 9 7 584 1352 bf 9 7 593 1352 bf 9 7 332 1359 bf 8 7 341 1359 bf 9 7 349 1359 bf 8 7 367 1359 bf 9 7 384 1359 bf 9 7 419 1359
bf 9 7 436 1359 bf 9 7 445 1359 bf 8 7 454 1359 bf 9 7 541 1359 bf 9 7 558 1359 bf 9 6 332 1366 bf 8 6 341 1366 bf 9 6 375 1366 bf 9 6 384 1366 bf 9 6 436 1366 bf 9 6 445 1366 bf 8 6 454 1366 bf 9 6 462 1366 bf 8 7 341 1372 bf 9 7 349 1372 bf 9 7
358 1372 bf 9 7 436 1372 bf 9 7 445 1372 bf 9 7 462 1372 bf 9 7 558 1372 bf 8 7 341 1379 bf 9 7 349 1379 bf 8 7 367 1379 bf 9 7 384 1379 bf 8 7 393 1379 bf 9 7 419 1379 bf 8 7 428 1379 bf 9 7 436 1379 bf 9 7 445 1379 bf 8 7 454 1379 bf 9 7 462 1379
bf 9 7 532 1379 bf 9 7 541 1379 bf 9 7 349 1386 bf 9 7 358 1386 bf 8 7 367 1386 bf 9 7 384 1386 bf 8 7 428 1386 bf 9 7 436 1386 bf 9 7 445 1386 bf 8 7 454 1386 bf 9 7 532 1386 bf 8 7 550 1386 bf 9 7 558 1386 bf 9 6 349 1393 bf 9 6 358 1393 bf 9 6
375 1393 bf 8 6 428 1393 bf 9 6 436 1393 bf 9 7 358 1399 bf 9 7 410 1399 bf 8 7 428 1399 bf 9 7 506 1399 bf 8 7 515 1399 bf 9 7 523 1399 bf 9 7 532 1399 bf 9 7 358 1406 bf 8 7 367 1406 bf 9 7 375 1406 bf 9 7 401 1406 bf 9 7 419 1406 bf 8 7 428 1406
bf 9 7 506 1406 bf 8 7 515 1406 bf 9 7 584 1406 bf 9 7 358 1413 bf 8 7 367 1413 bf 9 7 375 1413 bf 9 7 419 1413 bf 9 7 445 1413 bf 8 7 454 1413 bf 9 7 497 1413 bf 9 7 506 1413 bf 8 7 515 1413 bf 8 6 367 1420 bf 9 6 410 1420 bf 9 6 419 1420 bf 8 6
489 1420 bf 9 6 497 1420 bf 8 6 515 1420 bf 9 6 793 1420 bf 8 7 367 1426 bf 9 7 375 1426 bf 9 7 410 1426 bf 9 7 419 1426 bf 8 7 428 1426 bf 9 7 436 1426 bf 8 7 489 1426 bf 9 7 523 1426 bf 9 7 375 1433 bf 8 7 393 1433 bf 9 7 410 1433 bf 9 7 419 1433
bf 9 7 497 1433 bf 9 7 375 1440 bf 9 7 410 1440 bf 9 7 419 1440 bf 9 7 480 1440 bf 8 7 489 1440 bf 9 7 506 1440 bf 9 6 375 1447 bf 9 6 384 1447 bf 9 6 401 1447 bf 9 6 410 1447 bf 9 6 419 1447 bf 8 6 489 1447 bf 9 7 384 1453 bf 9 7 410 1453 bf 9 7
419 1453 bf 9 7 462 1453 bf 8 7 576 1453 bf 9 7 384 1460 bf 8 7 393 1460 bf 9 7 401 1460 bf 9 7 480 1460 bf 8 7 393 1467 bf 9 7 401 1467 bf 9 7 410 1467 bf 9 7 471 1467 bf 8 6 393 1474 bf 9 6 401 1474 bf 9 6 462 1474 bf 9 6 471 1474 bf 9 7 401 1480
bf 9 7 462 1480 bf 9 7 480 1480 bf 9 7 401 1487 bf 9 7 410 1487 bf 9 7 419 1487 bf 9 7 462 1487 bf 9 7 471 1487 bf 9 7 828 1487 bf 9 7 410 1494 bf 9 6 410 1501 bf 8 6 454 1501 bf 9 7 410 1507 bf 9 7 419 1507 bf 8 7 454 1507 bf 9 7 471 1507 bf 9 7
480 1507 bf 9 7 419 1514 bf 9 7 436 1514 bf 8 7 454 1514 bf 9 7 462 1514 bf 9 7 419 1521 bf 8 7 454 1521 bf 9 7 462 1521 bf 8 6 428 1528 bf 8 6 454 1528 bf 8 7 428 1534 bf 9 7 445 1534 bf 8 7 428 1541 bf 9 7 436 1541 bf 9 7 445 1541 bf 9 7 436 1548
bf 9 6 436 1555 bf 9 6 445 1555 bf 9 7 445 1561 bf 8 7 454 1561 bf 9 7 445 1568 bf 8 7 454 1575 bf 8 6 454 1582 bf 8 7 454 1588 bf 9 7 462 1588 bf 9 7 462 1595 bf 9 7 462 1602 bf 9 7 471 1602 bf 9 6 471 1609 bf 9 7 471 1615 bf 9 7 480 1622 bf 9 7
480 1629 bf 8 7 489 1629 bf 9 6 506 1636 bf 8 7 489 1642 bf 8 7 489 1649 bf 1 1 1 c black 132 981 m 870 X s
gsave 1088 844 23 896 C 569.206 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 1001 m -20 Y s 149 991 m -10 Y s 166 991 m -10 Y s 184 991 m -10 Y s 201 991 m -10 Y s 219 1001 m -20 Y s 236 991 m
-10 Y s 253 991 m -10 Y s 271 991 m -10 Y s 288 991 m -10 Y s 306 1001 m -20 Y s 323 991 m -10 Y s 341 991 m -10 Y s 358 991 m -10 Y s 375 991 m -10 Y s 393 1001 m -20 Y s 410 991 m -10 Y s 428 991 m -10 Y s 445 991 m -10 Y s 462 991 m -10 Y s 480
1001 m -20 Y s 497 991 m -10 Y s 515 991 m -10 Y s 532 991 m -10 Y s 550 991 m -10 Y s 567 1001 m -20 Y s 584 991 m -10 Y s 602 991 m -10 Y s 619 991 m -10 Y s 637 991 m -10 Y s 654 1001 m -20 Y s 671 991 m -10 Y s 689 991 m -10 Y s 706 991 m -10 Y
s 724 991 m -10 Y s 741 1001 m -20 Y s 759 991 m -10 Y s 776 991 m -10 Y s 793 991 m -10 Y s 811 991 m -10 Y s 828 1001 m -20 Y s 846 991 m -10 Y s 863 991 m -10 Y s 880 991 m -10 Y s 898 991 m -10 Y s 915 1001 m -20 Y s 933 991 m -10 Y s 950 991 m
-10 Y s 967 991 m -10 Y s 985 991 m -10 Y s 1002 1001 m -20 Y s
gsave 1088 844 23 896 C 120.672 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 182.146 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 268.665 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 355.185 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 441.704 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 23 896 C 530.5 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 23 896 C 617.019 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 23 896 C 703.539 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 23 896 C 790.058 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 23 896 C 876.577 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 23 896 C 956.266 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 1656 m 870 X s 132 1636 m 20 Y s 149 1646 m 10 Y s 166 1646 m 10 Y s 184 1646 m 10 Y s 201 1646 m 10 Y s 219 1636 m 20 Y s 236 1646 m 10
Y s 253 1646 m 10 Y s 271 1646 m 10 Y s 288 1646 m 10 Y s 306 1636 m 20 Y s 323 1646 m 10 Y s 341 1646 m 10 Y s 358 1646 m 10 Y s 375 1646 m 10 Y s 393 1636 m 20 Y s 410 1646 m 10 Y s 428 1646 m 10 Y s 445 1646 m 10 Y s 462 1646 m 10 Y s 480 1636 m
20 Y s 497 1646 m 10 Y s 515 1646 m 10 Y s 532 1646 m 10 Y s 550 1646 m 10 Y s 567 1636 m 20 Y s 584 1646 m 10 Y s 602 1646 m 10 Y s 619 1646 m 10 Y s 637 1646 m 10 Y s 654 1636 m 20 Y s 671 1646 m 10 Y s 689 1646 m 10 Y s 706 1646 m 10 Y s 724 1646
m 10 Y s 741 1636 m 20 Y s 759 1646 m 10 Y s 776 1646 m 10 Y s 793 1646 m 10 Y s 811 1646 m 10 Y s 828 1636 m 20 Y s 846 1646 m 10 Y s 863 1646 m 10 Y s 880 1646 m 10 Y s 898 1646 m 10 Y s 915 1636 m 20 Y s 933 1646 m 10 Y s 950 1646 m 10 Y s 967
1646 m 10 Y s 985 1646 m 10 Y s 1002 1636 m 20 Y s 132 981 m 675 Y s
gsave 1088 844 23 896 C 54.6438 1400.25 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 158 981 m -26 X s 145 997 m -13 X s 145 1013 m -13 X s 145 1029 m -13 X s 145 1045 m -13 X s 158 1061 m -26 X s 145 1077 m -13 X
s 145 1093 m -13 X s 145 1109 m -13 X s 145 1125 m -13 X s 158 1142 m -26 X s 145 1158 m -13 X s 145 1174 m -13 X s 145 1190 m -13 X s 145 1206 m -13 X s 158 1222 m -26 X s 145 1238 m -13 X s 145 1254 m -13 X s 145 1270 m -13 X s 145 1286 m -13 X s
158 1302 m -26 X s 145 1318 m -13 X s 145 1334 m -13 X s 145 1350 m -13 X s 145 1366 m -13 X s 158 1383 m -26 X s 145 1399 m -13 X s 145 1415 m -13 X s 145 1431 m -13 X s 145 1447 m -13 X s 158 1463 m -26 X s 145 1479 m -13 X s 145 1495 m -13 X s
145 1511 m -13 X s 145 1527 m -13 X s 158 1543 m -26 X s 145 1559 m -13 X s 145 1575 m -13 X s 145 1591 m -13 X s 145 1608 m -13 X s 158 1624 m -26 X s 158 1624 m -26 X s 145 1640 m -13 X s 145 1656 m -13 X s
gsave 1088 844 23 896 C 107.011 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 72.8584 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 844 23 896 C 54.6438 1129.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 54.6438 1208.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 844 23 896 C 54.6438 1288.68 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 54.6438 1370.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 844 23 896 C 54.6438 1450.34 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 54.6438 1530.03 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 844 23 896 C 54.6438 1611.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 1002 981 m 675 Y s 976 981 m 26 X s 989 997 m 13 X s 989 1013 m 13 X s 989 1029 m 13 X s 989 1045 m 13 X s 976 1061 m 26 X s 989 1077 m 13 X
s 989 1093 m 13 X s 989 1109 m 13 X s 989 1125 m 13 X s 976 1142 m 26 X s 989 1158 m 13 X s 989 1174 m 13 X s 989 1190 m 13 X s 989 1206 m 13 X s 976 1222 m 26 X s 989 1238 m 13 X s 989 1254 m 13 X s 989 1270 m 13 X s 989 1286 m 13 X s 976 1302 m 26
X s 989 1318 m 13 X s 989 1334 m 13 X s 989 1350 m 13 X s 989 1366 m 13 X s 976 1383 m 26 X s 989 1399 m 13 X s 989 1415 m 13 X s 989 1431 m 13 X s 989 1447 m 13 X s 976 1463 m 26 X s 989 1479 m 13 X s 989 1495 m 13 X s 989 1511 m 13 X s 989 1527 m
13 X s 976 1543 m 26 X s 989 1559 m 13 X s 989 1575 m 13 X s 989 1591 m 13 X s 989 1608 m 13 X s 976 1624 m 26 X s 976 1624 m 26 X s 989 1640 m 13 X s 989 1656 m 13 X s 0.386667 0 1 c 49 34 1008 981 bf 0.2 0 1 c 49 33 1008 1015 bf 0 0.0800001 1 c 49
34 1008 1048 bf 0 0.266667 1 c 49 34 1008 1082 bf 0 0.546666 1 c 49 34 1008 1116 bf 0 0.733333 1 c 49 33 1008 1150 bf 0 1 0.986667 c 49 34 1008 1183 bf 0 1 0.8 c 49 34 1008 1217 bf 0 1 0.52 c 49 34 1008 1251 bf 0 1 0.333333 c 49 33 1008 1285 bf 0 1
0.0533333 c 49 34 1008 1318 bf 0.133333 1 0 c 49 34 1008 1352 bf 0.413333 1 0 c 49 34 1008 1386 bf 0.6 1 0 c 49 33 1008 1420 bf 0.88 1 0 c 49 34 1008 1453 bf 1 0.933333 0 c 49 34 1008 1487 bf 1 0.653333 0 c 49 34 1008 1521 bf 1 0.466667 0 c 49 33
1008 1555 bf 1 0.186667 0 c 49 34 1008 1588 bf 1 0 0 c 49 34 1008 1622 bf black 1057 981 m 675 Y s 1031 981 m 26 X s 1031 1061 m 26 X s 1031 1142 m 26 X s 1031 1222 m 26 X s 1031 1303 m 26 X s 1031 1383 m 26 X s 1031 1464 m 26 X s 1031 1544 m 26 X s
1031 1624 m 26 X s 1031 1624 m 26 X s
gsave 1088 844 23 896 C 1061 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 1061 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2) show NC gr
gsave 1088 844 23 896 C 1061 1129.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4) show NC gr
gsave 1088 844 23 896 C 1061 1208.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6) show NC gr
gsave 1088 844 23 896 C 1061 1290.96 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8) show NC gr
gsave 1088 844 23 896 C 1061 1370.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 844 23 896 C 1061 1450.34 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (12) show NC gr
gsave 1088 844 23 896 C 1061 1532.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (14) show NC gr
gsave 1088 844 23 896 C 1061 1611.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (16) show NC gr
gsave 1088 844 23 896 C 1108.81 1678.02 t 0 r /Helvetica-Bold findfont 20.5224 sf 0 0 m (6) show NC gr
gsave 1088 844 23 896 C 1074.66 1659.8 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 844 23 896 C 1056.45 1659.8 t 0 r /Symbol findfont 31.9238 sf 0 0 m (<EFBFBD>) show NC gr 1 1 1 c 240 47 34 1689 bf black 34 1689 m 240 X s 274 1689 m 47 Y s 274 1736 m -240 X s 34 1736 m -47 Y s 1 1 1 c black
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gsave 1088 844 1157 896 C 1254.53 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
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gsave 1088 844 1157 896 C 1402.52 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 1157 896 C 1489.04 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 1157 896 C 1575.56 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 1157 896 C 1664.36 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
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gsave 1088 844 1157 896 C 1923.92 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 1157 896 C 2010.44 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 1157 896 C 2090.12 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 1265 1656 m 871 X s 1265 1636 m 20 Y s 1283 1646 m 10 Y s 1300 1646 m 10 Y s 1318 1646 m 10 Y s 1335 1646 m 10 Y s 1352 1636 m 20 Y s 1370
1646 m 10 Y s 1387 1646 m 10 Y s 1405 1646 m 10 Y s 1422 1646 m 10 Y s 1440 1636 m 20 Y s 1457 1646 m 10 Y s 1474 1646 m 10 Y s 1492 1646 m 10 Y s 1509 1646 m 10 Y s 1527 1636 m 20 Y s 1544 1646 m 10 Y s 1561 1646 m 10 Y s 1579 1646 m 10 Y s 1596
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gsave 1088 843 23 18 C 569.206 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 122 m -20 Y s 149 112 m -10 Y s 166 112 m -10 Y s 184 112 m -10 Y s 201 112 m -10 Y s 219 122 m -20 Y s 236 112 m -10 Y
s 253 112 m -10 Y s 271 112 m -10 Y s 288 112 m -10 Y s 306 122 m -20 Y s 323 112 m -10 Y s 341 112 m -10 Y s 358 112 m -10 Y s 375 112 m -10 Y s 393 122 m -20 Y s 410 112 m -10 Y s 428 112 m -10 Y s 445 112 m -10 Y s 462 112 m -10 Y s 480 122 m -20
Y s 497 112 m -10 Y s 515 112 m -10 Y s 532 112 m -10 Y s 550 112 m -10 Y s 567 122 m -20 Y s 584 112 m -10 Y s 602 112 m -10 Y s 619 112 m -10 Y s 637 112 m -10 Y s 654 122 m -20 Y s 671 112 m -10 Y s 689 112 m -10 Y s 706 112 m -10 Y s 724 112 m
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m -10 Y s 985 112 m -10 Y s 1002 122 m -20 Y s
gsave 1088 843 23 18 C 120.672 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 23 18 C 182.146 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 23 18 C 268.665 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 23 18 C 355.185 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 23 18 C 441.704 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 843 23 18 C 530.5 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 843 23 18 C 617.019 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 843 23 18 C 703.539 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 843 23 18 C 790.058 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 843 23 18 C 876.577 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 843 23 18 C 956.266 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 777 m 870 X s 132 757 m 20 Y s 149 767 m 10 Y s 166 767 m 10 Y s 184 767 m 10 Y s 201 767 m 10 Y s 219 757 m 20 Y s 236 767 m 10 Y s 253
767 m 10 Y s 271 767 m 10 Y s 288 767 m 10 Y s 306 757 m 20 Y s 323 767 m 10 Y s 341 767 m 10 Y s 358 767 m 10 Y s 375 767 m 10 Y s 393 757 m 20 Y s 410 767 m 10 Y s 428 767 m 10 Y s 445 767 m 10 Y s 462 767 m 10 Y s 480 757 m 20 Y s 497 767 m 10 Y
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102 m 675 Y s
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214 m -13 X s 145 231 m -13 X s 145 247 m -13 X s 158 263 m -26 X s 145 279 m -13 X s 145 295 m -13 X s 145 311 m -13 X s 145 327 m -13 X s 158 343 m -26 X s 145 359 m -13 X s 145 375 m -13 X s 145 391 m -13 X s 145 407 m -13 X s 158 423 m -26 X s
145 439 m -13 X s 145 455 m -13 X s 145 472 m -13 X s 145 488 m -13 X s 158 504 m -26 X s 145 520 m -13 X s 145 536 m -13 X s 145 552 m -13 X s 145 568 m -13 X s 158 584 m -26 X s 145 600 m -13 X s 145 616 m -13 X s 145 632 m -13 X s 145 648 m -13 X
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gsave 1088 843 23 18 C 107.011 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
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214 m 13 X s 989 231 m 13 X s 989 247 m 13 X s 976 263 m 26 X s 989 279 m 13 X s 989 295 m 13 X s 989 311 m 13 X s 989 327 m 13 X s 976 343 m 26 X s 989 359 m 13 X s 989 375 m 13 X s 989 391 m 13 X s 989 407 m 13 X s 976 423 m 26 X s 989 439 m 13 X
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13 X s 989 697 m 13 X s 989 713 m 13 X s 989 729 m 13 X s 976 745 m 26 X s 976 745 m 26 X s 989 761 m 13 X s 989 777 m 13 X s 0.386667 0 1 c 49 34 1008 102 bf 0.2 0 1 c 49 33 1008 136 bf 0 0.0800001 1 c 49 34 1008 169 bf 0 0.266667 1 c 49 34 1008
203 bf 0 0.546666 1 c 49 34 1008 237 bf 0 0.733333 1 c 49 33 1008 271 bf 0 1 0.986667 c 49 34 1008 304 bf 0 1 0.8 c 49 34 1008 338 bf 0 1 0.52 c 49 34 1008 372 bf 0 1 0.333333 c 49 33 1008 406 bf 0 1 0.0533333 c 49 34 1008 439 bf 0.133333 1 0 c 49
34 1008 473 bf 0.413333 1 0 c 49 34 1008 507 bf 0.6 1 0 c 49 33 1008 541 bf 0.88 1 0 c 49 34 1008 574 bf 1 0.933333 0 c 49 34 1008 608 bf 1 0.653333 0 c 49 34 1008 642 bf 1 0.466667 0 c 49 33 1008 676 bf 1 0.186667 0 c 49 34 1008 709 bf 1 0 0 c 49
34 1008 743 bf black 1057 102 m 675 Y s 1031 102 m 26 X s 1031 174 m 26 X s 1031 246 m 26 X s 1031 317 m 26 X s 1031 389 m 26 X s 1031 461 m 26 X s 1031 533 m 26 X s 1031 605 m 26 X s 1031 676 m 26 X s 1031 748 m 26 X s 1031 748 m 26 X s
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gsave 1088 843 23 18 C 1061 232.236 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
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gsave 1088 843 23 18 C 1061 448.534 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (25) show NC gr
gsave 1088 843 23 18 C 1061 519.116 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (30) show NC gr
gsave 1088 843 23 18 C 1061 591.974 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (35) show NC gr
gsave 1088 843 23 18 C 1061 664.833 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (40) show NC gr
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675 1265 102 bl 1 1 1 c 0 0.733333 1 c 9 7 1265 102 bf 0 0.546666 1 c 9 6 1265 109 bf 0.2 0 1 c 9 7 1265 115 bf 0 0.0800001 1 c 9 7 1274 115 bf 0.386667 0 1 c 8 7 1292 115 bf 9 7 1605 115 bf 0 0.733333 1 c 9 7 1274 122 bf 0 0.266667 1 c 9 7 1274 129
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gsave 1088 843 1157 18 C 1703.06 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 1265 122 m -20 Y s 1283 112 m -10 Y s 1300 112 m -10 Y s 1318 112 m -10 Y s 1335 112 m -10 Y s 1352 122 m -20 Y s 1370
112 m -10 Y s 1387 112 m -10 Y s 1405 112 m -10 Y s 1422 112 m -10 Y s 1440 122 m -20 Y s 1457 112 m -10 Y s 1474 112 m -10 Y s 1492 112 m -10 Y s 1509 112 m -10 Y s 1527 122 m -20 Y s 1544 112 m -10 Y s 1561 112 m -10 Y s 1579 112 m -10 Y s 1596
112 m -10 Y s 1614 122 m -20 Y s 1631 112 m -10 Y s 1649 112 m -10 Y s 1666 112 m -10 Y s 1683 112 m -10 Y s 1701 122 m -20 Y s 1718 112 m -10 Y s 1736 112 m -10 Y s 1753 112 m -10 Y s 1770 112 m -10 Y s 1788 122 m -20 Y s 1805 112 m -10 Y s 1823
112 m -10 Y s 1840 112 m -10 Y s 1858 112 m -10 Y s 1875 122 m -20 Y s 1892 112 m -10 Y s 1910 112 m -10 Y s 1927 112 m -10 Y s 1945 112 m -10 Y s 1962 122 m -20 Y s 1979 112 m -10 Y s 1997 112 m -10 Y s 2014 112 m -10 Y s 2032 112 m -10 Y s 2049
122 m -20 Y s 2067 112 m -10 Y s 2084 112 m -10 Y s 2101 112 m -10 Y s 2119 112 m -10 Y s 2136 122 m -20 Y s
gsave 1088 843 1157 18 C 1254.53 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 1157 18 C 1316 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 1157 18 C 1402.52 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 1157 18 C 1489.04 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 1157 18 C 1575.56 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 843 1157 18 C 1664.36 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 843 1157 18 C 1750.88 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 843 1157 18 C 1837.4 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 843 1157 18 C 1923.92 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 843 1157 18 C 2010.44 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 843 1157 18 C 2090.12 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 1265 777 m 871 X s 1265 757 m 20 Y s 1283 767 m 10 Y s 1300 767 m 10 Y s 1318 767 m 10 Y s 1335 767 m 10 Y s 1352 757 m 20 Y s 1370 767 m
10 Y s 1387 767 m 10 Y s 1405 767 m 10 Y s 1422 767 m 10 Y s 1440 757 m 20 Y s 1457 767 m 10 Y s 1474 767 m 10 Y s 1492 767 m 10 Y s 1509 767 m 10 Y s 1527 757 m 20 Y s 1544 767 m 10 Y s 1561 767 m 10 Y s 1579 767 m 10 Y s 1596 767 m 10 Y s 1614 757
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gsave 1088 843 1157 18 C 1188.5 521.393 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 1292 102 m -27 X s 1278 118 m -13 X s 1278 134 m -13 X s 1278 150 m -13 X s 1278 166 m -13 X s 1292 182 m -27 X s 1278 198 m -13
X s 1278 214 m -13 X s 1278 231 m -13 X s 1278 247 m -13 X s 1292 263 m -27 X s 1278 279 m -13 X s 1278 295 m -13 X s 1278 311 m -13 X s 1278 327 m -13 X s 1292 343 m -27 X s 1278 359 m -13 X s 1278 375 m -13 X s 1278 391 m -13 X s 1278 407 m -13 X
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gsave 1088 843 1157 18 C 1240.87 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 1157 18 C 1206.72 170.762 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 843 1157 18 C 1188.5 250.451 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 1157 18 C 1188.5 330.139 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 843 1157 18 C 1188.5 409.828 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 1157 18 C 1188.5 491.794 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 843 1157 18 C 1188.5 571.483 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 1157 18 C 1188.5 651.172 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 843 1157 18 C 1188.5 733.137 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 2136 102 m 675 Y s 2110 102 m 26 X s 2123 118 m 13 X s 2123 134 m 13 X s 2123 150 m 13 X s 2123 166 m 13 X s 2110 182 m 26 X s 2123 198 m 13
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\documentclass[12pt]{article}
\usepackage{latexsym,multicol,graphicx,rotating}
\usepackage{hyperref}
\usepackage{booktabs}
\usepackage{tabularx}
\usepackage{color}
\usepackage[affil-it]{authblk}
\hypersetup{
colorlinks = false,
linkcolor = red,
linktoc=page,
linkbordercolor={1 0 0}
%linkcolor=blue,
}
%%%%%%%%%%%%% user's command definitions
%\setlength{\textwidth}{16cm}
\newcommand{\ttbs}{\char'134}
\newcommand{\AmS}{{\protect\the\textfont2
A\kern-.1667em\lower.5ex\hbox{M}\kern-.125emS}}
\newcommand{\lagr}{\cal{L}}
\newcommand{\mueg}{$\mu^{+} \rightarrow e^{+}\gamma$~}
\newcommand{\meee}{$\mu \rightarrow eee$~}
\newcommand{\muenn}{$\mu \rightarrow e \nu \overline{\nu}$~}
\newcommand{\muenng}{$\mu \rightarrow e \nu \overline{\nu} \gamma$~}
\newcommand{\muec}{$\mu^{-} N \rightarrow e^{-} N$~}
\makeatletter
\def\@maketitle{%
\newpage
\null
\vskip 2em%
\begin{center}%
\let \footnote \thanks
{\Large\bfseries \@title \par}%
\vskip 1.5em%
{\normalsize
\lineskip .5em%
\begin{tabular}[t]{c}%
\@author
\end{tabular}\par}%
\vskip 1em%
{\normalsize \@date}%
\end{center}%
\par
\vskip 1.5em}
\makeatother
%%%%%%%%%%%%%%%%%%%%%%%%%%% Begin
\begin{document}
\title{Proposal \\
Measurements of Muon Nuclear Capture
\\on Aluminum to Study Background for \\
Muon to Electron Conversion Experiments}
\author[1]{Peter Kammel \thanks{pkammel@uw.edu}}
\author[2]{Yoshitaka Kuno \thanks{kuno@phys.sci.osaka-u.ac.jp}}
\affil[1]{University of Washington}
\affil[2]{Osaka University}
\maketitle
\newpage
%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{abstract}
The recent observation that neutrinos oscillate and change flavour and so have
mass requires an extension to the SM and demonstrates that lepton flavour is
not an absolutely conserved quantity. However, even in this minimal extension
to the SM, accommodating neutrino masses, the rate of charged lepton flavour
violating (CLFV) interactions is predicted to be $O(10^{-54})$, and is far too
small to be observed. As such, any experimental observation of CLFV
would be a clear evidence of new physics beyond the SM.
Two new projects have been established to search for a CLFV process,
$\mu^-N\rightarrow e^-N$ conversion. They are Mu2e experiment at FNAL and the
COMET experiment at J-PARC. The two experiments will both utilise multi-kW
pulsed 8$-$9 GeV proton beams to achieve a branching ratio sensitivities lower
than 10$^{-16}$, that is 10,000 better than current best limit established by
SINDRUM II. Both COMET Phase-I and Mu2e will be subject to significant
backgrounds from the products of the nuclear capture process. Among them, the
background for protons is a particularly acute one, and its detailed
investigation is the subject of this proposal, which is a joint proposal on
behalf of both the Mu2e and COMET collaborations.
The goal of the experiment is to measure the rate and energy spectra of the
charged particles emitted after a muon is captured on aluminum, silicon and
titanium targets. A precision of 5\% down to an energy of 2.5 MeV is required
for both the rate and the energy spectra. Thin targets and a high quality, low
energy muon beam with a small momentum spread are essential for the experiment
so that a high rate of stopped muons can be achieved, and so that the charged
particles do not lose a significant amount of energy in the target - a main
difficulty that prevents any relevant measurements on these targets.
\end{abstract}
\newpage
%%%%%%%%%%%%%%%%%%%%%%%%%%% TOC
\tableofcontents
\newpage
%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Beam requirements and Beam request}
\label{sec:beamrequest}
Experimental area: $\pi$E1 beam line
\noindent Required beam properties:
\begin{itemize}
\item Particle: $\mu^-$
\item Momentum: 30 MeV/c
\item Momentum width: 1.9 \% FWHM
\item Beam spot: maximum 5 cm in diameter \textcolor{red}{(?)}
\item Intensity: $5 \times 10^{4}$ s$^{-1}$
\item Beam purity: \textcolor{red}{???}
\end{itemize}
\noindent Duration of the experiment: we are requesting three weeks of
measurements, with details:
\begin{itemize}
\item 2 days for setting up the equipments,
\item 5 days for beam tuning and adjustment of data aquisition system,
\item 7$\times$2 days for data taking with two different targets, this is
based on the estimated rate of protons shown in Table~\ref{tb:rates} and we
want to have at least $10^5$ events for each sample.
\end{itemize}
\newpage
%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Declaration of hazardous materials and equipments} % (fold)
\label{sec:safety}
%Declaration sheet of hazardous materials, still need detailed description in
%the full text ,though.
\begin{enumerate}
\item Radiation: some calibration sources will be used, there is no dangerous
radioactivity involved.
\item High voltages: low current high voltages will be used, all HV cables
are concealed within commercial HV supply units, cables and SHV connectors.
\item Fire and explosion: no explosive material will be used in the
experiment.
\item Cryogenic apparatus: liquid nitrogen will be used for the Ge detector,
standard precautions will be taken.
\end{enumerate}
\newpage
% section safety (end)
%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Physics motivation} % (fold)
\label{sec:motivation}
\subsection{Introduction}
It is known that quarks and neutrinos are mixed and therefore their
flavors are not conserved in the Standard Model (SM). However, lepton
flavor violation for charged leptons has not yet been observed. In
the minimal version of the SM where massless neutrinos are assumed,
lepton flavor conservation is a natural consequence of the gauge
invariance. Therefore, it has been considered to naively explain why
charged lepton flavor violation (CLFV) is highly suppressed. More
recently, the observation of neutrino oscillations has demonstrated
that neutrinos are massive and mixed among different neutrino flavor
species. Therefore, lepton flavor for neutrinos is known to be
violated.
In the framework of the Standard Model (SM) with massive neutrinos and their
mixing, the branching ratio of $\mu\rightarrow e\gamma$ decay can be estimated.
This process is suppressed by the GIM mechanism and the estimated branching
ratio is tiny, about $O(10^{-54})$ As a result, the observation of CLFV would
indicate a clear signal of new physics beyond the SM. The discovery of CLFV is
considered to be one of the important subjects in elementary particle
physics~\cite{Kuno:1999jp}.
CLFV is known to be sensitive to various extension of new physics beyond the
SM. Among them, a well-motivated physics model is a supersymmetric (SUSY)
model. In SUSY models, the slepton mixing (given by off-diagonal elements of
the slepton mass matrix) would introduce CLFV. In the minimum SUSY scenario,
the slepton mass matrix is assumed to be diagonal at the Planck scale. At a low
energy scale, new physics phenomena such as grand-unification (GUT) or neutrino
seesaw would introduce off-diagonal matrix elements such as $\Delta
m_{\tilde{\mu}\tilde{e}}$ through quantum corrections (renormalization).
Therefore, the slepon mixing is sensitive to GUT (at $10^{16}$ GeV) or neutrino
seesaw mechanism (at $10^{13-14}$ GeV). As a result, CLFV has potential to
study physics at very high energy scale.
A prominent muon CLFV processes is coherent neutrino-less conversion of a
negative muon to an electron (\muec conversion) in a muonic atom. When a
negative muon is stopped in material, it is trapped by an atom, and a muonic
atom is formed. After it cascades down energy levels in the muonic atom, the
muon is bound in its 1{\em s} ground state. The fate of the muon is then either
decay in orbit (DIO) ($\mu^{-} \rightarrow e^{-}\nu_{\mu} \overline{\nu}_{e}$)
or nuclear muon capture by a nucleus $N(A,Z)$ of mass number $A$ and atomic
number $Z$, namely, $\mu^{-} + N(A,Z) \rightarrow \nu_{\mu} + N(A,Z-1)$.
However, in the context of lepton flavor violation in physics beyond the
Standard Model, the exotic process of neutrino-less muon capture, such as
%
\begin{equation} \mu^{-} + N(A,Z) \rightarrow e^{-} + N(A,Z), \end{equation}
%
is also expected. This process is called \muec conversion in a muonic atom.
This process violates the conservation of lepton flavor numbers, $L_{e}$ and
$L_{\mu}$, by one unit, but the total lepton number, $L$, is conserved.
The event signature of coherent \muec conversion in a muonic atom is a
mono-energetic single electron emitted from the conversion with an energy
($E_{\mu e}$) of $E_{\mu e} = m_{\mu} - B_{\mu} - E_{recoil}$, where $m_{\mu}$
is the muon mass, and $B_{\mu}$ is the binding energy of the 1$s$ muonic atom.
$E_{recoil}$ is the nuclear recoil energy which is small and can be ignored.
Since $B_{\mu}$ varies for various nuclei, $E_{\mu e}$ could be different. For
instance, $E_{\mu e} = 104.9$ MeV for aluminum (Al) and $E_{\mu e}$ = 104.3 MeV
for titanium (Ti).
From an experimental point of view, \muec conversion is a very attractive
process: Firstly, the energy of the signal electron of about 105 MeV is far
above the end-point energy of the normal muon decay spectrum ($\sim$ 52.8 MeV).
Secondly, since the event signature is a mono-energetic electron, no
coincidence measurement is required. The search for this process has the
potential to improve sensitivity by using a high muon rate without suffering
from accidental background events, which would be serious for other processes,
such as $\mu\rightarrow e\gamma$ and $\mu\rightarrow eee$ decays.
The previous search for \muec conversion was performed by the SINDRUM II
collaboration at PSI. The SINDRUM II spectrometer consisted of a set of
concentric cylindrical drift chambers inside a superconducting solenoid magnet
of 1.2 Tesla. They set an upper limit of \muec in Au of $B(\mu^{-} + Au
\rightarrow e^{-} + Au) < 7 \times 10^{-13}$.
\begin{figure}[htb]
%\vspace{-40mm}
\centering
\includegraphics[width=\textwidth]{figs/comet-mu2e}
\caption{Schematic layouts of the Mu2e (left) and the COMET (right).}
\label{fg:mu2ecomet}
%\vspace{-5mm}
\end{figure}
New experimental projects to search for \muec conversion with a higher
sensitivity are being pursued in the USA and Japan. The proposal in
the USA is the Mu2e experiment at FNAL~\cite{mu2e08}. It is aiming to
search for \muec conversion at a sensitivity of better than
$10^{-16}$. Figure~\ref{fg:mu2ecomet}(left) shows its proposed layout.
It consists of the production solenoid system, the transport solenoid system
and the detector solenoid system. The Mu2e experiment is planned to combat
beam-related background events with the help of a 8 GeV/$c$ bunched proton
beam of about 8 kW in beam power at FNAL. The detector solenoid is a straight
solenoid and therefore both positive and negative charged particles from the
target enter the detector. The Mu2e experiment was approved at FNAL PAC in
2009 and obtained the DOE CD-0 approval. Right now the Mu2e collaboration is
working on CD-1.
The other experimental proposal to search for \muec conversion, which is called
COMET (COherent Muon to Electron Transition), is being prepared at the Japan
Proton Accelerator Research Complex (J-PARC), Tokai, Japan~\cite{come07}. The
aimed sensitivity at COMET is similar to Mu2e, namely better than $10^{-16}$. A
schematic layout of the COMET experiment is presented in
Figure~\ref{fg:mu2ecomet}(right). The major differences of the designs between
Mu2e and COMET exist in the adoption of C-shape curved solenoid magnets for
electron transport. It is useful to eliminate oppositely-charged particles
(like protons) from nuclear muon capture, before going into the detector,
resulting in lower single counting rates in the detectors.
Recently, the COMET collaboration has taken a two-staged approach, in which
COMET Phase-I starts early and COMET Phase-II (the full COMET) will
follow~\cite{phaseI12}. KEK and J-PARC have endorsed the staged approach.
Because of the Phase-I budgetary constraints, a detector to search for \muec
conversion in COMET Phase-I would be a cylindrical drift chamber placed in a
solenoidal magnetic field, as shown in Fig.~\ref{fg:phase1}. In this
configuration, both positive and negative particles (including protons) could
enter the drift chamber. Right now, KEK is keen to start construction of COMET
Phase-I in 2013 as the earliest, if the budget is available.
%
\begin{figure}[htb!]
\centering
\includegraphics[width=.5\textwidth]{figs/comet_phase1_tracker}
\caption{Schematic layout of a cylindrical detector for COMET Phase-I.}
\label{fg:phase1}
%\vspace{-5mm}
\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\subsection{Scientific value of the experiment}
We, as a jointed force between Mu2e and COMET, would like to measure rates and
energy spectrum of charged particle emission after nuclear muon capture on
aluminum. The rates and spectra of charged particle emission, in particular
protons, is very important to optimize the detector configuration both for the
Mu2e and COMET Phase-I experiments.
\noindent The tracking chambers of COMET Phase-I and Mu2e are designed to be
measure charged particles of their momenta greater than 70 MeV/$c$ and 53
MeV/$c$ respectively. In that momentum ranges, it turns out that single hit
rates of the tracking chambers would be dominated by protons after nuclear muon
capture.
The second source of the hit rate will be electrons from muon decays in orbit
(DIO). In order to limit the single hit rate of the tracking chamber to an
acceptable level, both experiments are considering to place proton absorbers in
front of the tracking chambers to reduce proton hit rates. However, the proton
absorber would deteriorate the reconstructed momentum resolution of electrons
at birth. And similarly the rate of proton emission is important to determine
thickness of the muon stopping target made of aluminum. Therefore it is
important to know the rate so that the detector system can be optimized in
terms of both hit rate and momentum resolution.
\noindent Unfortunately the yield, energy spectrum and composition of the
charged particles emitted in muon capture on Al and Ti have not been measured
in the relevant energy range for COMET Phase-I and Mu2e.
Figure~\ref{fg:silicon-proton} shows the spectrum of charged particle emission
from muons being stopped and captured in a silicon detector \cite{sobo68}. The
peak below 1.4 MeV is from the recoiling heavy ions, mainly $^{27}$Al, when no
charged particles were emitted. Hungerford~\cite{hung34} fitted the silicon
spectrum in Fig.~\ref{fg:silicon-proton} with an empirical function given by
%
\begin{equation} p(T) = A(1-{T_{th} \over T})^{\alpha} e^{-(T/T_0)}
\label{eq:protons} \end{equation}
%
where $T$ is the kinetic energy and the fitted parameters are $A=0.105$
MeV$^{-1}$, $T_{th}$ = 1.4 MeV, $\alpha$=1.328 and $T_0$ = 3.1 MeV. The
spectrum is normalized to 0.1 per muon capture. Some other results in the past
experiments are summarized in Table~\ref{tb:proton}.
\begin{figure}[htb]
\centering
\includegraphics[width=0.7\textwidth]{figs/si-proton.pdf}
\caption{Charged particle spectrum from muons stopping and being captured in
a silicon detector~\cite{sobo68}.}
\label{fg:silicon-proton}
\end{figure}
\begin{table}[htb]
\centering \caption{Probabilities in unites of $10^{-3}$ per
muon capture for inclusive proton emission calculated by Lifshitz and
Singer~\cite{lifshitz80}.
The numbers in crescent parenthesis are estimates for the total inclusive
rate derived from the measured exclusive channels by the use of the
approximate regularity, such as $(\mu, \nu p):(\mu, \nu p n):(\mu, \nu p
2n):(\mu, \nu p 3n) = 1:6:4:4$.}
\label{tb:proton}
\vskip 3mm
\begin{tabularx}{\textwidth}{ccccX}
\toprule
Target nucleus & Calculation & Experiment & Estimate & Comments \\
\midrule
%$_{10}$Ne & & $200\pm 40$ & & \\
$^{27}_{13}$Al & 40 & $>28 \pm 4$ & (70) & 7.5 for $T>40$ MeV \\
$^{28}_{14}$Si & 144 & $150\pm30$ & & 3.1 and 0.34 $d$ for $T>18$ MeV \\
$^{31}_{15}$P & 35 & $>61\pm6$ & (91) & \\
$^{46}_{22}$Ti & & & & \\
$^{51}_{23}$V & 25 & $>20\pm1.8$ & (32) & \\
\bottomrule
\end{tabularx}
\end{table}
\noindent The limited information available at present makes it difficult to
draw quantitative conclusive detector design. From Table~\ref{tb:proton}, the
yield for Al can be taken from experiment to be $>$3\% for $T>40$ MeV, or from
theory to be 4\%, or estimated based on the ratio of exclusive channels from
other nuclei to be 7\%, or speculated to be as high as Si
%or Ne
, namely 15-20\%. The
energy spectrum can only be inferred from the Si data or from
Ref.~\cite{bala67}. At this moment, for both COMET Phase-I and Mu2e, this
analytical spectrum has been used to estimate proton emission. And also the $p,
d, \alpha$ composition is not known. The Ti proton yield can only be estimated
from V to be around 3\%.
\noindent It might be worth to present how proton emission affects a single
rate of the tracking chambers. As an example for COMET Phase-I, single rates
of the tracking chamber (cylindrical drift chamber) have been simulated based
on the spectrum given in Eq.(\ref{eq:protons}). To reduce protons entering the
tracking chamber, in addition to the inner wall of the drift chamber (of 400
$\mu$m) a cylindrical proton absorber of different thickness is located in
front of the tracking chamber. Monte Carlo simulations were done with three
different thickness of proton degrader, namely 0~mm, 5~mm, and 7.5~mm.
%Figure~\ref{fig:protongenerated} shows a proton momentum spectrum generated
(larger than 50 MeV/$c$) in the simulation study, and regions in red show
protons reaching the first layer. The results are summarized in
Table~\ref{tb:protonhits}, where the proton emission rate of 0.15 per muon
capture is assumed. If we assume the number of muons stopped in the
muon-stopping target is $5.8 \times 10^{9}$/s, the number of muon capture on
aluminum is about $3.5 \times 10^{9}$/s since the fraction of muon capture in
aluminum is $f_{cap}=0.61$. Therefore the total number of hits in all the cells
in the first layer is estimated to be 530 kHz (1.3 MHz) for the case of a
proton degrader of 5 mm (0 mm) thickness. This example present the importance
to understand the proton emission, rate and spectrum, from nuclear muon capture
on aluminum for COMET Phase-I and Mu2e.
%
\begin{table}[htb]
\begin{center}
\caption{Total numbers of hits in the first
layer by protons emitted from muon capture for different trigger counter
thickness. 100 k proton events were generated for COMET Phase-I. 15 \%
protons per muon capture is assumed.}
\label{tb:protonhits}
\vspace{5mm}
\begin{tabular}{lccc}
\toprule
Proton degrader thickness & 0 mm & 5 mm& 7.5 mm\\
\midrule
% number of 1 hit events & 2467 & 87 & 28 \cr\hline number of 2 hit events &
% 73 & 8 & 1 \cr\hline number of 3 hit events & 9 & 0 & 0 \cr\hline\hline
% number of 4 hit events & 1 & 0 & 0 \cr\hline\hline
Hits & 2644 & 103 & 30 \cr
Hits per proton emission & 2.6 \% & 0.1 \% & 0.03 \% \cr
Hits per muon capture & $3.9\times10^{-3}$ & $1.5\times10^{-4}$ & $4.5\times10^{-5}$ \cr
\bottomrule
\end{tabular}
\end{center}
\end{table}
\subsection{Urgency}
The Mu2e experiment is now under the DOE Critical Decision Review process. The
COMET Phase-I construction, at least the beam line, might start next year in
2013. The COMET collaboration needs to complete the detector design as soon as
possible. Therefore, measurements of proton emission rates and spectrum that
can be done as early as possible become one of the critical path for the both
experiments.
% section motivation (end)
%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Description of the experiment} % (fold) \label{sec:expdescpription}
%\begin{itemize}
%\item principle of the measurement, technique and apparatus
%\item proposed measurements, expected performance and rates
%\item estimation of beam time needed
%\item Involvement of the contributing partners: manpower and finances
%\item Requests to PSI
%\end{itemize}
The goal of the experiment is a measurement of the rate and energy spectrum of
charged particle emission after muon capture in the favored conversion target
Al, as well as Si (as normalization and cross check) and Ti (as an alternative
conversion target material). Both rate and energy spectrum should be measured
to 5\% precision down to an energy of 2.5 MeV.
The basic requirements are summarized is Fig.~\ref{basic.fig}. As the emitted
charged particles deposit a significant amount of energy during their passage
through the target material, thin targets and thus excellent momentum
resolution of the low energy muon beam are critical for this experiment. This
is exactly the reason, why the older experiments in the literature, performed
with thick targets and less sophisticated beams, are unsuitable for providing
the required yield and spectral information for low energy protons. In detail,
the observed energy spectrum $g(T_f)$ of protons emitted from the stopping
target is a convolution of the initial capture spectrum $f(T_i)$ with a
response function $k(T_f,T_i)$:
\begin{equation}
g(T_f) = \int_0^\infty k(T_f,T_i) f(T_i) dT_i
\end{equation}
The response function can be readily calculated for a uniform muon stopping
distribution within the target depth. The resulting distortion of the original
energy distribution taken from Equ.~\ref{eq:protons} is illustrated in
Fig.~\ref{response.fig} for different target thickness.
\begin{figure}[htb]
\begin{center}
\includegraphics[width=\textwidth]{figs/protonrange.png}
\caption{Left: Momentum vs. energy for p, d, $\alpha$, right: proton range
vs. energy in targets.}
\label{basic.fig}
\end{center}
\end{figure}
%\vskip-5ex
\begin{figure}[tb]
\begin{center}
\includegraphics[width=0.6\textwidth]{figs/Si_emitted.pdf}
\caption{Calculated proton emission spectrum as function of target
thickness (red: 0 $\mu m$, green: 50 $\mu m$, blue: 100 $\mu m$, black:
1000 $\mu m$, .}
\label{response.fig}
\end{center}
\end{figure}
\begin{figure}[tb]
\begin{center}
\includegraphics[width=0.405\textwidth]{figs/expcad.png}\includegraphics[width=0.6\textwidth]{figs/exp.png}
\caption{Left: CAD of layout, right: picture of vacuum vessel with
detectors.}
\label{setup.fig}
\end{center}
\end{figure}
A schematic layout of the experimental setup is shown in Fig.~\ref{setup.fig}.
It will be an improved version of a test experiment performed by part of this
collaboration at PSI in 2009.
Low energy muons will be detected by external beam counters (scintillator and
wire chamber, not shown) and then enter a vacuum vessel though a thin mylar
window. They will be stopped in passive Al and Ti foils of 25 to 100 $\mu m$
thickness, positioned under 45 degrees to the beam direction. As a cross check
they will also be stopped in active Si detectors used as target. Two packages
of charged particle detectors are positioned on opposite sides, perpenticular
to the target surface. The geometry is chosen so as to minimize the pathlength
of the emitted protons, and limit their direction to be nearly perpendicular to
the detectors, improving the PID resolution by dE/dx separation. The main
detector of the package is a 5$\times$5 cm$^2$ Si detector of 1500 $\mu m$
thickness (MSX), stopping protons up to about 12 MeV. Plastic scintillators
positioned
behind this Si detector observe potential higher energy protons and veto
through--going electrons. To provide dE/dx information some data will be taken
with two 10x10 cm$^2$ thin Si detectors (65 $\mu m$, MSQ). These detectors are
4-fold segmented. Still, their large capacitance deteriorates the overal
resolution, so measurement with and without them are foreseen. The symmetry
between the left and right Si station allows for a powerful monitor of
systematic effects. Differences between the detectors would indicate background
due to different stopping material, non--uniform stopping distribution or
differences due to muon scattering. Careful shielding of direct or scattered
muons is required, as the stopping fraction is small and proton emission is a
rare capture branch. As shown, we are considering a geometry, where there is no
direct line of sight between any low Z material exposed to muons, with all
shielding done with lead.
In order to normalize a number of muons stopping in the aluminum target, a
Germanium detector to measure muonic X-rays from muons stopping in the aluminum
target is installed. We also will have telescopes to detect electrons from
muons for additional normalization of a number of muons stopped.
The main systematic issues are as follows.
\begin{itemize}
\item Deconvolute the orginal proton spectrum $f(T_i)$. Firstly, an optimal
cloud muon beam is requested for the experiment. Second, the use of an active
Si target allow the experimental calibration of the response function,
because both $T_i$ and $T_f$ are accessible with an active target.
\item Absolute calibration. The number of muon stops will be determined with
the Ge detector. Again, the use of an active Si target allows for a cross
calibration. The proton detection efficiency will be simulated by Geant and
calibrated with the active Si target.
\item PID. The PID of emitted charged particles will be determined by dE/dx,
also the use of time of flight will be investigated.
\item Background. Electron background will be determined with $\mu^+$, neutron
recoils by absorbing the proton component before the Si detectors. A
dangerous background are muons stops in walls and scattered into the Si
detector.
\end{itemize}
A realistic Geant4 simulation is being developed. It will serve as an important
tool to optimize the geometry, in particular regarding background and response
function. Currently the geometry of the PSI test run is being implemented for a
realistic check of the simulation.
\begin{figure}[htb]
\begin{center}
\includegraphics[width=0.9\textwidth]{figs/dedx.png}
\caption{2-dim. plots of
S1 (vertical) vs S2 (horizontal) counters. The plot in top left is for all
charged particles. The ones in top right, bottom left and bottom right are
for only protons, proton+deuteron, proton+deuteron+muons.}
\label{fg:dedx}
\end{center}
\end{figure}
\begin{table}[htb]
\begin{center}
\caption{Estimated event rates for various targets of different
thickness. Incoming $10^{4}$ muons/sec and proton emission rate of
0.15 per muon capture are assumed. The efficiency of Si detector of
100 \% is also assumed. }
\vskip1ex
%\scalebox{0.75}{
\begin{tabular}{cccc}
\toprule
Target & \% Stopping & Event rate (Hz) & Event rate (Hz) \\
thickness ($\mu$m)& in target & All particles & Protons \\
\midrule
50 & 2 & 8.1 & 1.0 \\
100 & 16 & 21.3 & 1.5 \\
150 & 38 & 39.9 & 2.1 \\
200 & 53 & 51.1 & 2.4 \\
\bottomrule
\end{tabular}
%}
\end{center}
\label{tb:rates}
\end{table}
Figure~\ref{fg:dedx} shows Monte Carlo simulation studies of two-dimensional
plots of energy of the S1 counter (dE/dX) vs. energy of the S2 counter. From
Fig.~\ref{fg:dedx}, it is clearly seen that we can discriminate protons,
deuterons and scattered muons and electrons by this particle identification
method. And the range of proton energy from 2.5 MeV to 10 MeV can be detected.
The event rates are estimated based on Monte Carlo simulation. Preliminary
results are summarized in Table~\ref{tb:rates}. They will be updated once we
have full information about the PSI beam properties. As seen in
Table~\ref{tb:rates}, proton rates are not large. A muon beam
whose momentum is low and momentum width is narrow is of critical importance.
And also a ratio of signal to background is 1:50. Therefore, a good particle
identification is important. From Monte Carlo simulation, a combination of
dE/dX and E counters has a sufficient capability of discriminating protons from
the other charged particles.
%
%\begin{table}[htb!]
%\caption{Estimated event rates for various targets of
%different thickness. Incoming $10^{5}$ muons/sec and proton emission rate of
%0.15 per muon capture are assumed. The efficiency of Si detector of 100 \% is
%also assumed. }
%\label{tb:rates} \begin{center} \begin{tabular}{|c|c|c|c|c|c|}
%\hline target & stopping & geometry & hit rate & hit rate & hit rate \\
%thickness & in target & acceptance & all particles & protons & protons \\
%($\mu$m) & (\%) & ($\%$) & (Hz) & (Hz) & (Hz) ($T>$2.5 MeV) \\ \hline 50 &
%28 & 1.1 & 250 & 6 & 4 \\ \hline 100 & 58 & 1.1 & 800 & 25 & 18 \\ \hline
%150 & 77 & 1.0 & 1200 & 33 & 25 \\ \hline \end{tabular} \end{center}
%\end{table}
%\begin{comment} A schematic layout of the experimental setup is shown in
%Fig.~\ref{fg:setup}. The setup has silicon detectors to measure energy of
%charged particles emitted from nuclear muon capture on aluminum. We set an
%aluminum target in a vacuum chamber at the end of M9B muon channel. Negative
%muons of momentum of less than 40 MeV/$c$ are used. The use of lower momentum
%muons (cloud $\mu^{-}$ beam) would increase muons stopping in a thin aluminum
%target, thus reducing backgrounds. Or, we can use a degrader to maximize a
%number of muons in the aluminum target. Figure~\ref{fg:muonstop} shows muon
%stopping distribution in a 50 $\mu$m thick muon stopping target with various
%thick upstream plastic scintillator, and in this case the muon momentum is 30
%MeV/$c$. From Fig.~\ref{fg:muonstop}, the thickness of 13mm is found to be
%optimum.
%Two plastic scintillation counters to identify muons stopping in the aluminum
%target will be installed. The muons pass the beam counter and stops at the
%aluminum target, The muons that do not stop pass the downstream counter so that
%we can identify the muons stopped.
%\begin{figure}[t!] \parbox{0.5\textwidth}{ \begin{center}
%\includegraphics[width=0.48\textwidth]{figs/setup.pdf} \caption{schematic
%layout of the setup.}\label{fg:setup} \end{center} }
%\parbox{0.5\textwidth}{\vspace*{0cm} \begin{center}
%\includegraphics[width=0.48\textwidth]{figs/muonstop.pdf} \caption{Monte
%Carlo simulation on muon stopping distribution in a 50 $\mu$m target for
%various degrader thickness, in top from left to right, thickness of a
%upstream plastic scintillator is 10mm, 11mm, 12mm, in bottom from left to
%right, 13mm, 14 mm, and 15mm.}\label{fg:muonstop} \end{center} }
%\end{figure}
%Charged particles emitted from nuclear muon capture on aluminum are detected by
%a pair of two silicon detectors, one of which is a thin silicon detector to
%measure dE/dX of charged particles (``S1 counter"), and the other is a thick
%silicon detector to measure their total energies, (``S2 counter"). The S1 and
%S2 Si detectors are 65 $\mu$m and 1500 $\mu$m thickness respectively. Behind
%the $E$ counter, a veto counter to ensure charged particles stopping in the S2
%counter is set. In front of the silicon counters, collimators are installed to
%determine the fiducial.
%\begin{figure}[htb!] \begin{center}
%\includegraphics[width=\textwidth]{figs/dedx.pdf} \caption{2-dim. plots of S1
%(vertical) vs S2 (horizontal) counters. The plot in top left is for all
%charged particles. The ones in top right, bottom left and bottom right are
%for only protons, proton+deuteron, proton+deuteron+muons.}\label{fg:dedx}
%\end{center} \end{figure}
%In order to normalize a number of muons stopping in the aluminum target, a
%Germanium detector to measure muonic X-rays from muons stopping in the aluminum
%target is installed (not shown in Fig.~\ref{fg:setup}). It is also currently
%being considered to have a telescope to detect electrons from muons for
%additional normalization of a number of muons stopped.
%Aluminum targets with various thickness (from 50 $\mu$m to 200 $\mu$m) will be
%used. It can be tilted with an angle of $30-45^{\circ}$ with respect to the
%muon beam axis. It is important to have a thin target to measure the spectrum
%precisely, otherwise some deconvolution process to correct for energy loss of
%protons in the target should be involved. It is noted, however that a 200
%$\mu$m thick aluminum disk will be used in both COMET Phase-I and Mu2e
%experiment.
%\end{comment}
% section expdescpription (end)
%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Readiness}
We have a vacuum chamber and Si detectors, which were used for a
similar measurement done at PSI in 2009. For a coming beam test, the
vacuum chamber is being tested now at University of Washington
(UW). The two exiting Si detectors are also being tested at UW. A
possibility to prepare another set of Si detectors is being
sought. Amplifiers for the existing SI detects are available. The
Osaka University (OU) group is preparing DAQ system based on a PSI
standard data acquisition system (MIDAS). The OU group is making
arrangement of getting a Ge detector for muonic X-ray measurement,
either borrowing from someone or purchasing a new one. Monte Carlo
simulations necessary to optimize detector configuration is undergoing
at OU and University College London (UCL).
%Some test beam run to examine a number of muons of low momentum is
%being requested in September, 2012 and
%will be performed with a simplified set-up. The full set-up will be
%ready beginning December 2012.
%\section{Beam time estimation}
%We are requesting a 36 shifts (three weeks) for measurement. This is based on
%the estimation as follows. We will need a 2 days setup time including the
%installation of the equipment, and 5 days of beam tuning to maximize a number
%of muons stopping in the target, adjustment of data taking electronics, and
%2 different thick targets of 7 day data taking for each. Each sample must be
%installed in the chamber, evacuated (we need good vacuum). Data taking of
%7 days is based on the estimated rate of protons
%%whose kinetic energy $T>$ 2,6 MeV
%shown in Table~\ref{tb:rates}. We will accommodate at least 100 k events
%for each sample.
\section{Data analysis}
Data will be analyzed independently at Osaka University, University of
Washington, and University College London, using standard analysis libraries
and our own analysis routines. There is no special requirement on data analysis
support to PSI.
\vspace{5mm}
\begin{thebibliography}{9}
\bibitem{Kuno:1999jp}
Y.~Kuno and Y.~Okada,
%``Muon decay and physics beyond the standard model,''
{\it Rev.\ Mod.\ Phys.\ }{\bf 73}, 151 (2001)
%\bibitem{masi06} L.~Calibbi, A.~Faccia, A.~Masierro, and S.K. Vempati, Phys.
%Rev. {\bf D74} 116002 (2006).
%
\bibitem{mu2e08} R.M.~Carry {\it et al.} (Mu2e collaboration), ``Proposal to
Search for \muec with a Single Event Sensitivity Below $10^{-16}$, FNAL
proposal, 2008.
%
\bibitem{come07} Y.~Kuno {\it et al.} (COMET collaboration), ``A Experimental
Search for Lepton Flavor Violating \muec Conversion at Sensitivity of
$10^{-16}$ with A Slow-Extracted Bunched Proton Beam'', J-PARC Proposal, 2007
and J-PARC Conceptual Design Report, 2009.
%
\bibitem{phaseI12} Y.~Kuno {\it et al.} (COMET collaboration), ``Letter of
Intent of Phase-I for the COMET Experiment at J-PARC'', unpublished, March
2012.
%
\bibitem{sobo68} S.E. Sobotka and E.L. Willis, Phys. Rev. Lett. {\bf 20}
596-598, 1968.
\bibitem{lifshitz80} M. Lifshitz and P. Singer, Phys. Rev. C {\bf 22}
2135-2150, 1980.
%
\bibitem{bala67} V. Balashov and R. Eramzhyan. Atomic Energy Reviews 5, 1967.
%
\bibitem{hung34} E. Hungerford, ``Comment on Proton Emission after Muon
Capture", MECO note 34.
%
\end{thebibliography}
\end{document}

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% eec_nrp_dspr.tex written by M. Comyn last updated 23-05-2012 by NM
% Use this LaTeX file to submit your TRIUMF EEC New Research Proposal
% Detailed Statement of Proposed Research
% NOTE:
% You must enter your experiment number between the braces of the
% \setcounter{expnum}{}
% command located at the foot of this file, prior to entering your text.
%##########################################################################
\documentclass[12pt]{article}
\usepackage{latexsym,multicol,graphicx,rotating}
%\usepackage{amsmath}
%\usepackage{amssymb}
%\usepackage{dcolumn}
%\usepackage{longtable}
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% Use Michel Goossens' dense lists Itemize, Enumerate and Description
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\itemsep=0pt\topsep=0pt\partopsep=0pt\parskip=0pt\parsep=0pt
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\sfcode`\.=1000\relax}
\let\endthebibliography=\endlist
\makeatletter
\renewcommand{\ps@plain}{%
\renewcommand{\@oddhead}{\sffamily\bfseries
\hspace{-2mm}%
\begin{tabular}[t]{|p{180mm}|}\hline
{\footnotesize
TRIUMF EEC New Research Proposal
\hspace{\fill}
Detailed Statement of Proposed Research for Experiment \#: \theexpnum}\\ \hline
\rule[-242mm]{0mm}{0mm}\\ \hline
\end{tabular}}
\renewcommand{\@evenhead}{\@oddhead}
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%%%%%%%%%%%%% user's command definitions
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\newcommand{\AmS}{{\protect\the\textfont2
A\kern-.1667em\lower.5ex\hbox{M}\kern-.125emS}}
\newcommand{\lagr}{\cal{L}}
\newcommand{\mueg}{$\mu^{+} \rightarrow e^{+}\gamma$~}
\newcommand{\meee}{$\mu \rightarrow eee$~}
\newcommand{\muenn}{$\mu \rightarrow e \nu \overline{\nu}$~}
\newcommand{\muenng}{$\mu \rightarrow e \nu \overline{\nu} \gamma$~}
\newcommand{\muec}{$\mu^{-} N \rightarrow e^{-} N$~}
%%%%%%%%%%%%%
\begin{document}
\footnotesize\sffamily
\noindent
\textbf{The EEC committees strongly recommend that you limit your
submissions, including figures and tables, to no more than 4 pages for the
MMSEEC or 10 pages for the SAPEEC. \ The following information should be
included:}%
\vspace*{-2mm}
\scriptsize\sffamily
\begin{Itemize}
\item[(a)]
\textbf{Scientific value of the experiment:}
Describe the importance of the experiment and its relation to previous
work and to theory. All competitive measurements at other laboratories
should be mentioned. Include examples of the best available theoretical
calculations with which the data will be compared.
\item[(b)]
\textbf{Description of the experiment:}
Techniques to be used, scale drawing of the apparatus, measurements to be
made, data rates and background expected, sources of systematic error,
results and precision anticipated. Compare this precision with that
obtained in previous work and discuss its significance in regard to
constraining theory. Give a precise list of targets to be used in order of
their priority.
\item[(c)]
\textbf{Experimental equipment:}
Describe the purpose of all major equipment to be used.
\item[(d)]
\textbf{Readiness:}
Provide a schedule for assembly, construction and testing of equipment.
Include equipment to be provided by TRIUMF. For secondary beam for ISAC, provide information on established yields of the isotope of interest as well as the established isobaric contaminants form the same target/ion-source combination.
\item[(e)]
\textbf{Beam time required:}
State in terms of number of 12-hour shifts. Show details of the beam time
estimates, indicate whether prime-user or parasitic time is involved, and
distinguish time required for test and adjustment of apparatus.
\item[(f)]
\textbf{Data analysis:}
Give details and state what data processing facilities are to be provided
by TRIUMF.
\end{Itemize}
\footnotesize\sffamily
\noindent
\textbf{\boldmath For $\mu$SR experiments}, make sure that your detailed
information includes:
\vspace*{-2mm}
\scriptsize\sffamily
\begin{Itemize}
\item
a concise summary of the scientific problem under investigation, with
appropriate literature references;
\item
clear justification for the proposed experiments and, specifically, a
justification for using $\mu$SR/$\beta$-NMR techniques;
\item
a description of the experimental techniques to be used, naming the
$\mu$SR/$\beta$-NMR spectrometer(s) or ISAC facilities to be used;
\item
an analysis of beam time requirements, including a prioritized list of
samples;
\item
groups with multiple experiments should list all concurrent experiments and
proposals, including outside of TRIUMF, with an indication of how the
personnel effort is to be divided between these activities.
\end{Itemize}
\normalsize\rmfamily
%##########################################################################
\setcounter{expnum}{1371} %Enter your experiment number between the braces
%##########################################################################
% Enter Detailed Statement of Proposed Research below:
\section{Introduction}
It is known that quarks and neutrinos are mixed and therefore their flavors are not conserved in the Standard Model (SM). However, lepton flavor violation for charged leptons have not yet to be observed. In the minimal version of the SM where massless neutrinos are assumed, lepton flavor conservation is a natural consequence of the gauge invariance. Therefore, it has been considered to naively explain why charged lepton flavor violation (CLFV) is highly suppressed.
It have been confirmed that neutrinos are massive and mixed among different neutrino flavor species, by the observation of phenomena of neutrino oscillation. Therefore, lepton flavor for neutrinos is known to be violated. However, CLFV has been yet to be observed, and a discovery of CLFV is considered to be one of the important subjects in elementary particle physics~\cite{Kuno:1999jp}.
In the framework of the Standard Model (SM) with massive neutrinos and their mixing, the branching ratio of $\mu\rightarrow e\gamma$ decay can be estimated. This process is suppressed by the GIM mechanism and the estimated branching ratio is about $O(10^{-54})$. Therefore, the contribution from the SM with massive neutrinos turns out to be very tiny. As a result, it can be concluded that observation of CLFV would indicate a clear signal of new physics beyond the SM with massive neutrino.
CLFV is known to be sensitive to various extension of new physics beyond the SM. Among them, a well-motivated physics model is a supersymmetric (SUSY) model.
In SUSY models, the slepton mixing (given by off-diagonal elements of the slepton mass matrix) would introduce CLFV. In the minimum SUSY scenario, the slepton mass matrix is assumed to be diagonal at the Planck scale. At a low energy scale, new physics phenomena such as grand-unification (GUT) or neutrino seesaw would introduce off-diagonal matrix elements such as $\Delta m_{\tilde{\mu}\tilde{e}}$ through quantum corrections (renormalization). Therefore, the slepon mixing is sensitive to GUT (at $10^{16}$ GeV) or neutrino seesaw mechanism (at $10^{13-14}$ GeV). As a result, it can be concluded that CLFV has potential to study physics at very high energy scale.
The most prominent muon CLFV processes is coherent neutrino-less
conversion of a negative muon to an electron (\muec conversion) in a muonic atom.
When a negative muon is stopped in some material, it
is trapped by an atom, and a muonic atom is formed. After it cascades down
energy levels in the muonic atom, the muon is bound in its 1{\em s}
ground state. The fate of the muon is then either decay in orbit (DIO)
($\mu^{-} \rightarrow e^{-}\nu_{\mu}
\overline{\nu}_{e}$) or nuclear muon capture by a nucleus $N(A,Z)$ of mass number $A$
and atomic number $Z$, namely, $\mu^{-} + N(A,Z) \rightarrow \nu_{\mu} + N(A,Z-1)$.
However, in the context of lepton flavor violation in physics beyond the Standard
Model, the exotic process of neutrino-less muon capture, such as
%
\begin{equation}
\mu^{-} + N(A,Z) \rightarrow e^{-} + N(A,Z),
\end{equation}
%
is also expected. This process is called \muec conversion in a muonic atom.
This process violates the conservation of
lepton flavor numbers, $L_{e}$ and $L_{\mu}$, by one unit, but the
total lepton number, $L$, is conserved.
The event signature of coherent \muec conversion in a muonic atom
is a mono-energetic single electron emitted from the conversion with
an energy ($E_{\mu e}$) of $E_{\mu e} = m_{\mu} - B_{\mu} - E_{recoil}$,
where $m_{\mu}$ is the muon mass, and $B_{\mu}$ is the binding energy of the 1$s$ muonic atom. $E_{recoil}$ is the nuclear recoil energy which is small and can be ignored. Since $B_{\mu}$ varies for various nuclei, $E_{\mu e}$ could be different. For instance, $E_{\mu e} = 104.9$ MeV for aluminum (Al) and $E_{\mu e}$ = 104.3 MeV for titanium (Ti).
From an experimental point of view, \muec conversion is a very
attractive process in the following reasons: (1) First, the energy of the signal electron of about 105 MeV is far above the end-point energy of the normal muon decay spectrum ($\sim$ 52.8 MeV).
(2) Secondly, since the event signature is a mono-energetic electron,
no coincidence measurement is required. The search for this process
has the potential to improve sensitivity by using a high muon rate
without suffering from accidental background events, which would be serious
for other processes, such as $\mu\rightarrow e\gamma$ and $\mu\rightarrow eee$ decays.
The previous search for \muec conversion was performed by the SINDRUM II collaboration at PSI. The SINDRUM II spectrometer consisted of a set of concentric cylindrical drift chambers inside a superconducting solenoid magnet of 1.2 Tesla. They set an upper limit of \muec in Au of $B(\mu^{-} + Au \rightarrow e^{-} + Au) < 7 \times 10^{-13}$.
\begin{figure}[b!]
%\centering
\parbox{0.50\textwidth}{
\includegraphics[width=0.24\textwidth,angle=270]{figs/YK-mu2e-gs.eps}
}
\parbox{0.49\textwidth}{\vspace*{0cm}
\includegraphics[width=0.48\textwidth]{figs/YK-comet-gs.eps}
}
\caption{Schematic layouts of the Mu2e (left) and the COMET (right).}\label{fg:mu2ecomet}
%\vspace{-5mm}
\end{figure}
New experimental projects to search for \muec conversion with a higher sensitivity are being pursued in the USA and Japan. One proposal in the USA is the Mu2e experiment at FNAL.\cite{mu2e08} It is aiming to search for \muec conversion at a sensitivity of better than $10^{-16}$. Figure~\ref{fg:mu2ecomet}(left) shows the proposed layout of the Mu2e experiment. It consists of the production solenoid system, the transport solenoid system and the detector solenoid system. The Mu2e experiment is planned to combat beam-related background events with the help of a 8 GeV/$c$ bunched proton beam of about 8 kW in beam power at FNAL. The detector solenoid is a straight solenoid and therefore both positive and negative charged particles entering the detector. The Mu2e experiment was approved at FNAL PAC in 2009 and obtained the DOE CD-0 approval. Right now the Mu2e collaboration is working on CD-1.
The other experimental proposal to search for \muec conversion, which is called COMET (COherent Muon to Electron Transition), is being prepared at the Japan Proton Accelerator Research Complex (J-PARC), Tokai, Japan.\cite{come07} The aimed sensitivity at COMET is similar to Mu2e, namely better than $10^{-16}$. A schematic layout of the COMET experiment is presented in Figure~\ref{fg:mu2ecomet}(right). The major differences of the designs between Mu2e and COMET exist in the adoption of C-shape curved solenoid magnets for electron transport. It is useful to eliminate oppositely-charged particles (like protons) from nuclear muon capture, before going into the detector, resulting in lower single counting rates in the detectors.
Recently, the COMET collaboration has taken a two-staged approach, in which COMET Phase-I starts early and COMET Phase-II (the full COMET) will follow~\cite{phaseI12}. KEK and J-PARC have endorsed the staged approach. Because of the Phase-I budgetary constraints, a detector to search for \muec conversion in COMET Phase-I would be a cylindrical drift chamber placed in a solenoidal magnetic field, as shown in Fig.~\ref{fg:phase1}. In this configuration, both positive and negative particles (including protons) could enter the drift chamber. Right now, KEK is keen to start construction of COMET Phase-I in 2013 as the earliest, if the budget is available.
%
\begin{figure}[htb!]
\centering
\includegraphics[width=0.4\textwidth]{figs/COMET-Phase1-Detector.eps}
\caption{Schematic layout of a cylindrical detector for COMET Phase-I.}
\label{fg:phase1}
%\vspace{-5mm}
\end{figure}
\section{Scientific value of the experiment}
We, as a jointed force between Mu2e and COMET, would like to measure rates and energy spectrum of charged particle emission after nuclear muon capture on aluminum. The rates and spectra of charged particle emission, in particular protons, is very important to optimize the detector configuration both for the Mu2e and COMET Phase-I experiments.
The tracking chambers of COMET Phase-I and Mu2e are designed to be measure charged particles of their momenta greater than 70 MeV/$c$ and 53 MeV/$c$ respectively. In that momentum ranges, it turns out that single hit rates of the tracking chambers would be dominated by protons after nuclear muon capture. The second source on hit rates could be electrons from muon decays in orbit (DIO). In order to make a single hit rate of the tracking chamber at a reasonable level, the both experiments are considering to place proton absorbers in front of the tracking chambers to reduce proton hit rates. However, the proton absorber would deteriorate the reconstructed momentum resolution of electrons at birth. And similarly the rate of proton emission is important to determine thickness of the muon stopping target made of aluminum. Therefore it is important to know the rate so that the detector system can be optimized in terms of both hit rate and momentum resolution.
\begin{figure}[htb!]
\centering
\includegraphics[width=0.5\textwidth]{figs/si-proton.eps}
\caption{charged particle spectrum from muons stopping and being captured in a silicon detector~\cite{sobo68}.}
\label{fg:silicon-proton}
\vspace{-5mm}
\end{figure}
Unfortunately the yield, energy spectrum and composition of the charged particles emitted in muon capture on Al and Ti have not been measured directly in the relevant energy range for COMET Phase-I and Mu2e. Figure~\ref{fg:silicon-proton} shows the spectrum of charged particle emission from muons being stopped and captured in a silicon detector \cite{sobo68}. The peak below 1.4 MeV is from the recoiling heavy ions, mainly $^{27}$Al, when no charged particles were emitted. Hungerford~\cite{hung34} fitted the silicon spectrum in Fig.~\ref{fg:silicon-proton} with an empirical function given by
%
\begin{equation}
p(T) = A(1-{T_{th} \over T})^{\alpha} e^{-(T/T_0)}
\label{eq:protons}
\end{equation}
%
where $T$ is the kinetic energy and the fitted parameters are $A=0.105$ MeV$^{-1}$, $T_{th}$ = 1.4 MeV, $\alpha$=1.328 and $T_0$ = 3.1 MeV. The spectrum is normalized to 0.1 per muon capture. Some other results in the past experiments are summarized in Table~\ref{tb:proton}.
\begin{table}[b!]
\centering
\caption{Probabilities in unites of $10^{-3}$ per muon capture for inclusive proton emission calculated by Lifshitz and Singer. The numbers in crescent parenthesis are estimates for the total inclusive rate derived from the measured exclusive channels by the use of the approximate regularity, such as $(\mu, \nu p):(\mu, \nu p n):(\mu, \nu p 2n):(\mu. \nu p 3n) = 1:6:4:4$.}\label{tb:proton}
\vskip 3mm
\begin{tabular}{|c|c|c|c|c|}\hline
Target nucleus & Calculation & Experiment & Estimate & Comments \\ \hline
$_{10}$Ne & & $200\pm 40$ & & \\
$^{27}_{13}$Al & 40 & $>28 \pm 4$ & (70) & 7.5 for $T>40$ MeV \\
$^{28}_{14}$Si & 144 & $150\pm30$ & & 3.1 and 0.34 $d$ for $T>18$ MeV \\
$^{31}_{15}$P & 35 & $>61\pm6$ & (91) & \\
$^{46}_{22}$Ti & & & & \\
$^{51}_{23}$V & 25 & $>20\pm1.8$ & (32) & \\ \hline
\end{tabular}
\end{table}
The limited information available at present makes it difficult to draw quantitative conclusive detector design. From Table~\ref{tb:proton}, the yield for Al can be taken from experiment to be $>$3\% for $T>40$ MeV, or from theory to be 4\%, or estimated based on the ratio of exclusive channels from other nuclei to be 7\%, or speculated to be as high as Si or Ne, namely 15-20\%. The energy spectrum can only be inferred from the Si data or from Ref.~\cite{bala67}. At this moment, for both COMET Phase-I and Mu2e, this analytical spectrum has been used to estimate proton emission. And also the $p, d, \alpha$ composition is not known. The Ti proton yield can only be estimated from V to be around 3\%.
it might be worth to present how proton emission affects a single rate of the tracking chambers. As an example for COMET Phase-I, single rates of the tracking chamber (cylindrical drift chamber) has been done based on the spectrum given in Eq.(\ref{eq:protons}). To reduce protons entering the tracking chamber, in addition to the inner wall of the drift chamber (of 400 $\mu$m) a cylindrical proton absorber of different thickness is located in front of the tracking chamber. Monte Carlo simulations were done with three different thickness of proton degrader, namely 0~mm, 5~mm, and 7.5~mm. %Figure~\ref{fig:protongenerated} shows a proton momentum spectrum generated (larger than 50 MeV/$c$) in the simulation study, and regions in red show protons reaching the first layer.
The results are summarized in Table~\ref{tb:protonhits}, where the proton emission rate of 0.15 per muon capture is assumed. If we assume the number of muons stopped in the muon-stopping target is $5.8 \times 10^{9}$/s, the number of muon capture on aluminum is about $3.5 \times 10^{9}$/s since the fraction of muon capture in aluminum is $f_{cap}=0.61$. Therefore the total number of hits in all the cells in the first layer is estimated to be 530 kHz (1.3 MHz) for the case of a proton degrader of 5 mm (0 mm) thickness. This example present the importance to understand the proton emission, rate and spectrum, from nuclear muon capture on aluminum for COMET Phase-I and Mu2e.
%
\begin{table}[ht!]
\begin{center}
\caption{Total numbers of hits in the first layer by protons emitted from muon capture for different trigger counter thickness. 100 k proton events were generated for COMET Phase-I. 15 \% protons per muon capture is assumed.} \label{tb:protonhits}
\vspace{5mm}
\begin{tabular}{|l|c|c|c|} \hline
proton degrader thickness & 0 mm & 5 mm& 7.5 mm\cr\hline\hline
% number of 1 hit events & 2467 & 87 & 28 \cr\hline
% number of 2 hit events & 73 & 8 & 1 \cr\hline
% number of 3 hit events & 9 & 0 & 0 \cr\hline\hline
% number of 4 hit events & 1 & 0 & 0 \cr\hline\hline
hits & 2644 & 103 & 30 \cr\hline
hits per proton emission & 2.6 \% & 0.1 \% & 0.03 \% \cr\hline
hits per muon capture$^{*}$ & $3.9\times10^{-3}$ & $1.5\times10^{-4}$ & $4.5\times10^{-5}$ \cr\hline
\end{tabular}
\end{center}
\end{table}
\vspace{-10mm}
\subsection{Urgency}
The Mu2e experiment is now under the DOE Critical Decision Review process. The COMET Phase-I construction, at least the beam line, might start next year in 2013. The COMET collaboration needs to complete the detector design as soon as possible. Therefore, measurements of proton emission rates and spectrum that can be done as early as possible become one of the critical path for the both experiments.
\section{Description of the experiment}
The Mu2e and COMET collaboration are planning to work together as a joint force to A schematic layout of the experimental setup is shown in Fig.~\ref{fg:setup}. The setup has silicon detectors to measure energy of charged particles emitted from nuclear muon capture on aluminum. We set an aluminum target in a vacuum chamber at the end of M9B muon channel. Negative muons of momentum of less than 40 MeV/$c$ are used. The use of lower momentum muons (cloud $\mu^{-}$ beam) would increase muons stopping in a thin aluminum target, thus reducing backgrounds. Or, we can use a degrader to maximize a number of muons in the aluminum target. Figure~\ref{fg:muonstop} shows muon stopping distribution in a 50 $\mu$m thick muon stopping target with various thick upstream plastic scintillator, and in this case the muon momentum is 30 MeV/$c$. From Fig.~\ref{fg:muonstop}, the thickness of 13mm is found to be optimum.
Two plastic scintillation counters to identify muons stopping in the aluminum target will be installed. The muons pass the beam counter and stops at the aluminum target, The muons that do not stop pass the downstream counter so that we can identify the muons stopped.
%
\begin{figure}[t!]
\parbox{0.5\textwidth}{
\begin{center}
\includegraphics[width=0.48\textwidth]{figs/setup2.eps}
\caption{schematic layout of the setup.}\label{fg:setup}
\end{center}
}
\parbox{0.5\textwidth}{\vspace*{0cm}
\begin{center}
\includegraphics[width=0.48\textwidth]{figs/muonstop.eps}
\caption{Monte Carlo simulation on muon stopping distribution in a 50 $\mu$m target for various degrader thickness, in top from left to right, thickness of a upstream plastic scintillator is 10mm, 11mm, 12mm, in bottom from left to right, 13mm, 14 mm, and 15mm.}\label{fg:muonstop}
\end{center}
}
\end{figure}
Charged particles emitted from nuclear muon capture on aluminum are detected by a pair of two silicon detectors, one of which is a thin silicon detector to measure dE/dX of charged particles (``S1 counter"), and the other is a thick silicon detector to measure their total energies, (``S2 counter"). The S1 and S2 Si detectors are 65 $\mu$m and 1500 $\mu$m thickness respectively. Behind the $E$ counter, a veto counter to ensure charged particles stopping in the S2 counter is set. In front of the silicon counters, collimators are installed to determine the fiducial.
\begin{figure}[htb!]
\begin{center}
\includegraphics[width=\textwidth]{figs/dedx2.eps}
\caption{2-dim. plots of S1 (vertical) vs S2 (horizontal) counters. The plot in top left is for all charged particles. The ones in top right, bottom left and bottom right are for only protons, proton+deuteron, proton+deuteron+tritons.}\label{fg:dedx}
\end{center}
\end{figure}
In order to normalize a number of muons stopping in the aluminum target, a Germanium detector to measure muonic X-rays from muons stopping in the aluminum target is installed (not shown in Fig.~\ref{fg:setup}). It is also currently being considered to have a telescope to detect electrons from muons for additional normalization of a number of muons stopped.
Aluminum targets with various thickness (from 50 $\mu$m to 200 $\mu$m) will be used. It can be tilted with an angle of $30-45^{\circ}$ with respect to the muon beam axis.
It is important to have a thin target to measure the spectrum precisely, otherwise some deconvolution process to correct for energy loss of protons in the target should be involved. It is noted, however that a 200 $\mu$m thick aluminum disk will be used in both COMET Phase-I and Mu2e experiment.
Figure~\ref{fg:dedx} shows Monte Carlo simulation studies of two-dimensional plots of energy of the S1 counter (dE/dX) vs. energy of the S2 counter. From Fig.~\ref{fg:dedx}, it is clearly seen that we can discriminate protons, deuterons and scattered muons and electrons by this particle identification method. And the range of proton energy from 2.5 MeV to 20 MeV can be detected. This energy range is required for COMET Phase-I and Mu2e.
The event rates are estimated based on Monte Carlo simulation. The rates are summarized in Table~\ref{tb:rates}. As seen in Table~\ref{tb:rates}, proton rates of $T>2.6$ MeV are not large. A muon beam whose momentum is low and momentum width is narrow is of critical importance. And also a ratio of signal to background is 1:50. Therefore, a good particle identification is important. From Monte Carlo simulation, a combination of dE/dX and E counters has a sufficient capability of discriminating protons from the other charged particles.
%
\begin{table}[htb!]
\caption{Estimated event rates for various targets of different thickness. Incoming $10^{5}$ muons/sec and proton emission rate of 0.15 per muon capture are assumed. The efficiency of Si detector of 100 \% is also assumed. }\label{tb:rates}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|} \hline
target & stopping & geometry & hit rate & hit rate & hit rate \\
thickness & in target & acceptance & all particles & protons & protons \\
($\mu$m) & (\%) & ($\%$) & (Hz) & (Hz) & (Hz) ($T>$2.6 MeV) \\ \hline
50 & 2.2 & 8.9 & 44.8 & 9.9 & 9.6 \\ \hline
100 & 15.6 & 1.9 & 148.5 & 14.9 & 14.7 \\ \hline
150 & 38.2 & 1.1 & 186.0 & 20.7 & 20.2 \\ \hline
200 & 53.3 & 0.9 & 216.3 & 23.5 & 22.9 \\ \hline
\end{tabular}
\end{center}
\end{table}
\section{Experimental equipment}
not completed yet....
\section{Readiness}
We have a vacuum chamber and Si detectors, which were used for a similar measurement done at PSI in 2009. For a coming beam test, the vacuum chamber is being tested now at University of Washington (UW). The two exiting Si detectors are also being tested at UW. A possibility to prepare another set of Si detectors is being sought. Amplifiers for the existing SI detects are available. The Osaka University (OU) group is preparing DAQ system based on a TRIUMF standard data acquisition system (MIDAS). The OU group is making arrangement of getting a Ge detector for muonic X-ray measurement, either borrowing from someone or purchasing a new one. Monte Carlo simulations necessary to optimize detector configuration is undergoing at OU and University College London (UCL). Some test beam run to examine a number of muons of low momentum is being requested in September, 2012.
\section{Beam time required}
We are requesting a 36 shifts (three weeks) for measurement. This is based on the estimation as follows. We will need a 2 days setup time including the installation of the equipment, and 5 days of beam tuning to maximize a number of muons stopping in the target, adjustment of data taking electronics, and 2 different thick targets of 7 day data taking for each. Each sample must be installed in the chamber, evacuated (we
need good vacuum). Data taking of 7 days is based on the estimated rate of protons whose kinetic energy $T>$ 2,6 MeV, shown in Table~\ref{tb:rates}. We will accommodate at least 100 k events for each sample.
\section{Data analysis}
Data will be analyzed independently at Osaka University, University of Washington, and University College London, using standard analysis libraries and our own analysis routines. There is no special requirement on data analysis support to TRIUMF.
\vspace{5mm}
\begin{thebibliography}{9}
\bibitem{Kuno:1999jp}
Y.~Kuno and Y.~Okada,
%``Muon decay and physics beyond the standard model,''
{\it Rev.\ Mod.\ Phys.\ }{\bf 73}, 151 (2001)
%\bibitem{masi06} L.~Calibbi, A.~Faccia, A.~Masierro, and S.K. Vempati, Phys. Rev. {\bf D74} 116002 (2006).
%
\bibitem{mu2e08} R.M.~Carry {\it et al.} (Mu2e collaboration), ``Proposal to Search for \muec with a Single Event Sensitivity Below $10^{-16}$, FNAL proposal, 2008.
%
\bibitem{come07} Y.~Kuno {\it et al.} (COMET collaboration), ``A Experimental Search for Lepton Flavor Violating \muec Conversion at Sensitivity of $10^{-16}$ with A Slow-Extracted Bunched Proton Beam'', J-PARC Proposal, 2007 and J-PARC Conceptual Design Report, 2009.
%
\bibitem{phaseI12} Y.~Kuno {\it et al.} (COMET collaboration), ``Letter of Intent of Phase-I for the COMET Experiment at J-PARC'', unpublished, March 2012.
%
\bibitem{sobo68} S.E. Sobotka and E.L. Willis, Phys. Rev. Lett. {\bf 20} 596-598, (1968).
%
\bibitem{bala67} V. Balashov and R. Eramzhyan. Atomic Energy Reviews 5, 1967.
%
\bibitem{hung34} E. Hungerford, ``Comment on Proton Emission after Muon Capture", MECO note 34.
%
\end{thebibliography}
\end{document}

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<h1><a name="Call_for_New_Proposals_Letters_o"></a> Call for New Proposals/Letters of Intent/Beam Requests<br>for Experiments or Tests using PSI's Pion, Muon and cold polarized Neutron Beams </h1>
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Next Users' Meeting: January 14 - 16, 2013
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Deadline for submissions and beam requests: December 10, 2012
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<strong>Beam Time Request Form:</strong> <a href="/ltp/UserMeetingEN/beamtime_request.pdf" class='typepdf' target="_top">PDF file</a> / <a href="/ltp/UserMeetingEN/beamtime_request.doc" target="_top">MSWord file</a>
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<h2><a name="General_Remarks"></a> General Remarks </h2>
The pion and muon beams of PSI are normally available free of charge to user groups of universities and research laboratories. A prerequisite for the charge-free admission of external users is the readiness to publish the scientific results in internationally accepted journals, giving proper credit to PSI staff members involved in the experiments as well as proper mention of the PSI facilities.
<br><br>Research groups interested in beam time must first submit research proposals which are reviewed by an international committee and recommended for approval to PSI. Proposals, as well as letters of intent or beam time requests for approved experiments and hardware tests can be submitted once a year ( address , date ).
<h2><a name="Guidelines_for_submitting_new_pr"></a> Guidelines for submitting new proposals </h2>
The <strong>cover page</strong> of the proposal should contain the title, a list of authors with their affiliations and a summary (abstract) of the full experiment.
<br><br>The <strong>second page</strong> should contain the beam requirements:
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<li> beam line , area, special facilities ( Separators, SC magnets, spectrometers)
</li> <li> beam properties (type of particle, intensity, momentum....)
</li> <li> duration of the experiment ( time for setting up, tests, production runs)
</li> <li> any special conditions
</li> <li> beam time request for the first beam period after approval
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The <strong>third page</strong> should consist of the declaration sheet for hazardous samples/equipment ( PDF, Word) . This does not replace a detailed description of safety questions in the full text of the proposal.
<br><br>The <strong>main part</strong> of the proposal should contain the exact description of the experiment:
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<li> Motivation, physics and other goals. Comparison with other experiments and theory.
</li> <li> Principle of the measurement, its technique and apparatus.
</li> <li> Proposed measurements, milestones, expected performance and rates.
</li> <li> Estimate of beam time needed for each step.
</li> <li> Involvement of the contributing partners in terms of manpower (with percentageof each person), and finances.
</li> <li> Requests from PSI : manpower (workshop), finances, special equipment.
</li></ul>
<strong>An electronic copy (preferably as a PDF file) should be sent before the deadline to <a href="mailto&#58;anita&#46;vanloon&#64;psi&#46;ch">anita.vanloon&#64;psi.ch</a>.</strong>
<br><br>If you need beam time for the forthcoming period, please fill out and send us the beam time request form.
<br><br>Upon request from PSI the collaborations of larger projects must prior to final approval write a <strong>Memorandum of Understanding</strong> where each collaborating institute must list its financial and personnel involvement in the experiment. The MoU must show that the collaboration will be able to come up with the required resources. It  must be signed by the grant holders of each collaborating institute.
<h2><a name="Addenda_to_Proposals"></a> Addenda to Proposals </h2>
If a group working on an approved experiment wants to go beyond the scientific goals of the initially proposed experiment, it can submit an addendum which will be treated like a proposal . Please follow the safety procedures . Please fill out the beam time request form , if you want beam for the coming period.
<br><br><strong>An electronic copy (preferably as a PDF file) should be sent before the deadline to <a href="mailto&#58;anita&#46;vanloon&#64;psi&#46;ch">anita.vanloon&#64;psi.ch</a>.</strong>
<h2><a name="Beam_time_requests_for_approved"></a> Beam time requests for approved experiments </h2>
Beam time request forms should normally be accompanied by a status report (electronic copy, preferably as a PDF File), so that the committee can review the progress of the experiment, and sent before the deadline to <a href="mailto&#58;claude&#46;petitjean&#64;psi&#46;ch">claude.petitjean&#64;psi.ch</a>. 
<h2><a name="Beam_time_requests_for_hardware"></a> Beam time requests for hardware tests </h2>
Beam time request forms for testing experimental equipment in test beams should be submitted accompanied with a short justification (electronic copy, preferably as a PDF File) before the deadline to <a href="mailto&#58;claude&#46;petitjean&#64;psi&#46;ch&#46;">claude.petitjean&#64;psi.ch.</a> Please follow the safety procedures .
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<h2><a name="Addresses"></a> Addresses </h2>
<strong>Secretary</strong>
Paul Scherrer Institut
Mrs. Anita Van Loon-Govaerts
WMFA/C12 
CH-5232 Villigen PSI 
Switzerland
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Fax: +41 56 310 5230 
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<br><br><strong>Beam Coordinator</strong>
Paul Scherrer Institut 
Dr. Claude Petitjean
OFLC/005 
CH-5232 Villigen PSI 
Switzerland
<br><br>Phone: +41 56 310 3260 
Fax: +41 56 310 5230 
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<h3><a name="General_Contact"></a> General Contact </h3>
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% eec_nrp_dspr.tex written by M. Comyn last updated 23-05-2012 by NM
% Use this LaTeX file to submit your TRIUMF EEC New Research Proposal
% Detailed Statement of Proposed Research
% NOTE:
% You must enter your experiment number between the braces of the
% \setcounter{expnum}{}
% command located at the foot of this file, prior to entering your text.
%##########################################################################
\documentclass[12pt]{article}
\usepackage{latexsym,multicol,graphicx,rotating}
%\usepackage{amsmath}
%\usepackage{amssymb}
%\usepackage{dcolumn}
%\usepackage{longtable}
%\usepackage{pifont}
% Use Michel Goossens' dense lists Itemize, Enumerate and Description
\let\Otemize =\itemize
\let\Onumerate =\enumerate
\let\Oescription =\description
% Zero the vertical spacing parameters
\def\Nospacing{\itemsep=0pt\topsep=0pt\partopsep=0pt\parskip=0pt\parsep=0pt}
% Redefine the environments in terms of the original values
\newenvironment{Itemize}{\Otemize\Nospacing}{\endlist}
\newenvironment{Enumerate}{\Onumerate\Nospacing}{\endlist}
\newenvironment{Description}{\Oescription\Nospacing}{\endlist}
\newcounter{expnum}
\renewcommand{\thebibliography}[1]{\list
{\arabic{enumi}.}{\settowidth\labelwidth{[#1]}\leftmargin\labelwidth
\advance\leftmargin\labelsep
\usecounter{enumi}}
\renewcommand{\newblock}{\hskip .11em plus .33em minus -.07em}
\itemsep=0pt\topsep=0pt\partopsep=0pt\parskip=0pt\parsep=0pt
\sloppy
\sfcode`\.=1000\relax}
\let\endthebibliography=\endlist
\makeatletter
\renewcommand{\ps@plain}{%
\renewcommand{\@oddhead}{\sffamily\bfseries
\hspace{-2mm}%
\begin{tabular}[t]{|p{180mm}|}\hline
{\footnotesize
TRIUMF EEC New Research Proposal
\hspace{\fill}
Detailed Statement of Proposed Research for Experiment \#: \theexpnum}\\ \hline
\rule[-242mm]{0mm}{0mm}\\ \hline
\end{tabular}}
\renewcommand{\@evenhead}{\@oddhead}
\renewcommand{\@oddfoot}{\sffamily\hfil\thepage\hfil}
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\makeatother
\textwidth 180mm
\textheight 240mm
\topmargin -20mm
\oddsidemargin -7mm
\flushbottom
\frenchspacing
\pagestyle{plain}
%%%%%%%%%%%%% user's command definitions
\newcommand{\ttbs}{\char'134}
\newcommand{\AmS}{{\protect\the\textfont2
A\kern-.1667em\lower.5ex\hbox{M}\kern-.125emS}}
\newcommand{\lagr}{\cal{L}}
\newcommand{\mueg}{$\mu^{+} \rightarrow e^{+}\gamma$~}
\newcommand{\meee}{$\mu \rightarrow eee$~}
\newcommand{\muenn}{$\mu \rightarrow e \nu \overline{\nu}$~}
\newcommand{\muenng}{$\mu \rightarrow e \nu \overline{\nu} \gamma$~}
\newcommand{\muec}{$\mu^{-} N \rightarrow e^{-} N$~}
%%%%%%%%%%%%%
\begin{document}
\footnotesize\sffamily
\noindent
\textbf{The EEC committees strongly recommend that you limit your
submissions, including figures and tables, to no more than 4 pages for the
MMSEEC or 10 pages for the SAPEEC. \ The following information should be
included:}%
\vspace*{-2mm}
\scriptsize\sffamily
\begin{Itemize}
\item[(a)]
\textbf{Scientific value of the experiment:}
Describe the importance of the experiment and its relation to previous
work and to theory. All competitive measurements at other laboratories
should be mentioned. Include examples of the best available theoretical
calculations with which the data will be compared.
\item[(b)]
\textbf{Description of the experiment:}
Techniques to be used, scale drawing of the apparatus, measurements to be
made, data rates and background expected, sources of systematic error,
results and precision anticipated. Compare this precision with that
obtained in previous work and discuss its significance in regard to
constraining theory. Give a precise list of targets to be used in order of
their priority.
\item[(c)]
\textbf{Experimental equipment:}
Describe the purpose of all major equipment to be used.
\item[(d)]
\textbf{Readiness:}
Provide a schedule for assembly, construction and testing of equipment.
Include equipment to be provided by TRIUMF. For secondary beam for ISAC, provide information on established yields of the isotope of interest as well as the established isobaric contaminants form the same target/ion-source combination.
\item[(e)]
\textbf{Beam time required:}
State in terms of number of 12-hour shifts. Show details of the beam time
estimates, indicate whether prime-user or parasitic time is involved, and
distinguish time required for test and adjustment of apparatus.
\item[(f)]
\textbf{Data analysis:}
Give details and state what data processing facilities are to be provided
by TRIUMF.
\end{Itemize}
\footnotesize\sffamily
\noindent
\textbf{\boldmath For $\mu$SR experiments}, make sure that your detailed
information includes:
\vspace*{-2mm}
\scriptsize\sffamily
\begin{Itemize}
\item
a concise summary of the scientific problem under investigation, with
appropriate literature references;
\item
clear justification for the proposed experiments and, specifically, a
justification for using $\mu$SR/$\beta$-NMR techniques;
\item
a description of the experimental techniques to be used, naming the
$\mu$SR/$\beta$-NMR spectrometer(s) or ISAC facilities to be used;
\item
an analysis of beam time requirements, including a prioritized list of
samples;
\item
groups with multiple experiments should list all concurrent experiments and
proposals, including outside of TRIUMF, with an indication of how the
personnel effort is to be divided between these activities.
\end{Itemize}
\normalsize\rmfamily
%##########################################################################
\setcounter{expnum}{1371} %Enter your experiment number between the braces
%##########################################################################
% Enter Detailed Statement of Proposed Research below:
\section{Introduction}
It is known that quarks and neutrinos are mixed and therefore their flavors are not conserved in the Standard Model (SM). However, lepton flavor violation for charged leptons have not yet to be observed. In the minimal version of the SM where massless neutrinos are assumed, lepton flavor conservation is a natural consequence of the gauge invariance. Therefore, it has been considered to naively explain why charged lepton flavor violation (CLFV) is highly suppressed.
It have been confirmed that neutrinos are massive and mixed among different neutrino flavor species, by the observation of phenomena of neutrino oscillation. Therefore, lepton flavor for neutrinos is known to be violated. However, CLFV has been yet to be observed, and a discovery of CLFV is considered to be one of the important subjects in elementary particle physics~\cite{Kuno:1999jp}.
In the framework of the Standard Model (SM) with massive neutrinos and their mixing, the branching ratio of $\mu\rightarrow e\gamma$ decay can be estimated. This process is suppressed by the GIM mechanism and the estimated branching ratio is about $O(10^{-54})$. Therefore, the contribution from the SM with massive neutrinos turns out to be very tiny. As a result, it can be concluded that observation of CLFV would indicate a clear signal of new physics beyond the SM with massive neutrino.
CLFV is known to be sensitive to various extension of new physics beyond the SM. Among them, a well-motivated physics model is a supersymmetric (SUSY) model.
In SUSY models, the slepton mixing (given by off-diagonal elements of the slepton mass matrix) would introduce CLFV. In the minimum SUSY scenario, the slepton mass matrix is assumed to be diagonal at the Planck scale. At a low energy scale, new physics phenomena such as grand-unification (GUT) or neutrino seesaw would introduce off-diagonal matrix elements such as $\Delta m_{\tilde{\mu}\tilde{e}}$ through quantum corrections (renormalization). Therefore, the slepon mixing is sensitive to GUT (at $10^{16}$ GeV) or neutrino seesaw mechanism (at $10^{13-14}$ GeV). As a result, it can be concluded that CLFV has potential to study physics at very high energy scale.
The most prominent muon CLFV processes is coherent neutrino-less
conversion of a negative muon to an electron (\muec conversion) in a muonic atom.
When a negative muon is stopped in some material, it
is trapped by an atom, and a muonic atom is formed. After it cascades down
energy levels in the muonic atom, the muon is bound in its 1{\em s}
ground state. The fate of the muon is then either decay in orbit (DIO)
($\mu^{-} \rightarrow e^{-}\nu_{\mu}
\overline{\nu}_{e}$) or nuclear muon capture by a nucleus $N(A,Z)$ of mass number $A$
and atomic number $Z$, namely, $\mu^{-} + N(A,Z) \rightarrow \nu_{\mu} + N(A,Z-1)$.
However, in the context of lepton flavor violation in physics beyond the Standard
Model, the exotic process of neutrino-less muon capture, such as
%
\begin{equation}
\mu^{-} + N(A,Z) \rightarrow e^{-} + N(A,Z),
\end{equation}
%
is also expected. This process is called \muec conversion in a muonic atom.
This process violates the conservation of
lepton flavor numbers, $L_{e}$ and $L_{\mu}$, by one unit, but the
total lepton number, $L$, is conserved.
The event signature of coherent \muec conversion in a muonic atom
is a mono-energetic single electron emitted from the conversion with
an energy ($E_{\mu e}$) of $E_{\mu e} = m_{\mu} - B_{\mu} - E_{recoil}$,
where $m_{\mu}$ is the muon mass, and $B_{\mu}$ is the binding energy of the 1$s$ muonic atom. $E_{recoil}$ is the nuclear recoil energy which is small and can be ignored. Since $B_{\mu}$ varies for various nuclei, $E_{\mu e}$ could be different. For instance, $E_{\mu e} = 104.9$ MeV for aluminum (Al) and $E_{\mu e}$ = 104.3 MeV for titanium (Ti).
From an experimental point of view, \muec conversion is a very
attractive process in the following reasons: (1) First, the energy of the signal electron of about 105 MeV is far above the end-point energy of the normal muon decay spectrum ($\sim$ 52.8 MeV).
(2) Secondly, since the event signature is a mono-energetic electron,
no coincidence measurement is required. The search for this process
has the potential to improve sensitivity by using a high muon rate
without suffering from accidental background events, which would be serious
for other processes, such as $\mu\rightarrow e\gamma$ and $\mu\rightarrow eee$ decays.
The previous search for \muec conversion was performed by the SINDRUM II collaboration at PSI. The SINDRUM II spectrometer consisted of a set of concentric cylindrical drift chambers inside a superconducting solenoid magnet of 1.2 Tesla. They set an upper limit of \muec in Au of $B(\mu^{-} + Au \rightarrow e^{-} + Au) < 7 \times 10^{-13}$.
\begin{figure}[b!]
%\centering
\parbox{0.50\textwidth}{
\includegraphics[width=0.24\textwidth,angle=270]{figs/YK-mu2e-gs.eps}
}
\parbox{0.49\textwidth}{\vspace*{0cm}
\includegraphics[width=0.48\textwidth]{figs/YK-comet-gs.eps}
}
\caption{Schematic layouts of the Mu2e (left) and the COMET (right).}\label{fg:mu2ecomet}
%\vspace{-5mm}
\end{figure}
New experimental projects to search for \muec conversion with a higher sensitivity are being pursued in the USA and Japan. One proposal in the USA is the Mu2e experiment at FNAL.\cite{mu2e08} It is aiming to search for \muec conversion at a sensitivity of better than $10^{-16}$. Figure~\ref{fg:mu2ecomet}(left) shows the proposed layout of the Mu2e experiment. It consists of the production solenoid system, the transport solenoid system and the detector solenoid system. The Mu2e experiment is planned to combat beam-related background events with the help of a 8 GeV/$c$ bunched proton beam of about 8 kW in beam power at FNAL. The detector solenoid is a straight solenoid and therefore both positive and negative charged particles entering the detector. The Mu2e experiment was approved at FNAL PAC in 2009 and obtained the DOE CD-0 approval. Right now the Mu2e collaboration is working on CD-1.
The other experimental proposal to search for \muec conversion, which is called COMET (COherent Muon to Electron Transition), is being prepared at the Japan Proton Accelerator Research Complex (J-PARC), Tokai, Japan.\cite{come07} The aimed sensitivity at COMET is similar to Mu2e, namely better than $10^{-16}$. A schematic layout of the COMET experiment is presented in Figure~\ref{fg:mu2ecomet}(right). The major differences of the designs between Mu2e and COMET exist in the adoption of C-shape curved solenoid magnets for electron transport. It is useful to eliminate oppositely-charged particles (like protons) from nuclear muon capture, before going into the detector, resulting in lower single counting rates in the detectors.
Recently, the COMET collaboration has taken a two-staged approach, in which COMET Phase-I starts early and COMET Phase-II (the full COMET) will follow~\cite{phaseI12}. KEK and J-PARC have endorsed the staged approach. Because of the Phase-I budgetary constraints, a detector to search for \muec conversion in COMET Phase-I would be a cylindrical drift chamber placed in a solenoidal magnetic field, as shown in Fig.~\ref{fg:phase1}. In this configuration, both positive and negative particles (including protons) could enter the drift chamber. Right now, KEK is keen to start construction of COMET Phase-I in 2013 as the earliest, if the budget is available.
%
\begin{figure}[htb!]
\centering
\includegraphics[width=0.4\textwidth]{figs/COMET-Phase1-Detector.eps}
\caption{Schematic layout of a cylindrical detector for COMET Phase-I.}
\label{fg:phase1}
%\vspace{-5mm}
\end{figure}
\section{Scientific value of the experiment}
We, as a jointed force between Mu2e and COMET, would like to measure rates and energy spectrum of charged particle emission after nuclear muon capture on aluminum. The rates and spectra of charged particle emission, in particular protons, is very important to optimize the detector configuration both for the Mu2e and COMET Phase-I experiments.
The tracking chambers of COMET Phase-I and Mu2e are designed to be measure charged particles of their momenta greater than 70 MeV/$c$ and 53 MeV/$c$ respectively. In that momentum ranges, it turns out that single hit rates of the tracking chambers would be dominated by protons after nuclear muon capture. The second source on hit rates could be electrons from muon decays in orbit (DIO). In order to make a single hit rate of the tracking chamber at a reasonable level, the both experiments are considering to place proton absorbers in front of the tracking chambers to reduce proton hit rates. However, the proton absorber would deteriorate the reconstructed momentum resolution of electrons at birth. And similarly the rate of proton emission is important to determine thickness of the muon stopping target made of aluminum. Therefore it is important to know the rate so that the detector system can be optimized in terms of both hit rate and momentum resolution.
\begin{figure}[htb!]
\centering
\includegraphics[width=0.5\textwidth]{figs/si-proton.eps}
\caption{charged particle spectrum from muons stopping and being captured in a silicon detector~\cite{sobo68}.}
\label{fg:silicon-proton}
\vspace{-5mm}
\end{figure}
Unfortunately the yield, energy spectrum and composition of the charged particles emitted in muon capture on Al and Ti have not been measured directly in the relevant energy range for COMET Phase-I and Mu2e. Figure~\ref{fg:silicon-proton} shows the spectrum of charged particle emission from muons being stopped and captured in a silicon detector \cite{sobo68}. The peak below 1.4 MeV is from the recoiling heavy ions, mainly $^{27}$Al, when no charged particles were emitted. Hungerford~\cite{hung34} fitted the silicon spectrum in Fig.~\ref{fg:silicon-proton} with an empirical function given by
%
\begin{equation}
p(T) = A(1-{T_{th} \over T})^{\alpha} e^{-(T/T_0)}
\label{eq:protons}
\end{equation}
%
where $T$ is the kinetic energy and the fitted parameters are $A=0.105$ MeV$^{-1}$, $T_{th}$ = 1.4 MeV, $\alpha$=1.328 and $T_0$ = 3.1 MeV. The spectrum is normalized to 0.1 per muon capture. Some other results in the past experiments are summarized in Table~\ref{tb:proton}.
\begin{table}[b!]
\centering
\caption{Probabilities in unites of $10^{-3}$ per muon capture for inclusive proton emission calculated by Lifshitz and Singer. The numbers in crescent parenthesis are estimates for the total inclusive rate derived from the measured exclusive channels by the use of the approximate regularity, such as $(\mu, \nu p):(\mu, \nu p n):(\mu, \nu p 2n):(\mu. \nu p 3n) = 1:6:4:4$.}\label{tb:proton}
\vskip 3mm
\begin{tabular}{|c|c|c|c|c|}\hline
Target nucleus & Calculation & Experiment & Estimate & Comments \\ \hline
$_{10}$Ne & & $200\pm 40$ & & \\
$^{27}_{13}$Al & 40 & $>28 \pm 4$ & (70) & 7.5 for $T>40$ MeV \\
$^{28}_{14}$Si & 144 & $150\pm30$ & & 3.1 and 0.34 $d$ for $T>18$ MeV \\
$^{31}_{15}$P & 35 & $>61\pm6$ & (91) & \\
$^{46}_{22}$Ti & & & & \\
$^{51}_{23}$V & 25 & $>20\pm1.8$ & (32) & \\ \hline
\end{tabular}
\end{table}
The limited information available at present makes it difficult to draw quantitative conclusive detector design. From Table~\ref{tb:proton}, the yield for Al can be taken from experiment to be $>$3\% for $T>40$ MeV, or from theory to be 4\%, or estimated based on the ratio of exclusive channels from other nuclei to be 7\%, or speculated to be as high as Si or Ne, namely 15-20\%. The energy spectrum can only be inferred from the Si data or from Ref.~\cite{bala67}. At this moment, for both COMET Phase-I and Mu2e, this analytical spectrum has been used to estimate proton emission. And also the $p, d, \alpha$ composition is not known. The Ti proton yield can only be estimated from V to be around 3\%.
it might be worth to present how proton emission affects a single rate of the tracking chambers. As an example for COMET Phase-I, single rates of the tracking chamber (cylindrical drift chamber) has been done based on the spectrum given in Eq.(\ref{eq:protons}). To reduce protons entering the tracking chamber, in addition to the inner wall of the drift chamber (of 400 $\mu$m) a cylindrical proton absorber of different thickness is located in front of the tracking chamber. Monte Carlo simulations were done with three different thickness of proton degrader, namely 0~mm, 5~mm, and 7.5~mm. %Figure~\ref{fig:protongenerated} shows a proton momentum spectrum generated (larger than 50 MeV/$c$) in the simulation study, and regions in red show protons reaching the first layer.
The results are summarized in Table~\ref{tb:protonhits}, where the proton emission rate of 0.15 per muon capture is assumed. If we assume the number of muons stopped in the muon-stopping target is $5.8 \times 10^{9}$/s, the number of muon capture on aluminum is about $3.5 \times 10^{9}$/s since the fraction of muon capture in aluminum is $f_{cap}=0.61$. Therefore the total number of hits in all the cells in the first layer is estimated to be 530 kHz (1.3 MHz) for the case of a proton degrader of 5 mm (0 mm) thickness. This example present the importance to understand the proton emission, rate and spectrum, from nuclear muon capture on aluminum for COMET Phase-I and Mu2e.
%
\begin{table}[ht!]
\begin{center}
\caption{Total numbers of hits in the first layer by protons emitted from muon capture for different trigger counter thickness. 100 k proton events were generated for COMET Phase-I. 15 \% protons per muon capture is assumed.} \label{tb:protonhits}
\vspace{5mm}
\begin{tabular}{|l|c|c|c|} \hline
proton degrader thickness & 0 mm & 5 mm& 7.5 mm\cr\hline\hline
% number of 1 hit events & 2467 & 87 & 28 \cr\hline
% number of 2 hit events & 73 & 8 & 1 \cr\hline
% number of 3 hit events & 9 & 0 & 0 \cr\hline\hline
% number of 4 hit events & 1 & 0 & 0 \cr\hline\hline
hits & 2644 & 103 & 30 \cr\hline
hits per proton emission & 2.6 \% & 0.1 \% & 0.03 \% \cr\hline
hits per muon capture$^{*}$ & $3.9\times10^{-3}$ & $1.5\times10^{-4}$ & $4.5\times10^{-5}$ \cr\hline
\end{tabular}
\end{center}
\end{table}
\vspace{-10mm}
\subsection{Urgency}
The Mu2e experiment is now under the DOE Critical Decision Review process. The COMET Phase-I construction, at least the beam line, might start next year in 2013. The COMET collaboration needs to complete the detector design as soon as possible. Therefore, measurements of proton emission rates and spectrum that can be done as early as possible become one of the critical path for the both experiments.
\section{Description of the experiment}
The Mu2e and COMET collaboration are planning to work together as a joint force to A schematic layout of the experimental setup is shown in Fig.~\ref{fg:setup}. The setup has silicon detectors to measure energy of charged particles emitted from nuclear muon capture on aluminum. We set an aluminum target in a vacuum chamber at the end of M9B muon channel. Negative muons of momentum of less than 40 MeV/$c$ are used. The use of lower momentum muons (cloud $\mu^{-}$ beam) would increase muons stopping in a thin aluminum target, thus reducing backgrounds. Or, we can use a degrader to maximize a number of muons in the aluminum target. Figure~\ref{fg:muonstop} shows muon stopping distribution in a 50 $\mu$m thick muon stopping target with various thick upstream plastic scintillator, and in this case the muon momentum is 30 MeV/$c$. From Fig.~\ref{fg:muonstop}, the thickness of 13mm is found to be optimum.
Two plastic scintillation counters to identify muons stopping in the aluminum target will be installed. The muons pass the beam counter and stops at the aluminum target, The muons that do not stop pass the downstream counter so that we can identify the muons stopped.
%
\begin{figure}[t!]
\parbox{0.5\textwidth}{
\begin{center}
\includegraphics[width=0.48\textwidth]{figs/setup.eps}
\caption{schematic layout of the setup.}\label{fg:setup}
\end{center}
}
\parbox{0.5\textwidth}{\vspace*{0cm}
\begin{center}
\includegraphics[width=0.48\textwidth]{figs/muonstop.eps}
\caption{Monte Carlo simulation on muon stopping distribution in a 50 $\mu$m target for various degrader thickness, in top from left to right, thickness of a upstream plastic scintillator is 10mm, 11mm, 12mm, in bottom from left to right, 13mm, 14 mm, and 15mm.}\label{fg:muonstop}
\end{center}
}
\end{figure}
Charged particles emitted from nuclear muon capture on aluminum are detected by a pair of two silicon detectors, one of which is a thin silicon detector to measure dE/dX of charged particles (``S1 counter"), and the other is a thick silicon detector to measure their total energies, (``S2 counter"). The S1 and S2 Si detectors are 65 $\mu$m and 1500 $\mu$m thickness respectively. Behind the $E$ counter, a veto counter to ensure charged particles stopping in the S2 counter is set. In front of the silicon counters, collimators are installed to determine the fiducial.
\begin{figure}[htb!]
\begin{center}
\includegraphics[width=\textwidth]{figs/dedx.eps}
\caption{2-dim. plots of S1 (vertical) vs S2 (horizontal) counters. The plot in top left is for all charged particles. The ones in top right, bottom left and bottom right are for only protons, proton+deuteron, proton+deuteron+muons.}\label{fg:dedx}
\end{center}
\end{figure}
In order to normalize a number of muons stopping in the aluminum target, a Germanium detector to measure muonic X-rays from muons stopping in the aluminum target is installed (not shown in Fig.~\ref{fg:setup}). It is also currently being considered to have a telescope to detect electrons from muons for additional normalization of a number of muons stopped.
Aluminum targets with various thickness (from 50 $\mu$m to 200 $\mu$m) will be used. It can be tilted with an angle of $30-45^{\circ}$ with respect to the muon beam axis.
It is important to have a thin target to measure the spectrum precisely, otherwise some deconvolution process to correct for energy loss of protons in the target should be involved. It is noted, however that a 200 $\mu$m thick aluminum disk will be used in both COMET Phase-I and Mu2e experiment.
Figure~\ref{fg:dedx} shows Monte Carlo simulation studies of two-dimensional plots of energy of the S1 counter (dE/dX) vs. energy of the S2 counter. From Fig.~\ref{fg:dedx}, it is clearly seen that we can discriminate protons, deuterons and scattered muons and electrons by this particle identification method. And the range of proton energy from 2.5 MeV to 20 MeV can be detected. This energy range is required for COMET Phase-I and Mu2e.
The event rates are estimated based on Monte Carlo simulation. The rates are summarized in Table~\ref{tb:rates}. As seen in Table~\ref{tb:rates}, proton rates of $T>2.6$ MeV are not large. A muon beam whose momentum is low and momentum width is narrow is of critical importance. And also a ratio of signal to background is 1:50. Therefore, a good particle identification is important. From Monte Carlo simulation, a combination of dE/dX and E counters has a sufficient capability of discriminating protons from the other charged particles.
%
\begin{table}[htb!]
\caption{Estimated event rates for various targets of different thickness. Incoming $10^{5}$ muons/sec and proton emission rate of 0.15 per muon capture are assumed. The efficiency of Si detector of 100 \% is also assumed. }\label{tb:rates}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|} \hline
target & stopping & geometry & hit rate & hit rate & hit rate \\
thickness & in target & acceptance & all particles & protons & protons \\
($\mu$m) & (\%) & ($\%$) & (Hz) & (Hz) & (Hz) ($T>$2.6 MeV) \\ \hline
50 & 28 & 1.1 & 250 & 6 & 4 \\ \hline
100 & 58 & 1.1 & 800 & 25 & 18 \\ \hline
150 & 77 & 1.0 & 1200 & 33 & 25 \\ \hline
\end{tabular}
\end{center}
\end{table}
\section{Experimental equipment}
not completed yet....
\section{Readiness}
We have a vacuum chamber and Si detectors, which were used for a similar measurement done at PSI in 2009. For a coming beam test, the vacuum chamber is being tested now at University of Washington (UW). The two exiting Si detectors are also being tested at UW. A possibility to prepare another set of Si detectors is being sought. Amplifiers for the existing SI detects are available. The Osaka University (OU) group is preparing DAQ system based on a TRIUMF standard data acquisition system (MIDAS). The OU group is making arrangement of getting a Ge detector for muonic X-ray measurement, either borrowing from someone or purchasing a new one. Monte Carlo simulations necessary to optimize detector configuration is undergoing at OU and University College London (UCL). Some test beam run to examine a number of muons of low momentum is being requested in September, 2012.
\section{Beam time required}
We are requesting a 36 shifts (three weeks) for measurement. This is based on the estimation as follows. We will need a 2 days setup time including the installation of the equipment, and 5 days of beam tuning to maximize a number of muons stopping in the target, adjustment of data taking electronics, and 2 different thick targets of 7 day data taking for each. Each sample must be installed in the chamber, evacuated (we
need good vacuum). Data taking of 7 days is based on the estimated rate of protons whose kinetic energy $T>$ 2,6 MeV, shown in Table~\ref{tb:rates}. We will accommodate at least 100 k events for each sample.
\section{Data analysis}
Data will be analyzed independently at Osaka University, University of Washington, and University College London, using standard analysis libraries and our own analysis routines. There is no special requirement on data analysis support to TRIUMF.
\vspace{5mm}
\begin{thebibliography}{9}
\bibitem{Kuno:1999jp}
Y.~Kuno and Y.~Okada,
%``Muon decay and physics beyond the standard model,''
{\it Rev.\ Mod.\ Phys.\ }{\bf 73}, 151 (2001)
%\bibitem{masi06} L.~Calibbi, A.~Faccia, A.~Masierro, and S.K. Vempati, Phys. Rev. {\bf D74} 116002 (2006).
%
\bibitem{mu2e08} R.M.~Carry {\it et al.} (Mu2e collaboration), ``Proposal to Search for \muec with a Single Event Sensitivity Below $10^{-16}$, FNAL proposal, 2008.
%
\bibitem{come07} Y.~Kuno {\it et al.} (COMET collaboration), ``A Experimental Search for Lepton Flavor Violating \muec Conversion at Sensitivity of $10^{-16}$ with A Slow-Extracted Bunched Proton Beam'', J-PARC Proposal, 2007 and J-PARC Conceptual Design Report, 2009.
%
\bibitem{phaseI12} Y.~Kuno {\it et al.} (COMET collaboration), ``Letter of Intent of Phase-I for the COMET Experiment at J-PARC'', unpublished, March 2012.
%
\bibitem{sobo68} S.E. Sobotka and E.L. Willis, Phys. Rev. Lett. {\bf 20} 596-598, (1968).
%
\bibitem{bala67} V. Balashov and R. Eramzhyan. Atomic Energy Reviews 5, 1967.
%
\bibitem{hung34} E. Hungerford, ``Comment on Proton Emission after Muon Capture", MECO note 34.
%
\end{thebibliography}
\end{document}

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bf 9 6 227 1069 bf 9 6 236 1069 bf 9 6 253 1069 bf 8 6 280 1069 bf 9 6 288 1069 bf 9 6 314 1069 bf 9 6 323 1069 bf 8 6 341 1069 bf 8 6 428 1069 bf 8 6 724 1069 bf 9 6 732 1069 bf 9 6 741 1069 bf 9 6 750 1069 bf 9 6 767 1069 bf 9 6 776 1069 bf 8 6
785 1069 bf 9 6 802 1069 bf 8 6 811 1069 bf 9 6 819 1069 bf 9 6 828 1069 bf 9 6 837 1069 bf 8 6 846 1069 bf 9 6 854 1069 bf 9 6 863 1069 bf 8 6 872 1069 bf 9 6 880 1069 bf 9 6 889 1069 bf 9 6 898 1069 bf 8 6 907 1069 bf 9 6 915 1069 bf 9 6 924 1069
bf 8 6 933 1069 bf 9 6 941 1069 bf 9 6 950 1069 bf 8 6 959 1069 bf 9 6 967 1069 bf 9 6 976 1069 bf 9 6 985 1069 bf 8 6 994 1069 bf 9 7 175 1075 bf 8 7 184 1075 bf 9 7 227 1075 bf 9 7 236 1075 bf 8 7 245 1075 bf 9 7 262 1075 bf 8 7 280 1075 bf 9 7
297 1075 bf 8 7 306 1075 bf 9 7 384 1075 bf 9 7 671 1075 bf 9 7 706 1075 bf 9 7 715 1075 bf 8 7 724 1075 bf 9 7 732 1075 bf 9 7 741 1075 bf 9 7 750 1075 bf 8 7 759 1075 bf 9 7 767 1075 bf 9 7 776 1075 bf 8 7 785 1075 bf 9 7 793 1075 bf 9 7 802 1075
bf 8 7 811 1075 bf 9 7 819 1075 bf 9 7 828 1075 bf 9 7 837 1075 bf 8 7 846 1075 bf 9 7 854 1075 bf 9 7 863 1075 bf 8 7 872 1075 bf 9 7 880 1075 bf 9 7 889 1075 bf 9 7 898 1075 bf 8 7 907 1075 bf 9 7 915 1075 bf 9 7 924 1075 bf 8 7 933 1075 bf 9 7
941 1075 bf 9 7 950 1075 bf 8 7 959 1075 bf 9 7 967 1075 bf 9 7 976 1075 bf 9 7 985 1075 bf 8 7 994 1075 bf 8 7 184 1082 bf 8 7 219 1082 bf 9 7 236 1082 bf 9 7 253 1082 bf 9 7 271 1082 bf 8 7 280 1082 bf 8 7 341 1082 bf 9 7 523 1082 bf 8 7 576 1082
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785 1082 bf 9 7 793 1082 bf 9 7 802 1082 bf 8 7 811 1082 bf 9 7 819 1082 bf 9 7 828 1082 bf 9 7 837 1082 bf 8 7 846 1082 bf 9 7 854 1082 bf 9 7 863 1082 bf 8 7 872 1082 bf 9 7 880 1082 bf 9 7 889 1082 bf 9 7 898 1082 bf 8 7 907 1082 bf 9 7 915 1082
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341 1089 bf 9 7 375 1089 bf 9 7 462 1089 bf 9 7 567 1089 bf 9 7 593 1089 bf 9 7 610 1089 bf 9 7 619 1089 bf 9 7 628 1089 bf 8 7 637 1089 bf 9 7 645 1089 bf 9 7 654 1089 bf 8 7 663 1089 bf 9 7 671 1089 bf 9 7 680 1089 bf 9 7 689 1089 bf 8 7 698 1089
bf 9 7 706 1089 bf 9 7 715 1089 bf 8 7 724 1089 bf 9 7 732 1089 bf 9 7 741 1089 bf 9 7 750 1089 bf 8 7 759 1089 bf 9 7 767 1089 bf 9 7 776 1089 bf 8 7 785 1089 bf 9 7 793 1089 bf 9 7 802 1089 bf 8 7 811 1089 bf 9 7 819 1089 bf 9 7 828 1089 bf 9 7
837 1089 bf 8 7 846 1089 bf 9 7 854 1089 bf 9 7 863 1089 bf 8 7 872 1089 bf 9 7 880 1089 bf 9 7 889 1089 bf 8 7 907 1089 bf 9 7 941 1089 bf 9 7 950 1089 bf 8 7 959 1089 bf 9 7 967 1089 bf 8 7 994 1089 bf 8 6 184 1096 bf 9 6 192 1096 bf 8 6 393 1096
bf 9 6 558 1096 bf 9 6 567 1096 bf 8 6 576 1096 bf 9 6 584 1096 bf 9 6 593 1096 bf 8 6 602 1096 bf 9 6 610 1096 bf 9 6 619 1096 bf 9 6 628 1096 bf 8 6 637 1096 bf 9 6 645 1096 bf 9 6 654 1096 bf 8 6 663 1096 bf 9 6 671 1096 bf 9 6 680 1096 bf 9 6
689 1096 bf 8 6 698 1096 bf 9 6 706 1096 bf 9 6 715 1096 bf 8 6 724 1096 bf 9 6 732 1096 bf 9 6 741 1096 bf 9 6 750 1096 bf 8 6 759 1096 bf 9 6 767 1096 bf 9 6 776 1096 bf 8 6 785 1096 bf 9 6 793 1096 bf 9 6 802 1096 bf 8 6 811 1096 bf 9 6 819 1096
bf 9 6 828 1096 bf 9 6 837 1096 bf 8 6 846 1096 bf 9 6 854 1096 bf 9 6 863 1096 bf 9 6 889 1096 bf 9 6 898 1096 bf 8 6 907 1096 bf 9 6 915 1096 bf 9 6 924 1096 bf 9 6 950 1096 bf 9 7 192 1102 bf 9 7 201 1102 bf 9 7 558 1102 bf 9 7 567 1102 bf 9 7
584 1102 bf 8 7 602 1102 bf 9 7 610 1102 bf 9 7 619 1102 bf 9 7 628 1102 bf 8 7 637 1102 bf 9 7 645 1102 bf 9 7 654 1102 bf 8 7 663 1102 bf 9 7 671 1102 bf 9 7 680 1102 bf 9 7 689 1102 bf 8 7 698 1102 bf 9 7 706 1102 bf 9 7 715 1102 bf 8 7 724 1102
bf 9 7 732 1102 bf 9 7 741 1102 bf 9 7 750 1102 bf 8 7 759 1102 bf 9 7 767 1102 bf 9 7 776 1102 bf 8 7 785 1102 bf 9 7 793 1102 bf 9 7 802 1102 bf 8 7 811 1102 bf 9 7 819 1102 bf 9 7 828 1102 bf 9 7 837 1102 bf 8 7 846 1102 bf 9 7 854 1102 bf 9 7
863 1102 bf 9 7 880 1102 bf 9 7 898 1102 bf 9 7 915 1102 bf 9 7 985 1102 bf 8 7 994 1102 bf 9 7 192 1109 bf 9 7 201 1109 bf 8 7 219 1109 bf 9 7 314 1109 bf 9 7 332 1109 bf 9 7 401 1109 bf 8 7 550 1109 bf 9 7 558 1109 bf 9 7 567 1109 bf 8 7 576 1109
bf 9 7 584 1109 bf 9 7 593 1109 bf 8 7 602 1109 bf 9 7 610 1109 bf 9 7 619 1109 bf 9 7 628 1109 bf 8 7 637 1109 bf 9 7 645 1109 bf 9 7 654 1109 bf 8 7 663 1109 bf 9 7 671 1109 bf 9 7 680 1109 bf 9 7 689 1109 bf 8 7 698 1109 bf 9 7 706 1109 bf 9 7
715 1109 bf 8 7 724 1109 bf 9 7 732 1109 bf 9 7 741 1109 bf 9 7 750 1109 bf 8 7 759 1109 bf 9 7 767 1109 bf 9 7 776 1109 bf 8 7 785 1109 bf 9 7 802 1109 bf 8 7 811 1109 bf 9 7 819 1109 bf 9 7 828 1109 bf 8 7 872 1109 bf 9 7 880 1109 bf 8 7 907 1109
bf 9 7 941 1109 bf 9 7 976 1109 bf 9 7 201 1116 bf 9 7 210 1116 bf 8 7 245 1116 bf 9 7 253 1116 bf 9 7 288 1116 bf 9 7 523 1116 bf 9 7 567 1116 bf 8 7 576 1116 bf 9 7 584 1116 bf 9 7 593 1116 bf 8 7 602 1116 bf 9 7 610 1116 bf 9 7 619 1116 bf 9 7
628 1116 bf 8 7 637 1116 bf 9 7 645 1116 bf 9 7 654 1116 bf 8 7 663 1116 bf 9 7 671 1116 bf 9 7 680 1116 bf 9 7 689 1116 bf 8 7 698 1116 bf 9 7 706 1116 bf 9 7 715 1116 bf 8 7 724 1116 bf 9 7 732 1116 bf 9 7 741 1116 bf 9 7 750 1116 bf 8 7 759 1116
bf 9 7 767 1116 bf 9 7 776 1116 bf 9 7 793 1116 bf 8 7 811 1116 bf 9 7 828 1116 bf 8 7 846 1116 bf 9 7 889 1116 bf 8 7 907 1116 bf 9 7 924 1116 bf 9 7 976 1116 bf 8 7 994 1116 bf 9 6 201 1123 bf 9 6 210 1123 bf 8 6 219 1123 bf 9 6 227 1123 bf 8 6
245 1123 bf 8 6 280 1123 bf 9 6 419 1123 bf 9 6 506 1123 bf 8 6 515 1123 bf 9 6 532 1123 bf 9 6 541 1123 bf 8 6 550 1123 bf 9 6 558 1123 bf 9 6 567 1123 bf 8 6 576 1123 bf 9 6 584 1123 bf 9 6 593 1123 bf 8 6 602 1123 bf 9 6 610 1123 bf 9 6 619 1123
bf 9 6 628 1123 bf 8 6 637 1123 bf 9 6 645 1123 bf 9 6 654 1123 bf 8 6 663 1123 bf 9 6 671 1123 bf 9 6 680 1123 bf 9 6 689 1123 bf 8 6 698 1123 bf 9 6 706 1123 bf 9 6 715 1123 bf 8 6 724 1123 bf 9 6 732 1123 bf 8 6 759 1123 bf 9 6 767 1123 bf 9 6
776 1123 bf 9 6 793 1123 bf 9 6 802 1123 bf 8 6 811 1123 bf 8 6 846 1123 bf 9 6 854 1123 bf 9 6 889 1123 bf 9 6 941 1123 bf 9 6 967 1123 bf 8 6 994 1123 bf 9 7 210 1129 bf 9 7 227 1129 bf 8 7 245 1129 bf 9 7 253 1129 bf 9 7 297 1129 bf 9 7 323 1129
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619 1129 bf 9 7 628 1129 bf 8 7 637 1129 bf 9 7 645 1129 bf 9 7 654 1129 bf 8 7 663 1129 bf 9 7 671 1129 bf 9 7 680 1129 bf 9 7 689 1129 bf 8 7 698 1129 bf 9 7 706 1129 bf 9 7 715 1129 bf 8 7 724 1129 bf 9 7 732 1129 bf 9 7 741 1129 bf 9 7 750 1129
bf 8 7 759 1129 bf 9 7 767 1129 bf 9 7 776 1129 bf 9 7 854 1129 bf 8 7 872 1129 bf 9 7 889 1129 bf 8 7 907 1129 bf 9 7 915 1129 bf 9 7 924 1129 bf 8 7 933 1129 bf 9 7 941 1129 bf 9 7 967 1129 bf 9 7 976 1129 bf 9 7 985 1129 bf 8 7 994 1129 bf 9 7
210 1136 bf 8 7 219 1136 bf 9 7 236 1136 bf 9 7 480 1136 bf 8 7 489 1136 bf 9 7 497 1136 bf 9 7 506 1136 bf 8 7 515 1136 bf 9 7 523 1136 bf 9 7 532 1136 bf 9 7 541 1136 bf 8 7 550 1136 bf 9 7 558 1136 bf 9 7 567 1136 bf 8 7 576 1136 bf 9 7 584 1136
bf 9 7 593 1136 bf 8 7 602 1136 bf 9 7 610 1136 bf 9 7 619 1136 bf 9 7 628 1136 bf 8 7 637 1136 bf 9 7 645 1136 bf 9 7 654 1136 bf 8 7 663 1136 bf 9 7 671 1136 bf 9 7 680 1136 bf 9 7 689 1136 bf 8 7 698 1136 bf 9 7 706 1136 bf 8 7 724 1136 bf 9 7
741 1136 bf 9 7 767 1136 bf 9 7 776 1136 bf 9 7 793 1136 bf 9 7 819 1136 bf 9 7 828 1136 bf 9 7 837 1136 bf 9 7 863 1136 bf 9 7 889 1136 bf 9 7 898 1136 bf 8 7 907 1136 bf 9 7 924 1136 bf 8 7 933 1136 bf 9 7 941 1136 bf 9 7 950 1136 bf 9 7 967 1136
bf 9 7 976 1136 bf 8 7 994 1136 bf 9 7 210 1143 bf 8 7 219 1143 bf 8 7 245 1143 bf 9 7 349 1143 bf 9 7 480 1143 bf 8 7 489 1143 bf 9 7 497 1143 bf 9 7 506 1143 bf 8 7 515 1143 bf 9 7 523 1143 bf 9 7 532 1143 bf 9 7 541 1143 bf 8 7 550 1143 bf 9 7
558 1143 bf 9 7 567 1143 bf 8 7 576 1143 bf 9 7 584 1143 bf 9 7 593 1143 bf 8 7 602 1143 bf 9 7 610 1143 bf 9 7 619 1143 bf 8 7 637 1143 bf 9 7 645 1143 bf 9 7 654 1143 bf 8 7 663 1143 bf 9 7 671 1143 bf 9 7 680 1143 bf 9 7 689 1143 bf 9 7 750 1143
bf 9 7 776 1143 bf 9 7 819 1143 bf 9 7 828 1143 bf 8 7 846 1143 bf 9 7 854 1143 bf 9 7 863 1143 bf 8 7 872 1143 bf 9 7 880 1143 bf 9 7 889 1143 bf 9 7 898 1143 bf 8 7 907 1143 bf 9 7 915 1143 bf 9 7 924 1143 bf 9 7 941 1143 bf 9 7 967 1143 bf 9 7
976 1143 bf 9 7 985 1143 bf 8 6 219 1150 bf 9 6 227 1150 bf 9 6 262 1150 bf 8 6 454 1150 bf 9 6 462 1150 bf 9 6 471 1150 bf 9 6 480 1150 bf 8 6 489 1150 bf 9 6 497 1150 bf 9 6 506 1150 bf 8 6 515 1150 bf 9 6 523 1150 bf 9 6 532 1150 bf 9 6 541 1150
bf 8 6 550 1150 bf 9 6 558 1150 bf 9 6 567 1150 bf 8 6 576 1150 bf 9 6 584 1150 bf 9 6 593 1150 bf 8 6 602 1150 bf 9 6 610 1150 bf 9 6 619 1150 bf 9 6 628 1150 bf 8 6 637 1150 bf 9 6 645 1150 bf 9 6 654 1150 bf 8 6 663 1150 bf 8 6 698 1150 bf 9 6
732 1150 bf 9 6 776 1150 bf 8 6 785 1150 bf 9 6 802 1150 bf 9 6 819 1150 bf 9 6 828 1150 bf 9 6 837 1150 bf 8 6 846 1150 bf 9 6 854 1150 bf 8 6 872 1150 bf 9 6 880 1150 bf 9 6 898 1150 bf 8 6 907 1150 bf 9 6 924 1150 bf 8 6 933 1150 bf 8 6 959 1150
bf 9 6 967 1150 bf 8 7 219 1156 bf 9 7 227 1156 bf 8 7 428 1156 bf 9 7 445 1156 bf 8 7 454 1156 bf 9 7 462 1156 bf 9 7 471 1156 bf 9 7 480 1156 bf 8 7 489 1156 bf 9 7 497 1156 bf 9 7 506 1156 bf 8 7 515 1156 bf 9 7 523 1156 bf 9 7 532 1156 bf 9 7
541 1156 bf 8 7 550 1156 bf 9 7 558 1156 bf 9 7 567 1156 bf 8 7 576 1156 bf 9 7 584 1156 bf 9 7 593 1156 bf 8 7 602 1156 bf 9 7 610 1156 bf 9 7 628 1156 bf 8 7 637 1156 bf 9 7 645 1156 bf 8 7 663 1156 bf 9 7 689 1156 bf 8 7 724 1156 bf 9 7 732 1156
bf 8 7 759 1156 bf 9 7 776 1156 bf 8 7 785 1156 bf 9 7 793 1156 bf 9 7 802 1156 bf 8 7 811 1156 bf 9 7 819 1156 bf 9 7 828 1156 bf 9 7 837 1156 bf 8 7 846 1156 bf 9 7 854 1156 bf 8 7 872 1156 bf 9 7 880 1156 bf 9 7 889 1156 bf 8 7 907 1156 bf 8 7
933 1156 bf 9 7 941 1156 bf 9 7 227 1163 bf 8 7 428 1163 bf 9 7 436 1163 bf 9 7 445 1163 bf 8 7 454 1163 bf 9 7 462 1163 bf 9 7 471 1163 bf 9 7 480 1163 bf 8 7 489 1163 bf 9 7 497 1163 bf 9 7 506 1163 bf 8 7 515 1163 bf 9 7 523 1163 bf 9 7 532 1163
bf 9 7 541 1163 bf 8 7 550 1163 bf 9 7 558 1163 bf 9 7 584 1163 bf 9 7 593 1163 bf 8 7 602 1163 bf 9 7 610 1163 bf 9 7 654 1163 bf 9 7 680 1163 bf 9 7 706 1163 bf 9 7 732 1163 bf 9 7 741 1163 bf 9 7 750 1163 bf 8 7 759 1163 bf 9 7 767 1163 bf 9 7
776 1163 bf 8 7 785 1163 bf 9 7 793 1163 bf 9 7 802 1163 bf 8 7 811 1163 bf 9 7 828 1163 bf 9 7 837 1163 bf 8 7 846 1163 bf 9 7 854 1163 bf 8 7 872 1163 bf 9 7 898 1163 bf 9 7 915 1163 bf 9 7 227 1170 bf 9 7 236 1170 bf 9 7 253 1170 bf 8 7 428 1170
bf 9 7 436 1170 bf 9 7 445 1170 bf 8 7 454 1170 bf 9 7 462 1170 bf 9 7 471 1170 bf 9 7 480 1170 bf 8 7 489 1170 bf 9 7 497 1170 bf 9 7 506 1170 bf 8 7 515 1170 bf 9 7 523 1170 bf 9 7 532 1170 bf 9 7 541 1170 bf 8 7 550 1170 bf 9 7 558 1170 bf 9 7
567 1170 bf 8 7 576 1170 bf 9 7 584 1170 bf 8 7 637 1170 bf 9 7 645 1170 bf 9 7 689 1170 bf 8 7 724 1170 bf 9 7 732 1170 bf 9 7 741 1170 bf 9 7 750 1170 bf 8 7 759 1170 bf 9 7 767 1170 bf 9 7 776 1170 bf 8 7 785 1170 bf 9 7 793 1170 bf 9 7 802 1170
bf 8 7 811 1170 bf 9 7 819 1170 bf 9 7 828 1170 bf 8 7 846 1170 bf 9 7 889 1170 bf 9 6 227 1177 bf 9 6 236 1177 bf 9 6 410 1177 bf 9 6 419 1177 bf 8 6 428 1177 bf 9 6 436 1177 bf 9 6 445 1177 bf 8 6 454 1177 bf 9 6 462 1177 bf 9 6 471 1177 bf 9 6
480 1177 bf 8 6 489 1177 bf 9 6 497 1177 bf 9 6 506 1177 bf 9 6 532 1177 bf 8 6 550 1177 bf 9 6 584 1177 bf 9 6 593 1177 bf 8 6 602 1177 bf 8 6 637 1177 bf 9 6 680 1177 bf 9 6 689 1177 bf 9 6 706 1177 bf 9 6 715 1177 bf 8 6 724 1177 bf 9 6 732 1177
bf 9 6 741 1177 bf 9 6 750 1177 bf 8 6 759 1177 bf 9 6 767 1177 bf 9 6 776 1177 bf 9 6 793 1177 bf 9 6 802 1177 bf 8 6 811 1177 bf 9 6 819 1177 bf 9 6 837 1177 bf 9 6 854 1177 bf 9 6 924 1177 bf 9 6 950 1177 bf 9 7 236 1183 bf 8 7 245 1183 bf 8 7
393 1183 bf 9 7 401 1183 bf 9 7 419 1183 bf 8 7 428 1183 bf 9 7 436 1183 bf 9 7 445 1183 bf 8 7 454 1183 bf 9 7 462 1183 bf 9 7 471 1183 bf 9 7 480 1183 bf 8 7 489 1183 bf 9 7 497 1183 bf 9 7 506 1183 bf 8 7 515 1183 bf 9 7 523 1183 bf 9 7 532 1183
bf 9 7 541 1183 bf 8 7 550 1183 bf 8 7 602 1183 bf 9 7 628 1183 bf 9 7 654 1183 bf 9 7 680 1183 bf 8 7 698 1183 bf 9 7 706 1183 bf 9 7 732 1183 bf 9 7 741 1183 bf 9 7 750 1183 bf 8 7 759 1183 bf 9 7 767 1183 bf 9 7 776 1183 bf 8 7 785 1183 bf 9 7
802 1183 bf 8 7 811 1183 bf 9 7 915 1183 bf 9 7 941 1183 bf 9 7 950 1183 bf 8 7 959 1183 bf 9 7 985 1183 bf 8 7 994 1183 bf 9 7 236 1190 bf 8 7 245 1190 bf 9 7 401 1190 bf 9 7 410 1190 bf 9 7 419 1190 bf 8 7 428 1190 bf 9 7 436 1190 bf 9 7 445 1190
bf 8 7 454 1190 bf 9 7 462 1190 bf 9 7 471 1190 bf 9 7 480 1190 bf 8 7 489 1190 bf 9 7 497 1190 bf 9 7 506 1190 bf 8 7 515 1190 bf 9 7 523 1190 bf 9 7 532 1190 bf 8 7 550 1190 bf 9 7 558 1190 bf 8 7 576 1190 bf 9 7 619 1190 bf 9 7 628 1190 bf 8 7
637 1190 bf 9 7 645 1190 bf 9 7 654 1190 bf 9 7 671 1190 bf 9 7 680 1190 bf 9 7 689 1190 bf 8 7 698 1190 bf 9 7 706 1190 bf 9 7 715 1190 bf 9 7 732 1190 bf 9 7 767 1190 bf 9 7 828 1190 bf 9 7 941 1190 bf 9 7 950 1190 bf 9 7 976 1190 bf 8 7 994 1190
bf 8 7 245 1197 bf 9 7 253 1197 bf 9 7 384 1197 bf 9 7 401 1197 bf 9 7 410 1197 bf 9 7 419 1197 bf 8 7 428 1197 bf 9 7 436 1197 bf 9 7 445 1197 bf 8 7 454 1197 bf 9 7 462 1197 bf 9 7 471 1197 bf 9 7 480 1197 bf 8 7 489 1197 bf 9 7 497 1197 bf 9 7
567 1197 bf 9 7 584 1197 bf 8 7 637 1197 bf 9 7 645 1197 bf 8 7 663 1197 bf 9 7 671 1197 bf 9 7 680 1197 bf 9 7 689 1197 bf 8 7 698 1197 bf 9 7 706 1197 bf 9 7 715 1197 bf 8 7 724 1197 bf 9 7 732 1197 bf 9 7 741 1197 bf 8 7 759 1197 bf 9 7 802 1197
bf 9 7 854 1197 bf 9 7 863 1197 bf 8 7 872 1197 bf 9 7 880 1197 bf 9 7 889 1197 bf 8 7 907 1197 bf 8 6 245 1204 bf 9 6 253 1204 bf 8 6 393 1204 bf 9 6 401 1204 bf 9 6 410 1204 bf 9 6 419 1204 bf 8 6 428 1204 bf 9 6 436 1204 bf 9 6 445 1204 bf 8 6
454 1204 bf 9 6 462 1204 bf 9 6 471 1204 bf 9 6 480 1204 bf 8 6 489 1204 bf 9 6 497 1204 bf 9 6 506 1204 bf 9 6 523 1204 bf 8 6 602 1204 bf 9 6 619 1204 bf 9 6 628 1204 bf 8 6 637 1204 bf 9 6 645 1204 bf 8 6 663 1204 bf 9 6 671 1204 bf 9 6 680 1204
bf 9 6 689 1204 bf 8 6 698 1204 bf 9 6 706 1204 bf 9 6 741 1204 bf 9 6 750 1204 bf 9 6 767 1204 bf 8 6 846 1204 bf 9 6 854 1204 bf 9 6 863 1204 bf 8 6 872 1204 bf 9 6 924 1204 bf 9 6 941 1204 bf 9 7 253 1210 bf 9 7 384 1210 bf 8 7 393 1210 bf 9 7
401 1210 bf 9 7 410 1210 bf 9 7 419 1210 bf 8 7 428 1210 bf 9 7 436 1210 bf 9 7 445 1210 bf 8 7 454 1210 bf 9 7 471 1210 bf 9 7 480 1210 bf 8 7 489 1210 bf 9 7 506 1210 bf 9 7 584 1210 bf 9 7 610 1210 bf 9 7 619 1210 bf 9 7 628 1210 bf 8 7 637 1210
bf 9 7 645 1210 bf 9 7 654 1210 bf 8 7 663 1210 bf 9 7 680 1210 bf 9 7 689 1210 bf 9 7 706 1210 bf 9 7 715 1210 bf 9 7 776 1210 bf 8 7 907 1210 bf 9 7 924 1210 bf 9 7 950 1210 bf 9 7 253 1217 bf 9 7 262 1217 bf 9 7 384 1217 bf 8 7 393 1217 bf 9 7
401 1217 bf 9 7 410 1217 bf 9 7 419 1217 bf 8 7 428 1217 bf 9 7 436 1217 bf 9 7 445 1217 bf 8 7 454 1217 bf 9 7 462 1217 bf 8 7 489 1217 bf 9 7 497 1217 bf 9 7 523 1217 bf 9 7 584 1217 bf 9 7 593 1217 bf 8 7 602 1217 bf 9 7 610 1217 bf 9 7 619 1217
bf 9 7 628 1217 bf 9 7 645 1217 bf 8 7 663 1217 bf 8 7 698 1217 bf 9 7 715 1217 bf 9 7 776 1217 bf 9 7 802 1217 bf 8 7 811 1217 bf 9 7 828 1217 bf 9 7 837 1217 bf 9 7 863 1217 bf 9 7 915 1217 bf 8 7 933 1217 bf 9 7 967 1217 bf 9 7 253 1224 bf 9 7
262 1224 bf 8 7 393 1224 bf 9 7 401 1224 bf 9 7 410 1224 bf 9 7 419 1224 bf 8 7 428 1224 bf 9 7 436 1224 bf 9 7 445 1224 bf 8 7 454 1224 bf 9 7 462 1224 bf 9 7 471 1224 bf 9 7 480 1224 bf 8 7 489 1224 bf 8 7 515 1224 bf 9 7 567 1224 bf 8 7 576 1224
bf 9 7 584 1224 bf 9 7 593 1224 bf 8 7 602 1224 bf 9 7 610 1224 bf 9 7 619 1224 bf 9 7 628 1224 bf 8 7 637 1224 bf 9 7 645 1224 bf 9 7 654 1224 bf 8 7 663 1224 bf 9 7 715 1224 bf 9 7 767 1224 bf 9 7 793 1224 bf 8 7 811 1224 bf 9 7 819 1224 bf 9 7
837 1224 bf 9 7 854 1224 bf 9 6 262 1231 bf 9 6 271 1231 bf 8 6 367 1231 bf 9 6 375 1231 bf 9 6 384 1231 bf 8 6 393 1231 bf 9 6 401 1231 bf 9 6 410 1231 bf 9 6 419 1231 bf 8 6 428 1231 bf 9 6 436 1231 bf 8 6 454 1231 bf 9 6 462 1231 bf 9 6 471 1231
bf 9 6 558 1231 bf 9 6 567 1231 bf 8 6 576 1231 bf 9 6 593 1231 bf 8 6 602 1231 bf 9 6 610 1231 bf 9 6 619 1231 bf 9 6 628 1231 bf 8 6 637 1231 bf 9 6 645 1231 bf 9 6 654 1231 bf 8 6 663 1231 bf 9 6 671 1231 bf 8 6 724 1231 bf 9 6 732 1231 bf 9 6
741 1231 bf 8 6 785 1231 bf 9 6 793 1231 bf 9 6 802 1231 bf 8 6 811 1231 bf 9 7 262 1237 bf 9 7 271 1237 bf 9 7 358 1237 bf 8 7 367 1237 bf 9 7 375 1237 bf 9 7 384 1237 bf 8 7 393 1237 bf 9 7 401 1237 bf 9 7 410 1237 bf 9 7 419 1237 bf 8 7 428 1237
bf 9 7 436 1237 bf 9 7 445 1237 bf 8 7 454 1237 bf 9 7 462 1237 bf 9 7 497 1237 bf 9 7 523 1237 bf 9 7 558 1237 bf 9 7 567 1237 bf 8 7 576 1237 bf 9 7 584 1237 bf 8 7 602 1237 bf 9 7 610 1237 bf 9 7 645 1237 bf 9 7 680 1237 bf 8 7 724 1237 bf 9 7
767 1237 bf 9 7 802 1237 bf 9 7 271 1244 bf 8 7 280 1244 bf 9 7 288 1244 bf 9 7 349 1244 bf 9 7 358 1244 bf 8 7 367 1244 bf 9 7 375 1244 bf 9 7 384 1244 bf 8 7 393 1244 bf 9 7 401 1244 bf 9 7 410 1244 bf 9 7 419 1244 bf 8 7 454 1244 bf 8 7 489 1244
bf 9 7 523 1244 bf 9 7 532 1244 bf 8 7 550 1244 bf 9 7 558 1244 bf 9 7 567 1244 bf 8 7 576 1244 bf 9 7 584 1244 bf 9 7 593 1244 bf 8 7 602 1244 bf 9 7 619 1244 bf 9 7 628 1244 bf 8 7 637 1244 bf 9 7 671 1244 bf 9 7 715 1244 bf 8 7 759 1244 bf 9 7
776 1244 bf 8 7 785 1244 bf 9 7 793 1244 bf 9 7 271 1251 bf 8 7 280 1251 bf 9 7 297 1251 bf 8 7 367 1251 bf 9 7 375 1251 bf 9 7 384 1251 bf 8 7 393 1251 bf 9 7 401 1251 bf 9 7 410 1251 bf 9 7 419 1251 bf 9 7 445 1251 bf 8 7 454 1251 bf 9 7 541 1251
bf 8 7 550 1251 bf 9 7 558 1251 bf 9 7 567 1251 bf 8 7 576 1251 bf 9 7 584 1251 bf 9 7 593 1251 bf 9 7 628 1251 bf 8 7 698 1251 bf 9 7 715 1251 bf 8 7 724 1251 bf 9 7 732 1251 bf 9 7 741 1251 bf 9 7 750 1251 bf 9 7 776 1251 bf 9 6 271 1258 bf 8 6
280 1258 bf 8 6 341 1258 bf 9 6 358 1258 bf 8 6 367 1258 bf 9 6 375 1258 bf 9 6 384 1258 bf 8 6 393 1258 bf 9 6 401 1258 bf 9 6 410 1258 bf 9 6 419 1258 bf 8 6 428 1258 bf 8 6 515 1258 bf 9 6 523 1258 bf 9 6 541 1258 bf 8 6 550 1258 bf 9 6 558 1258
bf 9 6 567 1258 bf 9 6 584 1258 bf 9 6 593 1258 bf 9 6 610 1258 bf 9 6 628 1258 bf 9 6 689 1258 bf 8 6 698 1258 bf 9 6 706 1258 bf 9 6 715 1258 bf 8 6 724 1258 bf 9 6 741 1258 bf 9 6 750 1258 bf 8 6 759 1258 bf 9 6 776 1258 bf 8 6 785 1258 bf 8 7
280 1264 bf 9 7 288 1264 bf 8 7 341 1264 bf 9 7 349 1264 bf 9 7 358 1264 bf 8 7 367 1264 bf 9 7 375 1264 bf 9 7 384 1264 bf 8 7 393 1264 bf 9 7 401 1264 bf 9 7 419 1264 bf 8 7 428 1264 bf 9 7 436 1264 bf 9 7 497 1264 bf 9 7 506 1264 bf 9 7 523 1264
bf 9 7 532 1264 bf 9 7 541 1264 bf 8 7 550 1264 bf 9 7 558 1264 bf 8 7 576 1264 bf 9 7 680 1264 bf 9 7 689 1264 bf 8 7 698 1264 bf 9 7 732 1264 bf 9 7 750 1264 bf 8 7 280 1271 bf 9 7 288 1271 bf 9 7 358 1271 bf 8 7 367 1271 bf 9 7 375 1271 bf 9 7
384 1271 bf 8 7 393 1271 bf 9 7 401 1271 bf 8 7 428 1271 bf 9 7 436 1271 bf 8 7 489 1271 bf 9 7 497 1271 bf 9 7 506 1271 bf 9 7 523 1271 bf 9 7 532 1271 bf 9 7 541 1271 bf 8 7 550 1271 bf 8 7 576 1271 bf 9 7 645 1271 bf 9 7 654 1271 bf 8 7 663 1271
bf 9 7 680 1271 bf 8 7 698 1271 bf 9 7 706 1271 bf 9 7 715 1271 bf 9 7 741 1271 bf 9 7 750 1271 bf 9 7 776 1271 bf 9 7 288 1278 bf 8 7 341 1278 bf 9 7 349 1278 bf 9 7 358 1278 bf 8 7 367 1278 bf 9 7 375 1278 bf 9 7 384 1278 bf 8 7 393 1278 bf 9 7
401 1278 bf 9 7 419 1278 bf 8 7 428 1278 bf 9 7 471 1278 bf 9 7 497 1278 bf 9 7 506 1278 bf 8 7 515 1278 bf 9 7 523 1278 bf 9 7 532 1278 bf 9 7 541 1278 bf 8 7 550 1278 bf 8 7 637 1278 bf 9 7 671 1278 bf 9 7 680 1278 bf 8 7 698 1278 bf 9 7 706 1278
bf 9 6 288 1285 bf 9 6 297 1285 bf 9 6 349 1285 bf 9 6 358 1285 bf 8 6 367 1285 bf 9 6 375 1285 bf 9 6 384 1285 bf 9 6 401 1285 bf 9 6 410 1285 bf 9 6 419 1285 bf 9 6 436 1285 bf 9 6 471 1285 bf 9 6 497 1285 bf 9 6 506 1285 bf 8 6 515 1285 bf 9 6
523 1285 bf 9 6 532 1285 bf 9 6 541 1285 bf 8 6 550 1285 bf 9 6 654 1285 bf 8 6 663 1285 bf 9 6 680 1285 bf 8 6 698 1285 bf 9 6 706 1285 bf 9 7 288 1291 bf 9 7 297 1291 bf 9 7 349 1291 bf 9 7 358 1291 bf 8 7 367 1291 bf 9 7 375 1291 bf 9 7 384 1291
bf 8 7 393 1291 bf 9 7 401 1291 bf 8 7 489 1291 bf 9 7 497 1291 bf 9 7 506 1291 bf 8 7 515 1291 bf 9 7 610 1291 bf 9 7 619 1291 bf 9 7 654 1291 bf 9 7 706 1291 bf 9 7 297 1298 bf 8 7 306 1298 bf 8 7 341 1298 bf 9 7 349 1298 bf 9 7 358 1298 bf 8 7
367 1298 bf 9 7 375 1298 bf 9 7 384 1298 bf 9 7 410 1298 bf 8 7 428 1298 bf 9 7 480 1298 bf 8 7 489 1298 bf 9 7 497 1298 bf 9 7 506 1298 bf 8 7 515 1298 bf 9 7 532 1298 bf 9 7 541 1298 bf 8 7 602 1298 bf 9 7 619 1298 bf 8 7 637 1298 bf 9 7 671 1298
bf 9 7 741 1298 bf 8 7 759 1298 bf 9 7 297 1305 bf 8 7 306 1305 bf 9 7 332 1305 bf 8 7 341 1305 bf 9 7 349 1305 bf 9 7 358 1305 bf 8 7 367 1305 bf 9 7 375 1305 bf 9 7 384 1305 bf 8 7 428 1305 bf 9 7 462 1305 bf 9 7 471 1305 bf 8 7 489 1305 bf 9 7
497 1305 bf 9 7 541 1305 bf 9 7 610 1305 bf 9 7 671 1305 bf 8 6 306 1312 bf 9 6 314 1312 bf 9 6 349 1312 bf 9 6 358 1312 bf 8 6 367 1312 bf 9 6 375 1312 bf 9 6 384 1312 bf 8 6 393 1312 bf 9 6 471 1312 bf 9 6 480 1312 bf 8 6 489 1312 bf 9 6 497 1312
bf 9 6 506 1312 bf 8 6 515 1312 bf 8 6 576 1312 bf 9 6 584 1312 bf 9 6 619 1312 bf 8 6 637 1312 bf 8 7 306 1318 bf 9 7 314 1318 bf 8 7 341 1318 bf 9 7 349 1318 bf 9 7 358 1318 bf 9 7 375 1318 bf 8 7 393 1318 bf 9 7 401 1318 bf 9 7 462 1318 bf 9 7
471 1318 bf 9 7 480 1318 bf 8 7 489 1318 bf 9 7 497 1318 bf 9 7 506 1318 bf 9 7 523 1318 bf 9 7 610 1318 bf 9 7 628 1318 bf 8 7 637 1318 bf 9 7 645 1318 bf 9 7 654 1318 bf 8 7 785 1318 bf 9 7 314 1325 bf 9 7 323 1325 bf 8 7 341 1325 bf 9 7 349 1325
bf 9 7 358 1325 bf 8 7 367 1325 bf 9 7 375 1325 bf 9 7 384 1325 bf 8 7 393 1325 bf 9 7 471 1325 bf 9 7 497 1325 bf 9 7 523 1325 bf 9 7 567 1325 bf 8 7 602 1325 bf 9 7 610 1325 bf 8 7 637 1325 bf 9 7 802 1325 bf 9 7 314 1332 bf 9 7 323 1332 bf 9 7
332 1332 bf 8 7 341 1332 bf 9 7 349 1332 bf 9 7 358 1332 bf 8 7 367 1332 bf 9 7 384 1332 bf 9 7 401 1332 bf 9 7 436 1332 bf 9 7 445 1332 bf 8 7 454 1332 bf 9 7 471 1332 bf 8 7 602 1332 bf 9 7 628 1332 bf 8 7 785 1332 bf 9 6 323 1339 bf 9 6 332 1339
bf 8 6 341 1339 bf 9 6 349 1339 bf 9 6 358 1339 bf 8 6 367 1339 bf 8 6 454 1339 bf 9 6 462 1339 bf 9 6 471 1339 bf 9 6 480 1339 bf 8 6 489 1339 bf 9 6 497 1339 bf 8 6 550 1339 bf 9 6 558 1339 bf 8 6 576 1339 bf 9 6 584 1339 bf 9 6 593 1339 bf 9 6
610 1339 bf 9 6 680 1339 bf 9 7 323 1345 bf 9 7 332 1345 bf 8 7 341 1345 bf 9 7 349 1345 bf 9 7 358 1345 bf 9 7 384 1345 bf 8 7 393 1345 bf 9 7 419 1345 bf 9 7 445 1345 bf 8 7 454 1345 bf 9 7 471 1345 bf 8 7 489 1345 bf 9 7 541 1345 bf 9 7 567 1345
bf 8 7 576 1345 bf 9 7 584 1345 bf 8 7 602 1345 bf 9 7 628 1345 bf 9 7 323 1352 bf 9 7 332 1352 bf 9 7 349 1352 bf 9 7 358 1352 bf 8 7 367 1352 bf 9 7 375 1352 bf 9 7 436 1352 bf 9 7 445 1352 bf 8 7 454 1352 bf 9 7 462 1352 bf 9 7 558 1352 bf 8 7
576 1352 bf 9 7 584 1352 bf 9 7 593 1352 bf 9 7 332 1359 bf 8 7 341 1359 bf 9 7 349 1359 bf 9 7 358 1359 bf 9 7 375 1359 bf 9 7 384 1359 bf 9 7 410 1359 bf 9 7 436 1359 bf 9 7 445 1359 bf 8 7 454 1359 bf 9 7 462 1359 bf 9 7 471 1359 bf 8 7 515 1359
bf 9 7 567 1359 bf 8 7 602 1359 bf 9 6 332 1366 bf 8 6 341 1366 bf 9 6 349 1366 bf 9 6 375 1366 bf 9 6 401 1366 bf 8 6 428 1366 bf 9 6 436 1366 bf 9 6 445 1366 bf 8 6 454 1366 bf 9 6 462 1366 bf 9 6 541 1366 bf 8 7 341 1372 bf 9 7 349 1372 bf 9 7
384 1372 bf 8 7 393 1372 bf 9 7 436 1372 bf 9 7 445 1372 bf 8 7 454 1372 bf 9 7 532 1372 bf 9 7 558 1372 bf 8 7 341 1379 bf 9 7 349 1379 bf 8 7 393 1379 bf 9 7 401 1379 bf 9 7 419 1379 bf 8 7 428 1379 bf 9 7 436 1379 bf 9 7 445 1379 bf 9 7 462 1379
bf 9 7 541 1379 bf 9 7 567 1379 bf 9 7 349 1386 bf 9 7 358 1386 bf 8 7 367 1386 bf 9 7 375 1386 bf 8 7 428 1386 bf 9 7 436 1386 bf 9 7 445 1386 bf 9 7 532 1386 bf 9 6 349 1393 bf 9 6 358 1393 bf 9 6 375 1393 bf 8 6 393 1393 bf 9 6 410 1393 bf 8 6
428 1393 bf 9 6 436 1393 bf 9 6 445 1393 bf 9 6 497 1393 bf 9 6 506 1393 bf 9 6 558 1393 bf 9 7 358 1399 bf 8 7 393 1399 bf 9 7 410 1399 bf 8 7 428 1399 bf 9 7 436 1399 bf 9 7 445 1399 bf 9 7 462 1399 bf 9 7 506 1399 bf 9 7 358 1406 bf 8 7 367 1406
bf 9 7 419 1406 bf 8 7 428 1406 bf 8 7 454 1406 bf 8 7 515 1406 bf 9 7 523 1406 bf 9 7 358 1413 bf 8 7 367 1413 bf 9 7 401 1413 bf 9 7 410 1413 bf 9 7 419 1413 bf 8 7 428 1413 bf 9 7 436 1413 bf 8 7 489 1413 bf 9 7 497 1413 bf 9 7 506 1413 bf 8 7
515 1413 bf 9 7 523 1413 bf 9 7 541 1413 bf 9 7 584 1413 bf 8 6 367 1420 bf 9 6 384 1420 bf 9 6 419 1420 bf 9 6 523 1420 bf 8 7 367 1426 bf 9 7 375 1426 bf 9 7 410 1426 bf 9 7 419 1426 bf 9 7 436 1426 bf 8 7 454 1426 bf 9 7 480 1426 bf 9 7 506 1426
bf 8 7 515 1426 bf 9 7 802 1426 bf 8 7 367 1433 bf 9 7 375 1433 bf 8 7 393 1433 bf 9 7 401 1433 bf 9 7 410 1433 bf 8 7 428 1433 bf 9 7 445 1433 bf 8 7 515 1433 bf 9 7 532 1433 bf 9 7 567 1433 bf 9 7 375 1440 bf 9 7 384 1440 bf 9 7 401 1440 bf 8 7
428 1440 bf 8 7 454 1440 bf 9 7 497 1440 bf 9 6 375 1447 bf 9 6 384 1447 bf 8 6 393 1447 bf 9 6 410 1447 bf 9 6 419 1447 bf 9 6 436 1447 bf 9 6 480 1447 bf 8 6 489 1447 bf 9 6 497 1447 bf 9 7 384 1453 bf 8 7 393 1453 bf 9 7 401 1453 bf 9 7 410 1453
bf 9 7 419 1453 bf 9 7 384 1460 bf 8 7 393 1460 bf 9 7 401 1460 bf 8 7 454 1460 bf 8 7 393 1467 bf 9 7 410 1467 bf 9 7 471 1467 bf 8 7 489 1467 bf 8 7 515 1467 bf 8 6 393 1474 bf 9 6 401 1474 bf 9 6 410 1474 bf 9 6 480 1474 bf 9 7 401 1480 bf 9 7
410 1480 bf 9 7 471 1480 bf 9 7 819 1480 bf 9 7 401 1487 bf 9 7 410 1487 bf 9 7 445 1487 bf 9 7 462 1487 bf 9 7 480 1487 bf 9 7 401 1494 bf 9 7 410 1494 bf 9 7 462 1494 bf 9 6 410 1501 bf 9 6 419 1501 bf 9 6 445 1501 bf 9 7 410 1507 bf 9 7 419 1507
bf 8 7 428 1507 bf 8 7 454 1507 bf 9 7 480 1507 bf 9 7 419 1514 bf 9 7 445 1514 bf 9 7 419 1521 bf 8 7 428 1521 bf 9 7 436 1521 bf 8 6 428 1528 bf 9 6 436 1528 bf 8 6 454 1528 bf 9 6 462 1528 bf 9 6 471 1528 bf 8 7 428 1534 bf 9 7 462 1534 bf 8 7
428 1541 bf 9 7 462 1541 bf 9 7 436 1548 bf 8 7 454 1548 bf 9 6 436 1555 bf 9 6 445 1555 bf 8 6 454 1555 bf 9 7 445 1561 bf 8 7 454 1561 bf 9 7 445 1568 bf 8 7 454 1568 bf 9 7 445 1575 bf 8 7 454 1575 bf 8 6 454 1582 bf 9 6 462 1582 bf 8 7 454 1588
bf 9 7 462 1588 bf 9 7 462 1595 bf 9 7 471 1602 bf 9 6 471 1609 bf 9 7 471 1615 bf 9 7 471 1622 bf 9 7 480 1622 bf 9 7 480 1629 bf 9 6 480 1636 bf 8 6 489 1636 bf 9 6 506 1636 bf 8 7 489 1642 bf 8 7 489 1649 bf 1 1 1 c black 132 981 m 870 X s
gsave 1088 844 23 896 C 569.206 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 1001 m -20 Y s 149 991 m -10 Y s 166 991 m -10 Y s 184 991 m -10 Y s 201 991 m -10 Y s 219 1001 m -20 Y s 236 991 m
-10 Y s 253 991 m -10 Y s 271 991 m -10 Y s 288 991 m -10 Y s 306 1001 m -20 Y s 323 991 m -10 Y s 341 991 m -10 Y s 358 991 m -10 Y s 375 991 m -10 Y s 393 1001 m -20 Y s 410 991 m -10 Y s 428 991 m -10 Y s 445 991 m -10 Y s 462 991 m -10 Y s 480
1001 m -20 Y s 497 991 m -10 Y s 515 991 m -10 Y s 532 991 m -10 Y s 550 991 m -10 Y s 567 1001 m -20 Y s 584 991 m -10 Y s 602 991 m -10 Y s 619 991 m -10 Y s 637 991 m -10 Y s 654 1001 m -20 Y s 671 991 m -10 Y s 689 991 m -10 Y s 706 991 m -10 Y
s 724 991 m -10 Y s 741 1001 m -20 Y s 759 991 m -10 Y s 776 991 m -10 Y s 793 991 m -10 Y s 811 991 m -10 Y s 828 1001 m -20 Y s 846 991 m -10 Y s 863 991 m -10 Y s 880 991 m -10 Y s 898 991 m -10 Y s 915 1001 m -20 Y s 933 991 m -10 Y s 950 991 m
-10 Y s 967 991 m -10 Y s 985 991 m -10 Y s 1002 1001 m -20 Y s
gsave 1088 844 23 896 C 120.672 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 182.146 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 268.665 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 355.185 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 441.704 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 23 896 C 530.5 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 23 896 C 617.019 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 23 896 C 703.539 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 23 896 C 790.058 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 23 896 C 876.577 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 23 896 C 956.266 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 1656 m 870 X s 132 1636 m 20 Y s 149 1646 m 10 Y s 166 1646 m 10 Y s 184 1646 m 10 Y s 201 1646 m 10 Y s 219 1636 m 20 Y s 236 1646 m 10
Y s 253 1646 m 10 Y s 271 1646 m 10 Y s 288 1646 m 10 Y s 306 1636 m 20 Y s 323 1646 m 10 Y s 341 1646 m 10 Y s 358 1646 m 10 Y s 375 1646 m 10 Y s 393 1636 m 20 Y s 410 1646 m 10 Y s 428 1646 m 10 Y s 445 1646 m 10 Y s 462 1646 m 10 Y s 480 1636 m
20 Y s 497 1646 m 10 Y s 515 1646 m 10 Y s 532 1646 m 10 Y s 550 1646 m 10 Y s 567 1636 m 20 Y s 584 1646 m 10 Y s 602 1646 m 10 Y s 619 1646 m 10 Y s 637 1646 m 10 Y s 654 1636 m 20 Y s 671 1646 m 10 Y s 689 1646 m 10 Y s 706 1646 m 10 Y s 724 1646
m 10 Y s 741 1636 m 20 Y s 759 1646 m 10 Y s 776 1646 m 10 Y s 793 1646 m 10 Y s 811 1646 m 10 Y s 828 1636 m 20 Y s 846 1646 m 10 Y s 863 1646 m 10 Y s 880 1646 m 10 Y s 898 1646 m 10 Y s 915 1636 m 20 Y s 933 1646 m 10 Y s 950 1646 m 10 Y s 967
1646 m 10 Y s 985 1646 m 10 Y s 1002 1636 m 20 Y s 132 981 m 675 Y s
gsave 1088 844 23 896 C 54.6438 1400.25 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 158 981 m -26 X s 145 997 m -13 X s 145 1013 m -13 X s 145 1029 m -13 X s 145 1045 m -13 X s 158 1061 m -26 X s 145 1077 m -13 X
s 145 1093 m -13 X s 145 1109 m -13 X s 145 1125 m -13 X s 158 1142 m -26 X s 145 1158 m -13 X s 145 1174 m -13 X s 145 1190 m -13 X s 145 1206 m -13 X s 158 1222 m -26 X s 145 1238 m -13 X s 145 1254 m -13 X s 145 1270 m -13 X s 145 1286 m -13 X s
158 1302 m -26 X s 145 1318 m -13 X s 145 1334 m -13 X s 145 1350 m -13 X s 145 1366 m -13 X s 158 1383 m -26 X s 145 1399 m -13 X s 145 1415 m -13 X s 145 1431 m -13 X s 145 1447 m -13 X s 158 1463 m -26 X s 145 1479 m -13 X s 145 1495 m -13 X s
145 1511 m -13 X s 145 1527 m -13 X s 158 1543 m -26 X s 145 1559 m -13 X s 145 1575 m -13 X s 145 1591 m -13 X s 145 1608 m -13 X s 158 1624 m -26 X s 158 1624 m -26 X s 145 1640 m -13 X s 145 1656 m -13 X s
gsave 1088 844 23 896 C 107.011 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 72.8584 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 844 23 896 C 54.6438 1129.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 54.6438 1208.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 844 23 896 C 54.6438 1288.68 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 54.6438 1370.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 844 23 896 C 54.6438 1450.34 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 54.6438 1530.03 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 844 23 896 C 54.6438 1611.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 1002 981 m 675 Y s 976 981 m 26 X s 989 997 m 13 X s 989 1013 m 13 X s 989 1029 m 13 X s 989 1045 m 13 X s 976 1061 m 26 X s 989 1077 m 13 X
s 989 1093 m 13 X s 989 1109 m 13 X s 989 1125 m 13 X s 976 1142 m 26 X s 989 1158 m 13 X s 989 1174 m 13 X s 989 1190 m 13 X s 989 1206 m 13 X s 976 1222 m 26 X s 989 1238 m 13 X s 989 1254 m 13 X s 989 1270 m 13 X s 989 1286 m 13 X s 976 1302 m 26
X s 989 1318 m 13 X s 989 1334 m 13 X s 989 1350 m 13 X s 989 1366 m 13 X s 976 1383 m 26 X s 989 1399 m 13 X s 989 1415 m 13 X s 989 1431 m 13 X s 989 1447 m 13 X s 976 1463 m 26 X s 989 1479 m 13 X s 989 1495 m 13 X s 989 1511 m 13 X s 989 1527 m
13 X s 976 1543 m 26 X s 989 1559 m 13 X s 989 1575 m 13 X s 989 1591 m 13 X s 989 1608 m 13 X s 976 1624 m 26 X s 976 1624 m 26 X s 989 1640 m 13 X s 989 1656 m 13 X s 0.386667 0 1 c 49 34 1008 981 bf 0.2 0 1 c 49 33 1008 1015 bf 0 0.0800001 1 c 49
34 1008 1048 bf 0 0.266667 1 c 49 34 1008 1082 bf 0 0.546666 1 c 49 34 1008 1116 bf 0 0.733333 1 c 49 33 1008 1150 bf 0 1 0.986667 c 49 34 1008 1183 bf 0 1 0.8 c 49 34 1008 1217 bf 0 1 0.52 c 49 34 1008 1251 bf 0 1 0.333333 c 49 33 1008 1285 bf 0 1
0.0533333 c 49 34 1008 1318 bf 0.133333 1 0 c 49 34 1008 1352 bf 0.413333 1 0 c 49 34 1008 1386 bf 0.6 1 0 c 49 33 1008 1420 bf 0.88 1 0 c 49 34 1008 1453 bf 1 0.933333 0 c 49 34 1008 1487 bf 1 0.653333 0 c 49 34 1008 1521 bf 1 0.466667 0 c 49 33
1008 1555 bf 1 0.186667 0 c 49 34 1008 1588 bf 1 0 0 c 49 34 1008 1622 bf black 1057 981 m 675 Y s 1031 981 m 26 X s 1031 1070 m 26 X s 1031 1160 m 26 X s 1031 1249 m 26 X s 1031 1338 m 26 X s 1031 1428 m 26 X s 1031 1517 m 26 X s 1031 1607 m 26 X s
1031 1607 m 26 X s
gsave 1088 844 23 896 C 1061 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 1061 1058.72 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 844 23 896 C 1061 1147.52 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 1061 1236.32 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 844 23 896 C 1061 1325.11 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 1061 1416.18 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 844 23 896 C 1061 1504.98 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 1061 1593.78 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 844 23 896 C 1108.81 1678.02 t 0 r /Helvetica-Bold findfont 20.5224 sf 0 0 m (3) show NC gr
gsave 1088 844 23 896 C 1074.66 1659.8 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
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black 1265 981 m 871 X s
gsave 1088 844 1157 896 C 1703.06 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 1265 1001 m -20 Y s 1283 991 m -10 Y s 1300 991 m -10 Y s 1318 991 m -10 Y s 1335 991 m -10 Y s 1352 1001 m -20 Y s 1370
991 m -10 Y s 1387 991 m -10 Y s 1405 991 m -10 Y s 1422 991 m -10 Y s 1440 1001 m -20 Y s 1457 991 m -10 Y s 1474 991 m -10 Y s 1492 991 m -10 Y s 1509 991 m -10 Y s 1527 1001 m -20 Y s 1544 991 m -10 Y s 1561 991 m -10 Y s 1579 991 m -10 Y s 1596
991 m -10 Y s 1614 1001 m -20 Y s 1631 991 m -10 Y s 1649 991 m -10 Y s 1666 991 m -10 Y s 1683 991 m -10 Y s 1701 1001 m -20 Y s 1718 991 m -10 Y s 1736 991 m -10 Y s 1753 991 m -10 Y s 1770 991 m -10 Y s 1788 1001 m -20 Y s 1805 991 m -10 Y s 1823
991 m -10 Y s 1840 991 m -10 Y s 1858 991 m -10 Y s 1875 1001 m -20 Y s 1892 991 m -10 Y s 1910 991 m -10 Y s 1927 991 m -10 Y s 1945 991 m -10 Y s 1962 1001 m -20 Y s 1979 991 m -10 Y s 1997 991 m -10 Y s 2014 991 m -10 Y s 2032 991 m -10 Y s 2049
1001 m -20 Y s 2067 991 m -10 Y s 2084 991 m -10 Y s 2101 991 m -10 Y s 2119 991 m -10 Y s 2136 1001 m -20 Y s
gsave 1088 844 1157 896 C 1254.53 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 1157 896 C 1316 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 1157 896 C 1402.52 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 1157 896 C 1489.04 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 1157 896 C 1575.56 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 1157 896 C 1664.36 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 1157 896 C 1750.88 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 1157 896 C 1837.4 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 1157 896 C 1923.92 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 1157 896 C 2010.44 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 1157 896 C 2090.12 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 1265 1656 m 871 X s 1265 1636 m 20 Y s 1283 1646 m 10 Y s 1300 1646 m 10 Y s 1318 1646 m 10 Y s 1335 1646 m 10 Y s 1352 1636 m 20 Y s 1370
1646 m 10 Y s 1387 1646 m 10 Y s 1405 1646 m 10 Y s 1422 1646 m 10 Y s 1440 1636 m 20 Y s 1457 1646 m 10 Y s 1474 1646 m 10 Y s 1492 1646 m 10 Y s 1509 1646 m 10 Y s 1527 1636 m 20 Y s 1544 1646 m 10 Y s 1561 1646 m 10 Y s 1579 1646 m 10 Y s 1596
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gsave 1088 844 1157 896 C 1188.5 1400.25 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 1292 981 m -27 X s 1278 997 m -13 X s 1278 1013 m -13 X s 1278 1029 m -13 X s 1278 1045 m -13 X s 1292 1061 m -27 X s 1278 1077
m -13 X s 1278 1093 m -13 X s 1278 1109 m -13 X s 1278 1125 m -13 X s 1292 1142 m -27 X s 1278 1158 m -13 X s 1278 1174 m -13 X s 1278 1190 m -13 X s 1278 1206 m -13 X s 1292 1222 m -27 X s 1278 1238 m -13 X s 1278 1254 m -13 X s 1278 1270 m -13 X s
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gsave 1088 844 1157 896 C 1240.87 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 1157 896 C 1206.72 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 844 1157 896 C 1188.5 1129.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 1157 896 C 1188.5 1208.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 844 1157 896 C 1188.5 1288.68 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 1157 896 C 1188.5 1370.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 844 1157 896 C 1188.5 1450.34 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 1157 896 C 1188.5 1530.03 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
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642 bf 9 7 445 682 bf 1 1 1 c black 132 102 m 870 X s
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s 253 112 m -10 Y s 271 112 m -10 Y s 288 112 m -10 Y s 306 122 m -20 Y s 323 112 m -10 Y s 341 112 m -10 Y s 358 112 m -10 Y s 375 112 m -10 Y s 393 122 m -20 Y s 410 112 m -10 Y s 428 112 m -10 Y s 445 112 m -10 Y s 462 112 m -10 Y s 480 122 m -20
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m -10 Y s 985 112 m -10 Y s 1002 122 m -20 Y s
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gsave 1088 843 23 18 C 268.665 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
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767 m 10 Y s 271 767 m 10 Y s 288 767 m 10 Y s 306 757 m 20 Y s 323 767 m 10 Y s 341 767 m 10 Y s 358 767 m 10 Y s 375 767 m 10 Y s 393 757 m 20 Y s 410 767 m 10 Y s 428 767 m 10 Y s 445 767 m 10 Y s 462 767 m 10 Y s 480 757 m 20 Y s 497 767 m 10 Y
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102 m 675 Y s
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214 m -13 X s 145 231 m -13 X s 145 247 m -13 X s 158 263 m -26 X s 145 279 m -13 X s 145 295 m -13 X s 145 311 m -13 X s 145 327 m -13 X s 158 343 m -26 X s 145 359 m -13 X s 145 375 m -13 X s 145 391 m -13 X s 145 407 m -13 X s 158 423 m -26 X s
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214 m 13 X s 989 231 m 13 X s 989 247 m 13 X s 976 263 m 26 X s 989 279 m 13 X s 989 295 m 13 X s 989 311 m 13 X s 989 327 m 13 X s 976 343 m 26 X s 989 359 m 13 X s 989 375 m 13 X s 989 391 m 13 X s 989 407 m 13 X s 976 423 m 26 X s 989 439 m 13 X
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gsave 1088 843 23 18 C 1061 229.959 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
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8 7 1588 682 bf 9 7 1579 689 bf 8 7 1588 689 bf 9 7 1579 696 bf 8 7 1588 696 bf 9 6 1596 703 bf 8 7 1614 743 bf 1 1 1 c black 1265 102 m 871 X s
gsave 1088 843 1157 18 C 1703.06 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 1265 122 m -20 Y s 1283 112 m -10 Y s 1300 112 m -10 Y s 1318 112 m -10 Y s 1335 112 m -10 Y s 1352 122 m -20 Y s 1370
112 m -10 Y s 1387 112 m -10 Y s 1405 112 m -10 Y s 1422 112 m -10 Y s 1440 122 m -20 Y s 1457 112 m -10 Y s 1474 112 m -10 Y s 1492 112 m -10 Y s 1509 112 m -10 Y s 1527 122 m -20 Y s 1544 112 m -10 Y s 1561 112 m -10 Y s 1579 112 m -10 Y s 1596
112 m -10 Y s 1614 122 m -20 Y s 1631 112 m -10 Y s 1649 112 m -10 Y s 1666 112 m -10 Y s 1683 112 m -10 Y s 1701 122 m -20 Y s 1718 112 m -10 Y s 1736 112 m -10 Y s 1753 112 m -10 Y s 1770 112 m -10 Y s 1788 122 m -20 Y s 1805 112 m -10 Y s 1823
112 m -10 Y s 1840 112 m -10 Y s 1858 112 m -10 Y s 1875 122 m -20 Y s 1892 112 m -10 Y s 1910 112 m -10 Y s 1927 112 m -10 Y s 1945 112 m -10 Y s 1962 122 m -20 Y s 1979 112 m -10 Y s 1997 112 m -10 Y s 2014 112 m -10 Y s 2032 112 m -10 Y s 2049
122 m -20 Y s 2067 112 m -10 Y s 2084 112 m -10 Y s 2101 112 m -10 Y s 2119 112 m -10 Y s 2136 122 m -20 Y s
gsave 1088 843 1157 18 C 1254.53 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 1157 18 C 1316 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 1157 18 C 1402.52 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 1157 18 C 1489.04 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 1157 18 C 1575.56 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 843 1157 18 C 1664.36 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 843 1157 18 C 1750.88 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 843 1157 18 C 1837.4 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 843 1157 18 C 1923.92 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 843 1157 18 C 2010.44 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 843 1157 18 C 2090.12 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 1265 777 m 871 X s 1265 757 m 20 Y s 1283 767 m 10 Y s 1300 767 m 10 Y s 1318 767 m 10 Y s 1335 767 m 10 Y s 1352 757 m 20 Y s 1370 767 m
10 Y s 1387 767 m 10 Y s 1405 767 m 10 Y s 1422 767 m 10 Y s 1440 757 m 20 Y s 1457 767 m 10 Y s 1474 767 m 10 Y s 1492 767 m 10 Y s 1509 767 m 10 Y s 1527 757 m 20 Y s 1544 767 m 10 Y s 1561 767 m 10 Y s 1579 767 m 10 Y s 1596 767 m 10 Y s 1614 757
m 20 Y s 1631 767 m 10 Y s 1649 767 m 10 Y s 1666 767 m 10 Y s 1683 767 m 10 Y s 1701 757 m 20 Y s 1718 767 m 10 Y s 1736 767 m 10 Y s 1753 767 m 10 Y s 1770 767 m 10 Y s 1788 757 m 20 Y s 1805 767 m 10 Y s 1823 767 m 10 Y s 1840 767 m 10 Y s 1858
767 m 10 Y s 1875 757 m 20 Y s 1892 767 m 10 Y s 1910 767 m 10 Y s 1927 767 m 10 Y s 1945 767 m 10 Y s 1962 757 m 20 Y s 1979 767 m 10 Y s 1997 767 m 10 Y s 2014 767 m 10 Y s 2032 767 m 10 Y s 2049 757 m 20 Y s 2067 767 m 10 Y s 2084 767 m 10 Y s
2101 767 m 10 Y s 2119 767 m 10 Y s 2136 757 m 20 Y s 1265 102 m 675 Y s
gsave 1088 843 1157 18 C 1188.5 521.393 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 1292 102 m -27 X s 1278 118 m -13 X s 1278 134 m -13 X s 1278 150 m -13 X s 1278 166 m -13 X s 1292 182 m -27 X s 1278 198 m -13
X s 1278 214 m -13 X s 1278 231 m -13 X s 1278 247 m -13 X s 1292 263 m -27 X s 1278 279 m -13 X s 1278 295 m -13 X s 1278 311 m -13 X s 1278 327 m -13 X s 1292 343 m -27 X s 1278 359 m -13 X s 1278 375 m -13 X s 1278 391 m -13 X s 1278 407 m -13 X
s 1292 423 m -27 X s 1278 439 m -13 X s 1278 455 m -13 X s 1278 472 m -13 X s 1278 488 m -13 X s 1292 504 m -27 X s 1278 520 m -13 X s 1278 536 m -13 X s 1278 552 m -13 X s 1278 568 m -13 X s 1292 584 m -27 X s 1278 600 m -13 X s 1278 616 m -13 X s
1278 632 m -13 X s 1278 648 m -13 X s 1292 664 m -27 X s 1278 680 m -13 X s 1278 697 m -13 X s 1278 713 m -13 X s 1278 729 m -13 X s 1292 745 m -27 X s 1292 745 m -27 X s 1278 761 m -13 X s 1278 777 m -13 X s
gsave 1088 843 1157 18 C 1240.87 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 1157 18 C 1206.72 170.762 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 843 1157 18 C 1188.5 250.451 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 1157 18 C 1188.5 330.139 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 843 1157 18 C 1188.5 409.828 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 1157 18 C 1188.5 491.794 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 843 1157 18 C 1188.5 571.483 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 1157 18 C 1188.5 651.172 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 843 1157 18 C 1188.5 733.137 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 2136 102 m 675 Y s 2110 102 m 26 X s 2123 118 m 13 X s 2123 134 m 13 X s 2123 150 m 13 X s 2123 166 m 13 X s 2110 182 m 26 X s 2123 198 m 13
X s 2123 214 m 13 X s 2123 231 m 13 X s 2123 247 m 13 X s 2110 263 m 26 X s 2123 279 m 13 X s 2123 295 m 13 X s 2123 311 m 13 X s 2123 327 m 13 X s 2110 343 m 26 X s 2123 359 m 13 X s 2123 375 m 13 X s 2123 391 m 13 X s 2123 407 m 13 X s 2110 423 m
26 X s 2123 439 m 13 X s 2123 455 m 13 X s 2123 472 m 13 X s 2123 488 m 13 X s 2110 504 m 26 X s 2123 520 m 13 X s 2123 536 m 13 X s 2123 552 m 13 X s 2123 568 m 13 X s 2110 584 m 26 X s 2123 600 m 13 X s 2123 616 m 13 X s 2123 632 m 13 X s 2123 648
m 13 X s 2110 664 m 26 X s 2123 680 m 13 X s 2123 697 m 13 X s 2123 713 m 13 X s 2123 729 m 13 X s 2110 745 m 26 X s 2110 745 m 26 X s 2123 761 m 13 X s 2123 777 m 13 X s 0.386667 0 1 c 49 34 2142 102 bf 0.2 0 1 c 49 33 2142 136 bf 0 0.0800001 1 c
49 34 2142 169 bf 0 0.266667 1 c 49 34 2142 203 bf 0 0.546666 1 c 49 34 2142 237 bf 0 0.733333 1 c 49 33 2142 271 bf 0 1 0.986667 c 49 34 2142 304 bf 0 1 0.8 c 49 34 2142 338 bf 0 1 0.52 c 49 34 2142 372 bf 0 1 0.333333 c 49 33 2142 406 bf 0 1
0.0533333 c 49 34 2142 439 bf 0.133333 1 0 c 49 34 2142 473 bf 0.413333 1 0 c 49 34 2142 507 bf 0.6 1 0 c 49 33 2142 541 bf 0.88 1 0 c 49 34 2142 574 bf 1 0.933333 0 c 49 34 2142 608 bf 1 0.653333 0 c 49 34 2142 642 bf 1 0.466667 0 c 49 33 2142 676
bf 1 0.186667 0 c 49 34 2142 709 bf 1 0 0 c 49 34 2142 743 bf black 2191 102 m 675 Y s 2164 102 m 27 X s 2164 169 m 27 X s 2164 237 m 27 X s 2164 304 m 27 X s 2164 372 m 27 X s 2164 439 m 27 X s 2164 507 m 27 X s 2164 574 m 27 X s 2164 642 m 27 X s
2164 709 m 27 X s 2164 777 m 27 X s
gsave 1088 843 1157 18 C 2194.86 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 1157 18 C 2194.86 159.378 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5) show NC gr
gsave 1088 843 1157 18 C 2194.86 225.406 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 843 1157 18 C 2194.86 291.433 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (15) show NC gr
gsave 1088 843 1157 18 C 2194.86 359.738 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (20) show NC gr
gsave 1088 843 1157 18 C 2194.86 425.766 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (25) show NC gr
gsave 1088 843 1157 18 C 2194.86 494.071 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (30) show NC gr
gsave 1088 843 1157 18 C 2194.86 562.375 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (35) show NC gr
gsave 1088 843 1157 18 C 2194.86 628.403 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (40) show NC gr
gsave 1088 843 1157 18 C 2194.86 696.708 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (45) show NC gr
gsave 1088 843 1157 18 C 2194.86 765.013 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (50) show NC gr 1 1 1 c 587 44 1167 813 bf black 1167 813 m 587 X s 1754 813 m 44 Y s 1754 857 m -587 X s 1167 857 m -44 Y s 1 1 1 c black
gsave 1088 843 1157 18 C 1208.99 824.21 t 0 r /Helvetica-Bold findfont 34.204 sf 0 0 m (Protons, deuterons and tritons) show NC gr
gr gr showpage
end
%%EOF

871
AlCapPSI/figs/PID115-260keV.eps Normal file
View File

@@ -0,0 +1,871 @@
%!PS-Adobe-2.0 EPSF-2.0
%%BoundingBox: 0 0 567 439
%%Title: PID115-260keV.eps: c1
%%Creator: ROOT Version 5.30/02
%%CreationDate: Tue Jun 5 22:58:06 2012
%%EndComments
%%BeginProlog
80 dict begin
/s {stroke} def /l {lineto} def /m {moveto} def /t {translate} def
/r {rotate} def /rl {roll} def /R {repeat} def
/d {rlineto} def /rm {rmoveto} def /gr {grestore} def /f {eofill} def
/c {setrgbcolor} def /black {0 setgray} def /sd {setdash} def
/cl {closepath} def /sf {scalefont setfont} def /lw {setlinewidth} def
/box {m dup 0 exch d exch 0 d 0 exch neg d cl} def
/NC{systemdict begin initclip end}def/C{NC box clip newpath}def
/bl {box s} def /bf {box f} def /Y { 0 exch d} def /X { 0 d} def
/K {{pop pop 0 moveto} exch kshow} bind def
/ita {/ang 15 def gsave [1 0 ang dup sin exch cos div 1 0 0] concat} def
/mp {newpath /y exch def /x exch def} def
/side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def
/mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def
/mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def
/mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def
/m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26{mt s} def
/m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def
/m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def
/m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d 0 w3 neg d w3 neg 0 d cl s } def
/m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t 4 {side} repeat cl fill gr} def
/m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t 4 {side} repeat cl s gr} def
/m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d x w2 sub y w2 add m w w neg d x w2 sub y w2 sub m w w d s} def
/m32 {mp x y w2 sub m w2 w d w neg 0 d cl s} def
/m33 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl f} def
/m34 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d 0 w3 neg d w3 neg 0 d cl f } def
/m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def
/m5 {mp x w2 sub y w2 sub m w w d x w2 sub y w2 add m w w neg d s} def
/reEncode {exch findfont dup length dict begin {1 index /FID eq {pop pop} {def} ifelse } forall /Encoding exch def currentdict end dup /FontName get exch definefont pop } def [/Times-Bold /Times-Italic /Times-BoldItalic /Helvetica /Helvetica-Oblique
/Helvetica-Bold /Helvetica-BoldOblique /Courier /Courier-Oblique /Courier-Bold /Courier-BoldOblique /Times-Roman /AvantGarde-Book /AvantGarde-BookOblique /AvantGarde-Demi /AvantGarde-DemiOblique /Bookman-Demi /Bookman-DemiItalic /Bookman-Light
/Bookman-LightItalic /Helvetica-Narrow /Helvetica-Narrow-Bold /Helvetica-Narrow-BoldOblique /Helvetica-Narrow-Oblique /NewCenturySchlbk-Roman /NewCenturySchlbk-Bold /NewCenturySchlbk-BoldItalic /NewCenturySchlbk-Italic /Palatino-Bold
/Palatino-BoldItalic /Palatino-Italic /Palatino-Roman ] {ISOLatin1Encoding reEncode } forall%%EndProlog
%%BeginSetup
%%EndSetup
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7 132 981 bf 0.386667 0 1 c 9 7 140 981 bf 9 7 149 981 bf 8 7 158 981 bf 9 7 166 981 bf 9 7 175 981 bf 8 7 184 981 bf 9 7 192 981 bf 9 7 201 981 bf 9 7 210 981 bf 8 7 219 981 bf 9 7 227 981 bf 9 7 236 981 bf 8 7 245 981 bf 9 7 253 981 bf 9 7 262 981
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550 981 bf 9 7 558 981 bf 9 7 645 981 bf 9 7 680 981 bf 9 7 793 981 bf 1 0 0 c 8 6 132 988 bf 0.386667 0 1 c 9 6 140 988 bf 9 6 149 988 bf 8 6 158 988 bf 9 6 166 988 bf 9 6 175 988 bf 8 6 184 988 bf 9 6 192 988 bf 9 6 201 988 bf 9 6 210 988 bf 8 6
219 988 bf 9 6 227 988 bf 9 6 236 988 bf 8 6 245 988 bf 9 6 253 988 bf 9 6 262 988 bf 9 6 271 988 bf 8 6 280 988 bf 9 6 288 988 bf 9 6 297 988 bf 8 6 306 988 bf 9 6 314 988 bf 9 6 323 988 bf 9 6 332 988 bf 8 6 341 988 bf 9 6 349 988 bf 9 6 358 988
bf 8 6 367 988 bf 9 6 375 988 bf 9 6 384 988 bf 8 6 393 988 bf 9 6 436 988 bf 9 6 445 988 bf 8 6 454 988 bf 9 6 471 988 bf 8 6 489 988 bf 9 6 532 988 bf 9 6 593 988 bf 9 6 654 988 bf 9 6 671 988 bf 9 6 741 988 bf 8 6 872 988 bf 0 1 0.986667 c 8 7
132 994 bf 0 1 0.52 c 9 7 140 994 bf 0.386667 0 1 c 9 7 149 994 bf 8 7 158 994 bf 9 7 166 994 bf 9 7 175 994 bf 8 7 184 994 bf 9 7 192 994 bf 9 7 201 994 bf 9 7 210 994 bf 8 7 219 994 bf 9 7 227 994 bf 9 7 236 994 bf 8 7 245 994 bf 9 7 253 994 bf 9
7 262 994 bf 9 7 271 994 bf 8 7 280 994 bf 9 7 288 994 bf 9 7 297 994 bf 8 7 306 994 bf 9 7 314 994 bf 9 7 323 994 bf 9 7 332 994 bf 8 7 341 994 bf 9 7 349 994 bf 8 7 367 994 bf 9 7 375 994 bf 9 7 384 994 bf 8 7 393 994 bf 9 7 401 994 bf 9 7 410 994
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1001 bf 8 7 219 1001 bf 9 7 227 1001 bf 9 7 236 1001 bf 8 7 245 1001 bf 9 7 253 1001 bf 9 7 262 1001 bf 9 7 271 1001 bf 8 7 280 1001 bf 9 7 288 1001 bf 9 7 297 1001 bf 8 7 306 1001 bf 9 7 314 1001 bf 9 7 323 1001 bf 9 7 332 1001 bf 8 7 341 1001 bf 9
7 358 1001 bf 8 7 367 1001 bf 8 7 393 1001 bf 9 7 401 1001 bf 9 7 419 1001 bf 8 7 428 1001 bf 9 7 445 1001 bf 9 7 471 1001 bf 9 7 480 1001 bf 9 7 506 1001 bf 9 7 541 1001 bf 9 7 567 1001 bf 8 7 602 1001 bf 9 7 750 1001 bf 9 7 915 1001 bf 8 7 132
1008 bf 0 0.546666 1 c 9 7 140 1008 bf 0.2 0 1 c 9 7 149 1008 bf 0.386667 0 1 c 8 7 158 1008 bf 9 7 166 1008 bf 9 7 175 1008 bf 8 7 184 1008 bf 9 7 192 1008 bf 9 7 201 1008 bf 9 7 210 1008 bf 8 7 219 1008 bf 9 7 227 1008 bf 9 7 236 1008 bf 8 7 245
1008 bf 9 7 253 1008 bf 9 7 262 1008 bf 9 7 271 1008 bf 8 7 280 1008 bf 9 7 288 1008 bf 9 7 297 1008 bf 8 7 306 1008 bf 9 7 314 1008 bf 9 7 323 1008 bf 9 7 332 1008 bf 8 7 341 1008 bf 9 7 349 1008 bf 9 7 358 1008 bf 8 7 367 1008 bf 9 7 375 1008 bf 9
7 384 1008 bf 8 7 393 1008 bf 9 7 410 1008 bf 9 7 436 1008 bf 9 7 462 1008 bf 9 7 497 1008 bf 9 7 593 1008 bf 9 7 819 1008 bf 9 7 828 1008 bf 9 7 924 1008 bf 9 6 140 1015 bf 0 0.0800001 1 c 9 6 149 1015 bf 0.386667 0 1 c 8 6 158 1015 bf 9 6 166 1015
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306 1015 bf 9 6 314 1015 bf 9 6 323 1015 bf 9 6 332 1015 bf 8 6 341 1015 bf 9 6 349 1015 bf 8 6 367 1015 bf 9 6 375 1015 bf 8 6 393 1015 bf 9 6 401 1015 bf 9 6 419 1015 bf 9 6 445 1015 bf 8 6 454 1015 bf 9 6 497 1015 bf 9 6 506 1015 bf 8 6 550 1015
bf 9 6 619 1015 bf 9 6 645 1015 bf 9 6 880 1015 bf 9 6 924 1015 bf 9 7 140 1021 bf 0.2 0 1 c 9 7 149 1021 bf 0.386667 0 1 c 8 7 158 1021 bf 9 7 166 1021 bf 9 7 175 1021 bf 8 7 184 1021 bf 9 7 192 1021 bf 9 7 201 1021 bf 9 7 210 1021 bf 8 7 219 1021
bf 9 7 227 1021 bf 9 7 236 1021 bf 8 7 245 1021 bf 9 7 253 1021 bf 9 7 262 1021 bf 9 7 271 1021 bf 8 7 280 1021 bf 9 7 288 1021 bf 9 7 297 1021 bf 8 7 306 1021 bf 9 7 314 1021 bf 9 7 332 1021 bf 9 7 358 1021 bf 8 7 367 1021 bf 9 7 401 1021 bf 9 7
462 1021 bf 8 7 515 1021 bf 9 7 610 1021 bf 9 7 680 1021 bf 9 7 732 1021 bf 9 7 828 1021 bf 9 7 967 1021 bf 9 7 976 1021 bf 9 7 149 1028 bf 8 7 158 1028 bf 9 7 166 1028 bf 9 7 175 1028 bf 8 7 184 1028 bf 9 7 192 1028 bf 9 7 201 1028 bf 9 7 210 1028
bf 8 7 219 1028 bf 9 7 227 1028 bf 9 7 236 1028 bf 8 7 245 1028 bf 9 7 253 1028 bf 9 7 262 1028 bf 9 7 271 1028 bf 8 7 280 1028 bf 9 7 288 1028 bf 9 7 297 1028 bf 8 7 306 1028 bf 9 7 314 1028 bf 9 7 323 1028 bf 9 7 332 1028 bf 8 7 341 1028 bf 9 7
358 1028 bf 9 7 375 1028 bf 8 7 393 1028 bf 9 7 401 1028 bf 8 7 428 1028 bf 9 7 480 1028 bf 9 7 680 1028 bf 9 7 715 1028 bf 9 7 802 1028 bf 9 7 854 1028 bf 8 7 872 1028 bf 8 7 959 1028 bf 9 7 967 1028 bf 9 7 976 1028 bf 8 7 994 1028 bf 9 7 149 1035
bf 8 7 158 1035 bf 9 7 166 1035 bf 9 7 175 1035 bf 8 7 184 1035 bf 9 7 192 1035 bf 9 7 201 1035 bf 9 7 210 1035 bf 8 7 219 1035 bf 9 7 227 1035 bf 9 7 236 1035 bf 8 7 245 1035 bf 9 7 253 1035 bf 9 7 262 1035 bf 9 7 271 1035 bf 8 7 280 1035 bf 9 7
288 1035 bf 9 7 297 1035 bf 9 7 358 1035 bf 9 7 384 1035 bf 8 7 393 1035 bf 9 7 480 1035 bf 9 7 828 1035 bf 8 7 846 1035 bf 8 7 872 1035 bf 9 7 889 1035 bf 8 7 933 1035 bf 9 7 941 1035 bf 8 7 959 1035 bf 9 7 967 1035 bf 9 7 985 1035 bf 8 6 158 1042
bf 9 6 166 1042 bf 9 6 175 1042 bf 8 6 184 1042 bf 9 6 192 1042 bf 9 6 201 1042 bf 9 6 210 1042 bf 8 6 219 1042 bf 9 6 227 1042 bf 9 6 236 1042 bf 8 6 245 1042 bf 9 6 253 1042 bf 9 6 262 1042 bf 9 6 271 1042 bf 8 6 280 1042 bf 9 6 297 1042 bf 8 6
306 1042 bf 9 6 323 1042 bf 9 6 349 1042 bf 9 6 558 1042 bf 9 6 593 1042 bf 8 6 759 1042 bf 9 6 776 1042 bf 8 6 872 1042 bf 9 6 889 1042 bf 9 6 898 1042 bf 8 6 907 1042 bf 9 6 915 1042 bf 8 6 933 1042 bf 9 6 941 1042 bf 9 6 950 1042 bf 8 6 959 1042
bf 9 6 967 1042 bf 9 6 985 1042 bf 8 6 994 1042 bf 8 7 158 1048 bf 9 7 166 1048 bf 9 7 175 1048 bf 8 7 184 1048 bf 9 7 192 1048 bf 9 7 201 1048 bf 9 7 210 1048 bf 8 7 219 1048 bf 9 7 236 1048 bf 9 7 253 1048 bf 9 7 271 1048 bf 9 7 288 1048 bf 9 7
297 1048 bf 9 7 314 1048 bf 9 7 349 1048 bf 8 7 367 1048 bf 9 7 375 1048 bf 9 7 384 1048 bf 8 7 454 1048 bf 9 7 541 1048 bf 8 7 663 1048 bf 8 7 759 1048 bf 9 7 767 1048 bf 8 7 785 1048 bf 9 7 828 1048 bf 9 7 854 1048 bf 9 7 863 1048 bf 8 7 872 1048
bf 9 7 880 1048 bf 9 7 898 1048 bf 8 7 907 1048 bf 9 7 915 1048 bf 9 7 941 1048 bf 8 7 959 1048 bf 9 7 967 1048 bf 9 7 976 1048 bf 9 7 985 1048 bf 9 7 166 1055 bf 9 7 175 1055 bf 8 7 184 1055 bf 9 7 210 1055 bf 8 7 219 1055 bf 9 7 227 1055 bf 9 7
236 1055 bf 9 7 271 1055 bf 8 7 280 1055 bf 9 7 288 1055 bf 9 7 314 1055 bf 9 7 332 1055 bf 8 7 393 1055 bf 9 7 558 1055 bf 9 7 584 1055 bf 8 7 698 1055 bf 9 7 706 1055 bf 9 7 741 1055 bf 9 7 767 1055 bf 8 7 785 1055 bf 9 7 793 1055 bf 8 7 811 1055
bf 9 7 819 1055 bf 9 7 828 1055 bf 9 7 837 1055 bf 9 7 854 1055 bf 8 7 872 1055 bf 9 7 880 1055 bf 9 7 889 1055 bf 9 7 898 1055 bf 8 7 907 1055 bf 9 7 915 1055 bf 9 7 924 1055 bf 8 7 933 1055 bf 9 7 941 1055 bf 9 7 950 1055 bf 9 7 985 1055 bf 8 7
994 1055 bf 9 7 166 1062 bf 9 7 175 1062 bf 8 7 184 1062 bf 9 7 192 1062 bf 8 7 219 1062 bf 9 7 236 1062 bf 9 7 262 1062 bf 9 7 271 1062 bf 9 7 288 1062 bf 9 7 297 1062 bf 8 7 306 1062 bf 9 7 314 1062 bf 9 7 384 1062 bf 8 7 428 1062 bf 8 7 489 1062
bf 9 7 593 1062 bf 9 7 645 1062 bf 9 7 671 1062 bf 9 7 680 1062 bf 9 7 689 1062 bf 8 7 698 1062 bf 9 7 706 1062 bf 9 7 715 1062 bf 8 7 724 1062 bf 9 7 732 1062 bf 9 7 741 1062 bf 9 7 767 1062 bf 8 7 785 1062 bf 9 7 793 1062 bf 8 7 811 1062 bf 9 7
828 1062 bf 9 7 837 1062 bf 8 7 846 1062 bf 8 7 872 1062 bf 9 7 880 1062 bf 9 7 889 1062 bf 9 7 898 1062 bf 8 7 907 1062 bf 9 7 915 1062 bf 9 7 924 1062 bf 8 7 933 1062 bf 9 7 941 1062 bf 9 7 950 1062 bf 8 7 959 1062 bf 9 7 967 1062 bf 9 7 976 1062
bf 9 7 985 1062 bf 9 6 175 1069 bf 8 6 184 1069 bf 9 6 201 1069 bf 9 6 210 1069 bf 8 6 245 1069 bf 9 6 262 1069 bf 9 6 271 1069 bf 9 6 288 1069 bf 9 6 314 1069 bf 9 6 323 1069 bf 9 6 332 1069 bf 9 6 384 1069 bf 8 6 637 1069 bf 9 6 645 1069 bf 9 6
671 1069 bf 9 6 680 1069 bf 9 6 689 1069 bf 9 6 706 1069 bf 9 6 715 1069 bf 8 6 724 1069 bf 9 6 732 1069 bf 9 6 741 1069 bf 9 6 750 1069 bf 8 6 759 1069 bf 9 6 767 1069 bf 9 6 776 1069 bf 8 6 785 1069 bf 9 6 793 1069 bf 9 6 802 1069 bf 8 6 811 1069
bf 9 6 828 1069 bf 9 6 837 1069 bf 8 6 846 1069 bf 9 6 854 1069 bf 9 6 863 1069 bf 8 6 872 1069 bf 9 6 880 1069 bf 9 6 889 1069 bf 9 6 898 1069 bf 8 6 907 1069 bf 9 6 915 1069 bf 9 6 924 1069 bf 8 6 933 1069 bf 9 6 941 1069 bf 9 6 950 1069 bf 8 6
959 1069 bf 9 6 967 1069 bf 9 6 976 1069 bf 9 6 985 1069 bf 8 6 994 1069 bf 9 7 175 1075 bf 8 7 184 1075 bf 9 7 201 1075 bf 9 7 236 1075 bf 9 7 253 1075 bf 9 7 262 1075 bf 9 7 271 1075 bf 8 7 280 1075 bf 9 7 297 1075 bf 8 7 306 1075 bf 9 7 314 1075
bf 8 7 341 1075 bf 9 7 358 1075 bf 9 7 584 1075 bf 8 7 602 1075 bf 9 7 619 1075 bf 9 7 628 1075 bf 8 7 637 1075 bf 9 7 645 1075 bf 9 7 654 1075 bf 8 7 663 1075 bf 9 7 671 1075 bf 9 7 680 1075 bf 9 7 689 1075 bf 9 7 706 1075 bf 9 7 715 1075 bf 8 7
724 1075 bf 9 7 732 1075 bf 9 7 741 1075 bf 9 7 750 1075 bf 8 7 759 1075 bf 9 7 767 1075 bf 9 7 776 1075 bf 8 7 785 1075 bf 9 7 793 1075 bf 9 7 802 1075 bf 8 7 811 1075 bf 9 7 819 1075 bf 9 7 828 1075 bf 9 7 837 1075 bf 8 7 846 1075 bf 9 7 854 1075
bf 9 7 863 1075 bf 8 7 872 1075 bf 9 7 880 1075 bf 9 7 889 1075 bf 9 7 898 1075 bf 9 7 915 1075 bf 9 7 924 1075 bf 8 7 933 1075 bf 9 7 941 1075 bf 9 7 950 1075 bf 8 7 959 1075 bf 9 7 967 1075 bf 9 7 976 1075 bf 9 7 985 1075 bf 8 7 994 1075 bf 9 7
175 1082 bf 8 7 184 1082 bf 9 7 192 1082 bf 8 7 219 1082 bf 9 7 253 1082 bf 9 7 262 1082 bf 8 7 280 1082 bf 9 7 297 1082 bf 8 7 306 1082 bf 8 7 341 1082 bf 9 7 375 1082 bf 9 7 593 1082 bf 9 7 610 1082 bf 9 7 619 1082 bf 8 7 637 1082 bf 9 7 645 1082
bf 9 7 654 1082 bf 8 7 663 1082 bf 9 7 671 1082 bf 9 7 680 1082 bf 9 7 689 1082 bf 8 7 698 1082 bf 9 7 706 1082 bf 9 7 715 1082 bf 8 7 724 1082 bf 9 7 732 1082 bf 9 7 741 1082 bf 9 7 750 1082 bf 8 7 759 1082 bf 9 7 767 1082 bf 9 7 776 1082 bf 8 7
785 1082 bf 9 7 793 1082 bf 9 7 802 1082 bf 8 7 811 1082 bf 9 7 819 1082 bf 9 7 828 1082 bf 9 7 837 1082 bf 8 7 846 1082 bf 9 7 854 1082 bf 9 7 863 1082 bf 8 7 872 1082 bf 9 7 880 1082 bf 9 7 889 1082 bf 9 7 898 1082 bf 8 7 907 1082 bf 9 7 915 1082
bf 9 7 924 1082 bf 8 7 933 1082 bf 9 7 941 1082 bf 8 7 959 1082 bf 9 7 967 1082 bf 9 7 976 1082 bf 8 7 994 1082 bf 8 7 184 1089 bf 9 7 192 1089 bf 9 7 236 1089 bf 8 7 245 1089 bf 9 7 271 1089 bf 8 7 306 1089 bf 8 7 341 1089 bf 9 7 558 1089 bf 9 7
567 1089 bf 9 7 584 1089 bf 8 7 602 1089 bf 9 7 610 1089 bf 9 7 619 1089 bf 9 7 628 1089 bf 8 7 637 1089 bf 9 7 645 1089 bf 9 7 654 1089 bf 8 7 663 1089 bf 9 7 671 1089 bf 9 7 680 1089 bf 9 7 689 1089 bf 8 7 698 1089 bf 9 7 706 1089 bf 9 7 715 1089
bf 8 7 724 1089 bf 9 7 732 1089 bf 9 7 741 1089 bf 9 7 750 1089 bf 8 7 759 1089 bf 9 7 767 1089 bf 9 7 776 1089 bf 8 7 785 1089 bf 9 7 802 1089 bf 8 7 811 1089 bf 9 7 819 1089 bf 9 7 828 1089 bf 9 7 837 1089 bf 8 7 846 1089 bf 9 7 854 1089 bf 9 7
863 1089 bf 8 7 872 1089 bf 9 7 880 1089 bf 9 7 889 1089 bf 9 7 898 1089 bf 8 7 907 1089 bf 9 7 915 1089 bf 8 7 933 1089 bf 9 7 950 1089 bf 8 7 959 1089 bf 9 7 967 1089 bf 9 7 985 1089 bf 8 7 994 1089 bf 8 6 184 1096 bf 9 6 192 1096 bf 9 6 210 1096
bf 8 6 306 1096 bf 9 6 314 1096 bf 9 6 332 1096 bf 9 6 541 1096 bf 8 6 550 1096 bf 9 6 558 1096 bf 9 6 567 1096 bf 8 6 576 1096 bf 9 6 593 1096 bf 8 6 602 1096 bf 9 6 610 1096 bf 9 6 619 1096 bf 9 6 628 1096 bf 9 6 645 1096 bf 9 6 654 1096 bf 8 6
663 1096 bf 9 6 671 1096 bf 9 6 680 1096 bf 9 6 689 1096 bf 8 6 698 1096 bf 9 6 706 1096 bf 9 6 715 1096 bf 8 6 724 1096 bf 9 6 732 1096 bf 9 6 741 1096 bf 9 6 750 1096 bf 8 6 759 1096 bf 9 6 767 1096 bf 9 6 776 1096 bf 8 6 785 1096 bf 9 6 793 1096
bf 9 6 802 1096 bf 8 6 811 1096 bf 9 6 819 1096 bf 9 6 828 1096 bf 9 6 837 1096 bf 8 6 846 1096 bf 9 6 854 1096 bf 9 6 863 1096 bf 8 6 872 1096 bf 9 6 880 1096 bf 9 6 889 1096 bf 9 6 898 1096 bf 8 6 907 1096 bf 9 6 915 1096 bf 9 6 924 1096 bf 8 6
933 1096 bf 9 6 941 1096 bf 9 6 950 1096 bf 8 6 959 1096 bf 9 6 976 1096 bf 9 6 985 1096 bf 8 6 994 1096 bf 9 7 192 1102 bf 9 7 201 1102 bf 9 7 210 1102 bf 9 7 236 1102 bf 8 7 245 1102 bf 9 7 262 1102 bf 9 7 271 1102 bf 9 7 480 1102 bf 8 7 515 1102
bf 9 7 532 1102 bf 9 7 558 1102 bf 8 7 576 1102 bf 9 7 584 1102 bf 9 7 593 1102 bf 9 7 610 1102 bf 9 7 619 1102 bf 9 7 628 1102 bf 8 7 637 1102 bf 9 7 645 1102 bf 9 7 654 1102 bf 8 7 663 1102 bf 9 7 671 1102 bf 9 7 680 1102 bf 9 7 689 1102 bf 8 7
698 1102 bf 9 7 706 1102 bf 9 7 715 1102 bf 8 7 724 1102 bf 9 7 732 1102 bf 9 7 741 1102 bf 9 7 750 1102 bf 8 7 759 1102 bf 9 7 767 1102 bf 9 7 776 1102 bf 8 7 785 1102 bf 9 7 793 1102 bf 9 7 802 1102 bf 8 7 811 1102 bf 9 7 819 1102 bf 9 7 828 1102
bf 9 7 837 1102 bf 9 7 854 1102 bf 9 7 863 1102 bf 8 7 872 1102 bf 9 7 880 1102 bf 9 7 889 1102 bf 9 7 898 1102 bf 8 7 907 1102 bf 9 7 924 1102 bf 9 7 941 1102 bf 9 7 967 1102 bf 9 7 976 1102 bf 9 7 985 1102 bf 8 7 994 1102 bf 9 7 192 1109 bf 9 7
201 1109 bf 9 7 253 1109 bf 8 7 280 1109 bf 9 7 288 1109 bf 9 7 401 1109 bf 9 7 471 1109 bf 8 7 515 1109 bf 9 7 523 1109 bf 9 7 532 1109 bf 9 7 541 1109 bf 8 7 550 1109 bf 9 7 558 1109 bf 9 7 567 1109 bf 8 7 576 1109 bf 9 7 584 1109 bf 9 7 593 1109
bf 8 7 602 1109 bf 9 7 610 1109 bf 9 7 619 1109 bf 9 7 628 1109 bf 8 7 637 1109 bf 9 7 645 1109 bf 9 7 654 1109 bf 8 7 663 1109 bf 9 7 671 1109 bf 9 7 680 1109 bf 9 7 689 1109 bf 8 7 698 1109 bf 9 7 706 1109 bf 9 7 715 1109 bf 8 7 724 1109 bf 9 7
732 1109 bf 9 7 741 1109 bf 9 7 750 1109 bf 8 7 759 1109 bf 9 7 767 1109 bf 9 7 776 1109 bf 8 7 785 1109 bf 9 7 793 1109 bf 9 7 802 1109 bf 8 7 811 1109 bf 9 7 819 1109 bf 9 7 828 1109 bf 8 7 846 1109 bf 9 7 854 1109 bf 9 7 863 1109 bf 8 7 872 1109
bf 9 7 880 1109 bf 9 7 898 1109 bf 8 7 907 1109 bf 9 7 915 1109 bf 9 7 924 1109 bf 8 7 933 1109 bf 9 7 941 1109 bf 9 7 950 1109 bf 9 7 967 1109 bf 9 7 201 1116 bf 9 7 210 1116 bf 9 7 227 1116 bf 8 7 341 1116 bf 9 7 480 1116 bf 8 7 489 1116 bf 9 7
497 1116 bf 9 7 506 1116 bf 8 7 515 1116 bf 9 7 523 1116 bf 9 7 532 1116 bf 8 7 550 1116 bf 9 7 558 1116 bf 9 7 567 1116 bf 8 7 576 1116 bf 9 7 584 1116 bf 9 7 593 1116 bf 8 7 602 1116 bf 9 7 610 1116 bf 9 7 619 1116 bf 9 7 628 1116 bf 8 7 637 1116
bf 9 7 645 1116 bf 9 7 654 1116 bf 8 7 663 1116 bf 9 7 671 1116 bf 9 7 680 1116 bf 9 7 689 1116 bf 8 7 698 1116 bf 9 7 706 1116 bf 9 7 715 1116 bf 8 7 724 1116 bf 9 7 732 1116 bf 9 7 741 1116 bf 9 7 750 1116 bf 8 7 759 1116 bf 9 7 767 1116 bf 9 7
776 1116 bf 8 7 785 1116 bf 9 7 793 1116 bf 9 7 802 1116 bf 8 7 811 1116 bf 9 7 828 1116 bf 9 7 837 1116 bf 9 7 854 1116 bf 9 7 863 1116 bf 8 7 872 1116 bf 9 7 880 1116 bf 8 7 907 1116 bf 9 7 915 1116 bf 9 7 924 1116 bf 8 7 933 1116 bf 9 7 950 1116
bf 9 7 967 1116 bf 9 7 985 1116 bf 9 6 201 1123 bf 9 6 210 1123 bf 9 6 297 1123 bf 9 6 419 1123 bf 9 6 480 1123 bf 8 6 489 1123 bf 9 6 497 1123 bf 9 6 506 1123 bf 8 6 515 1123 bf 9 6 523 1123 bf 9 6 532 1123 bf 9 6 541 1123 bf 8 6 550 1123 bf 9 6
558 1123 bf 9 6 567 1123 bf 8 6 576 1123 bf 9 6 584 1123 bf 9 6 593 1123 bf 8 6 602 1123 bf 9 6 610 1123 bf 9 6 619 1123 bf 9 6 628 1123 bf 8 6 637 1123 bf 9 6 645 1123 bf 9 6 654 1123 bf 8 6 663 1123 bf 9 6 671 1123 bf 9 6 680 1123 bf 9 6 689 1123
bf 8 6 698 1123 bf 9 6 706 1123 bf 9 6 715 1123 bf 8 6 724 1123 bf 9 6 732 1123 bf 9 6 741 1123 bf 9 6 750 1123 bf 8 6 759 1123 bf 9 6 767 1123 bf 8 6 785 1123 bf 8 6 811 1123 bf 9 6 819 1123 bf 9 6 828 1123 bf 9 6 837 1123 bf 8 6 846 1123 bf 9 6
854 1123 bf 9 6 863 1123 bf 8 6 872 1123 bf 9 6 889 1123 bf 9 6 898 1123 bf 8 6 907 1123 bf 9 6 924 1123 bf 9 6 941 1123 bf 9 6 950 1123 bf 9 6 976 1123 bf 9 6 985 1123 bf 9 7 210 1129 bf 8 7 245 1129 bf 9 7 253 1129 bf 9 7 288 1129 bf 9 7 323 1129
bf 8 7 341 1129 bf 8 7 454 1129 bf 9 7 462 1129 bf 9 7 471 1129 bf 8 7 489 1129 bf 9 7 497 1129 bf 9 7 506 1129 bf 8 7 515 1129 bf 9 7 523 1129 bf 9 7 532 1129 bf 9 7 541 1129 bf 8 7 550 1129 bf 9 7 558 1129 bf 9 7 567 1129 bf 8 7 576 1129 bf 9 7
584 1129 bf 9 7 593 1129 bf 8 7 602 1129 bf 9 7 610 1129 bf 9 7 619 1129 bf 9 7 628 1129 bf 8 7 637 1129 bf 9 7 645 1129 bf 9 7 654 1129 bf 8 7 663 1129 bf 9 7 671 1129 bf 9 7 680 1129 bf 9 7 689 1129 bf 8 7 698 1129 bf 9 7 706 1129 bf 9 7 715 1129
bf 8 7 724 1129 bf 9 7 732 1129 bf 9 7 741 1129 bf 9 7 750 1129 bf 9 7 776 1129 bf 8 7 785 1129 bf 8 7 811 1129 bf 9 7 828 1129 bf 8 7 846 1129 bf 9 7 854 1129 bf 9 7 863 1129 bf 9 7 889 1129 bf 9 7 915 1129 bf 9 7 924 1129 bf 8 7 959 1129 bf 9 7
967 1129 bf 9 7 976 1129 bf 8 7 994 1129 bf 9 7 210 1136 bf 8 7 219 1136 bf 9 7 262 1136 bf 8 7 280 1136 bf 9 7 445 1136 bf 8 7 454 1136 bf 9 7 462 1136 bf 9 7 471 1136 bf 9 7 480 1136 bf 8 7 489 1136 bf 9 7 497 1136 bf 9 7 506 1136 bf 8 7 515 1136
bf 9 7 523 1136 bf 9 7 532 1136 bf 9 7 541 1136 bf 8 7 550 1136 bf 9 7 558 1136 bf 9 7 567 1136 bf 8 7 576 1136 bf 9 7 584 1136 bf 9 7 593 1136 bf 8 7 602 1136 bf 9 7 610 1136 bf 9 7 619 1136 bf 9 7 628 1136 bf 8 7 637 1136 bf 9 7 645 1136 bf 9 7
654 1136 bf 8 7 663 1136 bf 9 7 671 1136 bf 9 7 680 1136 bf 9 7 689 1136 bf 8 7 698 1136 bf 9 7 706 1136 bf 9 7 715 1136 bf 8 7 724 1136 bf 9 7 741 1136 bf 9 7 750 1136 bf 8 7 759 1136 bf 9 7 767 1136 bf 9 7 776 1136 bf 9 7 793 1136 bf 9 7 802 1136
bf 8 7 811 1136 bf 9 7 819 1136 bf 9 7 828 1136 bf 9 7 837 1136 bf 9 7 854 1136 bf 9 7 863 1136 bf 8 7 872 1136 bf 9 7 889 1136 bf 8 7 907 1136 bf 9 7 915 1136 bf 9 7 924 1136 bf 8 7 933 1136 bf 9 7 985 1136 bf 9 7 210 1143 bf 8 7 219 1143 bf 9 7
236 1143 bf 9 7 410 1143 bf 9 7 419 1143 bf 9 7 436 1143 bf 9 7 445 1143 bf 8 7 454 1143 bf 9 7 462 1143 bf 9 7 471 1143 bf 9 7 480 1143 bf 8 7 489 1143 bf 9 7 506 1143 bf 8 7 515 1143 bf 9 7 523 1143 bf 9 7 532 1143 bf 9 7 541 1143 bf 8 7 550 1143
bf 9 7 558 1143 bf 9 7 567 1143 bf 8 7 576 1143 bf 9 7 584 1143 bf 9 7 593 1143 bf 8 7 602 1143 bf 9 7 610 1143 bf 9 7 619 1143 bf 9 7 628 1143 bf 8 7 637 1143 bf 9 7 645 1143 bf 9 7 654 1143 bf 8 7 663 1143 bf 9 7 680 1143 bf 9 7 689 1143 bf 8 7
698 1143 bf 9 7 706 1143 bf 9 7 715 1143 bf 8 7 724 1143 bf 9 7 741 1143 bf 9 7 750 1143 bf 8 7 759 1143 bf 9 7 793 1143 bf 8 7 811 1143 bf 9 7 837 1143 bf 8 7 846 1143 bf 9 7 854 1143 bf 9 7 863 1143 bf 8 7 872 1143 bf 9 7 880 1143 bf 9 7 898 1143
bf 8 7 907 1143 bf 9 7 924 1143 bf 9 7 941 1143 bf 9 7 950 1143 bf 8 7 959 1143 bf 9 7 967 1143 bf 9 7 976 1143 bf 8 6 219 1150 bf 9 6 227 1150 bf 8 6 245 1150 bf 9 6 436 1150 bf 9 6 445 1150 bf 8 6 454 1150 bf 9 6 462 1150 bf 9 6 471 1150 bf 9 6
480 1150 bf 8 6 489 1150 bf 9 6 497 1150 bf 9 6 506 1150 bf 8 6 515 1150 bf 9 6 523 1150 bf 9 6 532 1150 bf 9 6 541 1150 bf 8 6 550 1150 bf 9 6 558 1150 bf 9 6 567 1150 bf 8 6 576 1150 bf 9 6 584 1150 bf 9 6 593 1150 bf 8 6 602 1150 bf 9 6 610 1150
bf 9 6 619 1150 bf 9 6 628 1150 bf 8 6 637 1150 bf 9 6 645 1150 bf 9 6 654 1150 bf 8 6 663 1150 bf 9 6 671 1150 bf 9 6 680 1150 bf 9 6 689 1150 bf 8 6 698 1150 bf 9 6 715 1150 bf 9 6 732 1150 bf 9 6 741 1150 bf 9 6 750 1150 bf 9 6 776 1150 bf 8 6
785 1150 bf 9 6 793 1150 bf 9 6 802 1150 bf 8 6 811 1150 bf 9 6 828 1150 bf 9 6 837 1150 bf 9 6 854 1150 bf 8 6 872 1150 bf 9 6 880 1150 bf 9 6 889 1150 bf 9 6 898 1150 bf 8 6 907 1150 bf 8 7 219 1156 bf 9 7 227 1156 bf 9 7 401 1156 bf 9 7 419 1156
bf 9 7 445 1156 bf 8 7 454 1156 bf 9 7 462 1156 bf 9 7 471 1156 bf 9 7 480 1156 bf 8 7 489 1156 bf 9 7 497 1156 bf 9 7 506 1156 bf 8 7 515 1156 bf 9 7 523 1156 bf 9 7 532 1156 bf 9 7 541 1156 bf 8 7 550 1156 bf 9 7 558 1156 bf 9 7 567 1156 bf 8 7
576 1156 bf 9 7 584 1156 bf 9 7 593 1156 bf 8 7 602 1156 bf 9 7 610 1156 bf 9 7 619 1156 bf 9 7 628 1156 bf 8 7 637 1156 bf 9 7 645 1156 bf 8 7 663 1156 bf 9 7 671 1156 bf 9 7 680 1156 bf 8 7 698 1156 bf 9 7 715 1156 bf 8 7 724 1156 bf 9 7 732 1156
bf 8 7 759 1156 bf 9 7 776 1156 bf 8 7 785 1156 bf 8 7 811 1156 bf 9 7 828 1156 bf 8 7 846 1156 bf 9 7 854 1156 bf 9 7 863 1156 bf 8 7 872 1156 bf 9 7 880 1156 bf 9 7 889 1156 bf 9 7 898 1156 bf 9 7 924 1156 bf 9 7 941 1156 bf 9 7 976 1156 bf 9 7
985 1156 bf 9 7 227 1163 bf 9 7 262 1163 bf 9 7 419 1163 bf 8 7 428 1163 bf 9 7 436 1163 bf 9 7 445 1163 bf 8 7 454 1163 bf 9 7 462 1163 bf 9 7 471 1163 bf 9 7 480 1163 bf 8 7 489 1163 bf 9 7 497 1163 bf 9 7 506 1163 bf 8 7 515 1163 bf 9 7 523 1163
bf 9 7 532 1163 bf 9 7 541 1163 bf 8 7 550 1163 bf 9 7 558 1163 bf 9 7 567 1163 bf 8 7 576 1163 bf 9 7 584 1163 bf 9 7 593 1163 bf 9 7 610 1163 bf 9 7 619 1163 bf 9 7 628 1163 bf 9 7 671 1163 bf 9 7 689 1163 bf 9 7 706 1163 bf 9 7 715 1163 bf 9 7
732 1163 bf 9 7 741 1163 bf 9 7 750 1163 bf 9 7 767 1163 bf 9 7 776 1163 bf 8 7 785 1163 bf 9 7 802 1163 bf 9 7 828 1163 bf 9 7 837 1163 bf 8 7 846 1163 bf 9 7 854 1163 bf 9 7 863 1163 bf 9 7 898 1163 bf 8 7 907 1163 bf 9 7 915 1163 bf 8 7 959 1163
bf 8 7 994 1163 bf 9 7 227 1170 bf 9 7 236 1170 bf 9 7 271 1170 bf 9 7 384 1170 bf 8 7 393 1170 bf 9 7 401 1170 bf 9 7 410 1170 bf 9 7 419 1170 bf 8 7 428 1170 bf 9 7 436 1170 bf 9 7 445 1170 bf 8 7 454 1170 bf 9 7 462 1170 bf 9 7 471 1170 bf 9 7
480 1170 bf 8 7 489 1170 bf 9 7 497 1170 bf 9 7 506 1170 bf 8 7 515 1170 bf 9 7 523 1170 bf 9 7 532 1170 bf 9 7 541 1170 bf 8 7 550 1170 bf 9 7 558 1170 bf 9 7 567 1170 bf 8 7 576 1170 bf 9 7 584 1170 bf 9 7 593 1170 bf 8 7 602 1170 bf 9 7 610 1170
bf 9 7 619 1170 bf 9 7 628 1170 bf 9 7 671 1170 bf 9 7 689 1170 bf 8 7 698 1170 bf 9 7 715 1170 bf 8 7 724 1170 bf 9 7 732 1170 bf 9 7 741 1170 bf 9 7 750 1170 bf 8 7 759 1170 bf 9 7 776 1170 bf 8 7 785 1170 bf 8 7 811 1170 bf 9 7 837 1170 bf 8 7
846 1170 bf 9 7 854 1170 bf 9 7 889 1170 bf 8 7 907 1170 bf 9 7 915 1170 bf 9 7 924 1170 bf 9 7 950 1170 bf 9 7 967 1170 bf 9 6 227 1177 bf 9 6 236 1177 bf 9 6 401 1177 bf 9 6 410 1177 bf 9 6 419 1177 bf 8 6 428 1177 bf 9 6 436 1177 bf 9 6 445 1177
bf 8 6 454 1177 bf 9 6 462 1177 bf 9 6 471 1177 bf 9 6 480 1177 bf 8 6 489 1177 bf 9 6 497 1177 bf 9 6 506 1177 bf 8 6 515 1177 bf 9 6 523 1177 bf 9 6 532 1177 bf 9 6 541 1177 bf 9 6 558 1177 bf 9 6 567 1177 bf 9 6 584 1177 bf 9 6 610 1177 bf 9 6
619 1177 bf 9 6 628 1177 bf 8 6 637 1177 bf 9 6 654 1177 bf 8 6 663 1177 bf 9 6 671 1177 bf 9 6 689 1177 bf 8 6 698 1177 bf 9 6 706 1177 bf 8 6 724 1177 bf 9 6 732 1177 bf 9 6 741 1177 bf 9 6 750 1177 bf 8 6 759 1177 bf 9 6 767 1177 bf 9 6 776 1177
bf 8 6 785 1177 bf 8 6 811 1177 bf 9 6 828 1177 bf 9 6 837 1177 bf 9 6 915 1177 bf 9 6 924 1177 bf 8 6 959 1177 bf 9 6 976 1177 bf 9 6 985 1177 bf 8 6 994 1177 bf 9 7 236 1183 bf 8 7 245 1183 bf 9 7 375 1183 bf 9 7 384 1183 bf 8 7 393 1183 bf 9 7
401 1183 bf 9 7 410 1183 bf 9 7 419 1183 bf 8 7 428 1183 bf 9 7 436 1183 bf 9 7 445 1183 bf 8 7 454 1183 bf 9 7 462 1183 bf 9 7 471 1183 bf 9 7 480 1183 bf 8 7 489 1183 bf 9 7 497 1183 bf 9 7 506 1183 bf 8 7 515 1183 bf 9 7 523 1183 bf 9 7 541 1183
bf 9 7 558 1183 bf 9 7 567 1183 bf 9 7 584 1183 bf 9 7 593 1183 bf 8 7 602 1183 bf 8 7 637 1183 bf 9 7 645 1183 bf 9 7 654 1183 bf 8 7 663 1183 bf 9 7 671 1183 bf 9 7 680 1183 bf 9 7 689 1183 bf 8 7 698 1183 bf 9 7 706 1183 bf 8 7 724 1183 bf 9 7
741 1183 bf 9 7 750 1183 bf 8 7 759 1183 bf 9 7 767 1183 bf 9 7 776 1183 bf 8 7 785 1183 bf 9 7 802 1183 bf 8 7 811 1183 bf 9 7 819 1183 bf 8 7 846 1183 bf 9 7 854 1183 bf 9 7 915 1183 bf 9 7 941 1183 bf 9 7 950 1183 bf 9 7 985 1183 bf 9 7 236 1190
bf 8 7 245 1190 bf 8 7 367 1190 bf 9 7 375 1190 bf 9 7 384 1190 bf 8 7 393 1190 bf 9 7 401 1190 bf 9 7 410 1190 bf 9 7 419 1190 bf 8 7 428 1190 bf 9 7 436 1190 bf 9 7 445 1190 bf 8 7 454 1190 bf 9 7 462 1190 bf 9 7 471 1190 bf 9 7 480 1190 bf 8 7
489 1190 bf 9 7 497 1190 bf 9 7 506 1190 bf 8 7 515 1190 bf 9 7 523 1190 bf 9 7 532 1190 bf 9 7 541 1190 bf 8 7 550 1190 bf 9 7 558 1190 bf 9 7 584 1190 bf 9 7 593 1190 bf 9 7 610 1190 bf 9 7 619 1190 bf 9 7 628 1190 bf 9 7 654 1190 bf 8 7 663 1190
bf 9 7 680 1190 bf 9 7 706 1190 bf 9 7 715 1190 bf 8 7 724 1190 bf 9 7 732 1190 bf 9 7 741 1190 bf 9 7 750 1190 bf 9 7 776 1190 bf 8 7 785 1190 bf 9 7 793 1190 bf 9 7 802 1190 bf 8 7 811 1190 bf 9 7 854 1190 bf 9 7 863 1190 bf 9 7 880 1190 bf 9 7
985 1190 bf 8 7 994 1190 bf 8 7 245 1197 bf 9 7 358 1197 bf 9 7 375 1197 bf 8 7 393 1197 bf 9 7 401 1197 bf 9 7 410 1197 bf 9 7 419 1197 bf 8 7 428 1197 bf 9 7 436 1197 bf 9 7 445 1197 bf 8 7 454 1197 bf 9 7 462 1197 bf 9 7 480 1197 bf 8 7 489 1197
bf 9 7 497 1197 bf 9 7 506 1197 bf 8 7 515 1197 bf 9 7 523 1197 bf 9 7 541 1197 bf 9 7 558 1197 bf 8 7 576 1197 bf 9 7 610 1197 bf 9 7 619 1197 bf 9 7 628 1197 bf 8 7 637 1197 bf 9 7 645 1197 bf 8 7 663 1197 bf 9 7 680 1197 bf 9 7 689 1197 bf 8 7
698 1197 bf 9 7 715 1197 bf 8 7 724 1197 bf 9 7 741 1197 bf 8 7 759 1197 bf 9 7 776 1197 bf 8 7 811 1197 bf 9 7 828 1197 bf 9 7 898 1197 bf 9 7 950 1197 bf 8 6 245 1204 bf 9 6 253 1204 bf 9 6 358 1204 bf 9 6 375 1204 bf 9 6 384 1204 bf 9 6 401 1204
bf 9 6 410 1204 bf 9 6 419 1204 bf 8 6 428 1204 bf 9 6 436 1204 bf 9 6 445 1204 bf 8 6 454 1204 bf 9 6 462 1204 bf 9 6 471 1204 bf 9 6 480 1204 bf 8 6 489 1204 bf 9 6 497 1204 bf 9 6 506 1204 bf 8 6 515 1204 bf 9 6 523 1204 bf 9 6 532 1204 bf 9 6
541 1204 bf 8 6 550 1204 bf 8 6 576 1204 bf 9 6 584 1204 bf 8 6 602 1204 bf 9 6 619 1204 bf 9 6 628 1204 bf 8 6 637 1204 bf 9 6 645 1204 bf 8 6 663 1204 bf 9 6 680 1204 bf 9 6 689 1204 bf 9 6 715 1204 bf 8 6 724 1204 bf 8 6 759 1204 bf 9 6 767 1204
bf 8 6 785 1204 bf 9 6 828 1204 bf 9 6 837 1204 bf 8 6 872 1204 bf 9 6 898 1204 bf 8 6 907 1204 bf 9 6 915 1204 bf 9 6 924 1204 bf 8 7 245 1210 bf 9 7 253 1210 bf 8 7 367 1210 bf 9 7 384 1210 bf 8 7 393 1210 bf 9 7 401 1210 bf 9 7 410 1210 bf 9 7
419 1210 bf 8 7 428 1210 bf 9 7 436 1210 bf 9 7 445 1210 bf 8 7 454 1210 bf 9 7 462 1210 bf 9 7 471 1210 bf 9 7 480 1210 bf 8 7 489 1210 bf 9 7 497 1210 bf 9 7 506 1210 bf 9 7 523 1210 bf 8 7 550 1210 bf 9 7 567 1210 bf 8 7 602 1210 bf 9 7 610 1210
bf 9 7 619 1210 bf 9 7 628 1210 bf 8 7 637 1210 bf 9 7 645 1210 bf 9 7 671 1210 bf 9 7 706 1210 bf 9 7 715 1210 bf 8 7 724 1210 bf 9 7 741 1210 bf 9 7 750 1210 bf 9 7 767 1210 bf 8 7 811 1210 bf 8 7 846 1210 bf 9 7 854 1210 bf 9 7 863 1210 bf 8 7
872 1210 bf 9 7 898 1210 bf 8 7 933 1210 bf 9 7 253 1217 bf 9 7 262 1217 bf 9 7 349 1217 bf 8 7 367 1217 bf 9 7 375 1217 bf 9 7 384 1217 bf 8 7 393 1217 bf 9 7 401 1217 bf 9 7 410 1217 bf 9 7 419 1217 bf 8 7 428 1217 bf 9 7 436 1217 bf 9 7 445 1217
bf 8 7 454 1217 bf 9 7 462 1217 bf 9 7 471 1217 bf 9 7 497 1217 bf 8 7 515 1217 bf 9 7 532 1217 bf 8 7 550 1217 bf 9 7 567 1217 bf 8 7 576 1217 bf 9 7 584 1217 bf 8 7 602 1217 bf 9 7 610 1217 bf 9 7 619 1217 bf 9 7 628 1217 bf 8 7 637 1217 bf 9 7
645 1217 bf 9 7 654 1217 bf 8 7 663 1217 bf 8 7 698 1217 bf 9 7 706 1217 bf 8 7 724 1217 bf 9 7 750 1217 bf 8 7 811 1217 bf 9 7 828 1217 bf 9 7 837 1217 bf 9 7 854 1217 bf 9 7 898 1217 bf 9 7 924 1217 bf 9 7 950 1217 bf 9 7 253 1224 bf 9 7 262 1224
bf 9 7 358 1224 bf 8 7 367 1224 bf 9 7 375 1224 bf 9 7 384 1224 bf 8 7 393 1224 bf 9 7 401 1224 bf 9 7 410 1224 bf 9 7 419 1224 bf 8 7 428 1224 bf 9 7 436 1224 bf 9 7 445 1224 bf 8 7 454 1224 bf 9 7 462 1224 bf 9 7 471 1224 bf 9 7 480 1224 bf 9 7
506 1224 bf 8 7 515 1224 bf 9 7 523 1224 bf 8 7 550 1224 bf 9 7 558 1224 bf 9 7 567 1224 bf 8 7 576 1224 bf 8 7 637 1224 bf 9 7 654 1224 bf 8 7 663 1224 bf 9 7 671 1224 bf 9 7 689 1224 bf 8 7 698 1224 bf 9 7 715 1224 bf 8 7 724 1224 bf 9 7 750 1224
bf 8 7 785 1224 bf 8 7 811 1224 bf 9 7 967 1224 bf 9 6 262 1231 bf 9 6 271 1231 bf 9 6 349 1231 bf 9 6 358 1231 bf 8 6 367 1231 bf 9 6 375 1231 bf 9 6 384 1231 bf 8 6 393 1231 bf 9 6 401 1231 bf 9 6 410 1231 bf 9 6 419 1231 bf 8 6 428 1231 bf 9 6
436 1231 bf 9 6 445 1231 bf 8 6 454 1231 bf 9 6 462 1231 bf 9 6 471 1231 bf 9 6 480 1231 bf 8 6 515 1231 bf 8 6 550 1231 bf 9 6 558 1231 bf 9 6 567 1231 bf 9 6 593 1231 bf 8 6 602 1231 bf 9 6 619 1231 bf 9 6 645 1231 bf 9 6 654 1231 bf 8 6 663 1231
bf 8 6 724 1231 bf 8 6 759 1231 bf 9 6 802 1231 bf 8 6 811 1231 bf 9 6 819 1231 bf 9 6 837 1231 bf 9 6 854 1231 bf 8 6 872 1231 bf 9 6 967 1231 bf 9 7 262 1237 bf 9 7 271 1237 bf 9 7 349 1237 bf 8 7 367 1237 bf 9 7 375 1237 bf 9 7 384 1237 bf 8 7
393 1237 bf 9 7 401 1237 bf 9 7 410 1237 bf 9 7 419 1237 bf 8 7 428 1237 bf 9 7 436 1237 bf 9 7 445 1237 bf 8 7 454 1237 bf 9 7 462 1237 bf 8 7 489 1237 bf 9 7 532 1237 bf 9 7 558 1237 bf 9 7 567 1237 bf 8 7 576 1237 bf 9 7 593 1237 bf 8 7 602 1237
bf 9 7 610 1237 bf 9 7 628 1237 bf 8 7 637 1237 bf 9 7 645 1237 bf 9 7 671 1237 bf 9 7 689 1237 bf 8 7 698 1237 bf 9 7 715 1237 bf 9 7 767 1237 bf 9 7 776 1237 bf 8 7 785 1237 bf 9 7 802 1237 bf 9 7 271 1244 bf 9 7 297 1244 bf 9 7 349 1244 bf 9 7
358 1244 bf 8 7 367 1244 bf 9 7 375 1244 bf 9 7 384 1244 bf 8 7 393 1244 bf 9 7 401 1244 bf 9 7 410 1244 bf 9 7 419 1244 bf 8 7 428 1244 bf 9 7 436 1244 bf 9 7 471 1244 bf 9 7 480 1244 bf 9 7 497 1244 bf 9 7 523 1244 bf 9 7 532 1244 bf 9 7 567 1244
bf 8 7 576 1244 bf 9 7 584 1244 bf 9 7 593 1244 bf 8 7 602 1244 bf 9 7 610 1244 bf 9 7 628 1244 bf 8 7 637 1244 bf 9 7 645 1244 bf 9 7 671 1244 bf 9 7 680 1244 bf 9 7 689 1244 bf 8 7 698 1244 bf 9 7 706 1244 bf 8 7 724 1244 bf 9 7 767 1244 bf 9 7
776 1244 bf 9 7 828 1244 bf 9 7 271 1251 bf 8 7 280 1251 bf 9 7 358 1251 bf 8 7 367 1251 bf 9 7 375 1251 bf 9 7 384 1251 bf 8 7 393 1251 bf 9 7 401 1251 bf 9 7 410 1251 bf 9 7 419 1251 bf 8 7 428 1251 bf 9 7 445 1251 bf 8 7 454 1251 bf 9 7 462 1251
bf 9 7 471 1251 bf 9 7 480 1251 bf 8 7 489 1251 bf 9 7 506 1251 bf 9 7 523 1251 bf 9 7 532 1251 bf 9 7 558 1251 bf 9 7 567 1251 bf 8 7 576 1251 bf 9 7 584 1251 bf 9 7 593 1251 bf 9 7 619 1251 bf 9 7 628 1251 bf 9 7 645 1251 bf 8 7 663 1251 bf 9 7
680 1251 bf 9 7 732 1251 bf 9 7 741 1251 bf 9 7 750 1251 bf 9 7 767 1251 bf 9 7 776 1251 bf 9 7 854 1251 bf 9 6 271 1258 bf 8 6 280 1258 bf 9 6 314 1258 bf 9 6 332 1258 bf 8 6 341 1258 bf 9 6 349 1258 bf 8 6 367 1258 bf 9 6 375 1258 bf 9 6 384 1258
bf 8 6 393 1258 bf 9 6 401 1258 bf 9 6 410 1258 bf 9 6 419 1258 bf 8 6 428 1258 bf 9 6 445 1258 bf 8 6 454 1258 bf 9 6 462 1258 bf 9 6 480 1258 bf 9 6 497 1258 bf 9 6 506 1258 bf 9 6 532 1258 bf 9 6 541 1258 bf 8 6 550 1258 bf 9 6 558 1258 bf 8 6
576 1258 bf 9 6 584 1258 bf 9 6 619 1258 bf 9 6 628 1258 bf 8 6 663 1258 bf 9 6 680 1258 bf 9 6 689 1258 bf 8 6 698 1258 bf 9 6 715 1258 bf 9 6 750 1258 bf 8 6 785 1258 bf 9 6 837 1258 bf 8 7 280 1264 bf 9 7 288 1264 bf 9 7 349 1264 bf 9 7 358 1264
bf 8 7 367 1264 bf 9 7 375 1264 bf 9 7 384 1264 bf 8 7 393 1264 bf 9 7 401 1264 bf 9 7 410 1264 bf 9 7 419 1264 bf 8 7 428 1264 bf 9 7 462 1264 bf 9 7 497 1264 bf 9 7 506 1264 bf 8 7 515 1264 bf 9 7 523 1264 bf 9 7 532 1264 bf 9 7 541 1264 bf 8 7
550 1264 bf 9 7 558 1264 bf 9 7 567 1264 bf 9 7 584 1264 bf 9 7 593 1264 bf 9 7 671 1264 bf 9 7 689 1264 bf 8 7 698 1264 bf 9 7 706 1264 bf 8 7 724 1264 bf 9 7 741 1264 bf 9 7 750 1264 bf 8 7 759 1264 bf 9 7 767 1264 bf 8 7 785 1264 bf 9 7 288 1271
bf 9 7 349 1271 bf 9 7 358 1271 bf 8 7 367 1271 bf 9 7 375 1271 bf 9 7 384 1271 bf 8 7 393 1271 bf 9 7 401 1271 bf 9 7 410 1271 bf 9 7 419 1271 bf 9 7 497 1271 bf 8 7 515 1271 bf 9 7 523 1271 bf 9 7 541 1271 bf 8 7 550 1271 bf 9 7 567 1271 bf 8 7
602 1271 bf 9 7 610 1271 bf 8 7 698 1271 bf 9 7 750 1271 bf 8 7 759 1271 bf 9 7 288 1278 bf 9 7 297 1278 bf 8 7 341 1278 bf 9 7 349 1278 bf 9 7 358 1278 bf 8 7 367 1278 bf 9 7 384 1278 bf 8 7 393 1278 bf 9 7 401 1278 bf 9 7 419 1278 bf 8 7 428 1278
bf 8 7 454 1278 bf 9 7 471 1278 bf 9 7 497 1278 bf 8 7 515 1278 bf 9 7 532 1278 bf 9 7 541 1278 bf 8 7 550 1278 bf 8 7 576 1278 bf 8 7 637 1278 bf 9 7 645 1278 bf 9 7 654 1278 bf 8 7 663 1278 bf 9 7 706 1278 bf 8 7 724 1278 bf 9 7 750 1278 bf 9 6
288 1285 bf 9 6 297 1285 bf 9 6 314 1285 bf 9 6 332 1285 bf 9 6 349 1285 bf 9 6 358 1285 bf 8 6 367 1285 bf 9 6 375 1285 bf 9 6 384 1285 bf 8 6 393 1285 bf 8 6 454 1285 bf 9 6 462 1285 bf 9 6 471 1285 bf 9 6 480 1285 bf 9 6 497 1285 bf 8 6 515 1285
bf 9 6 532 1285 bf 9 6 541 1285 bf 8 6 602 1285 bf 9 6 654 1285 bf 9 6 680 1285 bf 9 6 689 1285 bf 9 6 706 1285 bf 9 6 715 1285 bf 8 6 759 1285 bf 8 6 811 1285 bf 9 7 297 1291 bf 8 7 306 1291 bf 9 7 332 1291 bf 8 7 341 1291 bf 9 7 349 1291 bf 9 7
358 1291 bf 8 7 367 1291 bf 9 7 375 1291 bf 9 7 384 1291 bf 9 7 401 1291 bf 9 7 471 1291 bf 9 7 480 1291 bf 8 7 489 1291 bf 9 7 497 1291 bf 9 7 506 1291 bf 8 7 515 1291 bf 9 7 523 1291 bf 9 7 532 1291 bf 8 7 550 1291 bf 9 7 567 1291 bf 8 7 576 1291
bf 9 7 584 1291 bf 9 7 619 1291 bf 8 7 663 1291 bf 9 7 671 1291 bf 9 7 689 1291 bf 8 7 698 1291 bf 9 7 706 1291 bf 9 7 732 1291 bf 8 7 759 1291 bf 9 7 297 1298 bf 8 7 306 1298 bf 8 7 341 1298 bf 9 7 358 1298 bf 8 7 367 1298 bf 9 7 375 1298 bf 9 7
384 1298 bf 8 7 393 1298 bf 9 7 401 1298 bf 9 7 471 1298 bf 9 7 480 1298 bf 8 7 489 1298 bf 9 7 497 1298 bf 8 7 515 1298 bf 9 7 523 1298 bf 9 7 532 1298 bf 9 7 558 1298 bf 9 7 584 1298 bf 9 7 610 1298 bf 9 7 645 1298 bf 9 7 654 1298 bf 9 7 706 1298
bf 9 7 297 1305 bf 8 7 306 1305 bf 9 7 323 1305 bf 9 7 332 1305 bf 8 7 341 1305 bf 9 7 349 1305 bf 9 7 358 1305 bf 8 7 367 1305 bf 9 7 375 1305 bf 9 7 384 1305 bf 9 7 401 1305 bf 9 7 410 1305 bf 9 7 419 1305 bf 9 7 436 1305 bf 9 7 462 1305 bf 9 7
471 1305 bf 9 7 480 1305 bf 8 7 489 1305 bf 9 7 497 1305 bf 8 7 515 1305 bf 9 7 523 1305 bf 9 7 541 1305 bf 8 7 550 1305 bf 9 7 558 1305 bf 8 7 602 1305 bf 8 7 637 1305 bf 9 7 645 1305 bf 9 7 671 1305 bf 9 7 767 1305 bf 8 6 306 1312 bf 9 6 314 1312
bf 9 6 332 1312 bf 8 6 341 1312 bf 9 6 349 1312 bf 9 6 358 1312 bf 8 6 367 1312 bf 9 6 375 1312 bf 9 6 384 1312 bf 8 6 393 1312 bf 9 6 419 1312 bf 9 6 445 1312 bf 9 6 471 1312 bf 9 6 480 1312 bf 8 6 489 1312 bf 9 6 497 1312 bf 9 6 506 1312 bf 8 6
515 1312 bf 9 6 558 1312 bf 9 6 567 1312 bf 8 6 576 1312 bf 8 6 602 1312 bf 9 6 619 1312 bf 9 6 628 1312 bf 8 7 306 1318 bf 9 7 314 1318 bf 9 7 332 1318 bf 8 7 341 1318 bf 9 7 349 1318 bf 9 7 358 1318 bf 8 7 367 1318 bf 9 7 375 1318 bf 8 7 454 1318
bf 9 7 462 1318 bf 9 7 471 1318 bf 9 7 480 1318 bf 8 7 489 1318 bf 9 7 506 1318 bf 8 7 515 1318 bf 8 7 550 1318 bf 9 7 610 1318 bf 9 7 619 1318 bf 8 7 637 1318 bf 9 7 654 1318 bf 8 7 724 1318 bf 8 7 785 1318 bf 9 7 314 1325 bf 9 7 323 1325 bf 9 7
332 1325 bf 8 7 341 1325 bf 9 7 349 1325 bf 9 7 358 1325 bf 8 7 367 1325 bf 9 7 375 1325 bf 9 7 384 1325 bf 8 7 393 1325 bf 9 7 401 1325 bf 8 7 428 1325 bf 9 7 436 1325 bf 8 7 454 1325 bf 9 7 471 1325 bf 9 7 480 1325 bf 8 7 489 1325 bf 9 7 497 1325
bf 9 7 506 1325 bf 8 7 515 1325 bf 9 7 523 1325 bf 9 7 584 1325 bf 9 7 671 1325 bf 9 7 314 1332 bf 9 7 323 1332 bf 9 7 332 1332 bf 8 7 341 1332 bf 9 7 349 1332 bf 9 7 358 1332 bf 8 7 367 1332 bf 9 7 384 1332 bf 9 7 401 1332 bf 9 7 445 1332 bf 8 7
454 1332 bf 9 7 471 1332 bf 8 7 489 1332 bf 9 7 497 1332 bf 9 6 323 1339 bf 9 6 332 1339 bf 8 6 341 1339 bf 9 6 349 1339 bf 9 6 358 1339 bf 8 6 367 1339 bf 9 6 375 1339 bf 9 6 384 1339 bf 9 6 419 1339 bf 9 6 436 1339 bf 9 6 445 1339 bf 8 6 454 1339
bf 9 6 462 1339 bf 9 6 471 1339 bf 9 6 480 1339 bf 9 6 532 1339 bf 9 6 680 1339 bf 9 7 323 1345 bf 9 7 332 1345 bf 8 7 341 1345 bf 9 7 349 1345 bf 9 7 358 1345 bf 8 7 367 1345 bf 9 7 375 1345 bf 9 7 384 1345 bf 8 7 454 1345 bf 9 7 462 1345 bf 8 7
489 1345 bf 9 7 506 1345 bf 8 7 602 1345 bf 9 7 619 1345 bf 9 7 323 1352 bf 9 7 332 1352 bf 8 7 341 1352 bf 9 7 349 1352 bf 9 7 358 1352 bf 8 7 367 1352 bf 9 7 384 1352 bf 8 7 393 1352 bf 9 7 410 1352 bf 9 7 419 1352 bf 8 7 428 1352 bf 9 7 436 1352
bf 9 7 445 1352 bf 8 7 454 1352 bf 9 7 462 1352 bf 8 7 489 1352 bf 9 7 497 1352 bf 9 7 506 1352 bf 9 7 541 1352 bf 8 7 550 1352 bf 8 7 576 1352 bf 9 7 584 1352 bf 8 7 602 1352 bf 9 7 332 1359 bf 8 7 341 1359 bf 9 7 349 1359 bf 9 7 358 1359 bf 8 7
367 1359 bf 9 7 436 1359 bf 8 7 454 1359 bf 9 7 462 1359 bf 8 7 550 1359 bf 9 7 584 1359 bf 9 6 332 1366 bf 8 6 341 1366 bf 9 6 349 1366 bf 9 6 358 1366 bf 9 6 384 1366 bf 9 6 419 1366 bf 8 6 428 1366 bf 9 6 445 1366 bf 8 6 454 1366 bf 9 6 497 1366
bf 9 6 541 1366 bf 9 6 567 1366 bf 8 6 576 1366 bf 9 6 584 1366 bf 8 6 602 1366 bf 9 6 828 1366 bf 8 7 341 1372 bf 9 7 349 1372 bf 9 7 358 1372 bf 9 7 375 1372 bf 9 7 384 1372 bf 8 7 393 1372 bf 8 7 428 1372 bf 9 7 445 1372 bf 8 7 454 1372 bf 9 7
471 1372 bf 9 7 541 1372 bf 8 7 341 1379 bf 9 7 349 1379 bf 8 7 367 1379 bf 9 7 384 1379 bf 9 7 401 1379 bf 9 7 419 1379 bf 8 7 428 1379 bf 9 7 445 1379 bf 8 7 454 1379 bf 9 7 462 1379 bf 9 7 471 1379 bf 9 7 480 1379 bf 9 7 497 1379 bf 9 7 523 1379
bf 9 7 532 1379 bf 9 7 567 1379 bf 8 7 576 1379 bf 9 7 610 1379 bf 9 7 349 1386 bf 9 7 358 1386 bf 8 7 367 1386 bf 9 7 384 1386 bf 9 7 419 1386 bf 8 7 428 1386 bf 9 7 445 1386 bf 8 7 454 1386 bf 9 7 471 1386 bf 9 7 497 1386 bf 9 7 506 1386 bf 9 6
349 1393 bf 9 6 358 1393 bf 8 6 367 1393 bf 9 6 375 1393 bf 8 6 428 1393 bf 9 6 436 1393 bf 9 6 445 1393 bf 9 6 584 1393 bf 9 7 349 1399 bf 9 7 358 1399 bf 8 7 367 1399 bf 9 7 410 1399 bf 9 7 419 1399 bf 8 7 428 1399 bf 9 7 436 1399 bf 9 7 445 1399
bf 8 7 454 1399 bf 8 7 515 1399 bf 9 7 532 1399 bf 9 7 558 1399 bf 9 7 358 1406 bf 8 7 367 1406 bf 9 7 401 1406 bf 9 7 410 1406 bf 9 7 419 1406 bf 8 7 428 1406 bf 9 7 445 1406 bf 8 7 454 1406 bf 9 7 480 1406 bf 8 7 489 1406 bf 9 7 506 1406 bf 8 7
550 1406 bf 9 7 358 1413 bf 8 7 367 1413 bf 9 7 375 1413 bf 9 7 419 1413 bf 8 7 428 1413 bf 9 7 445 1413 bf 8 7 489 1413 bf 9 7 506 1413 bf 8 7 515 1413 bf 9 7 532 1413 bf 9 7 541 1413 bf 8 6 367 1420 bf 9 6 375 1420 bf 9 6 401 1420 bf 9 6 419 1420
bf 9 6 436 1420 bf 8 7 367 1426 bf 9 7 375 1426 bf 8 7 393 1426 bf 9 7 401 1426 bf 9 7 419 1426 bf 8 7 428 1426 bf 9 7 436 1426 bf 8 7 489 1426 bf 9 7 523 1426 bf 9 7 802 1426 bf 9 7 375 1433 bf 9 7 401 1433 bf 9 7 410 1433 bf 9 7 462 1433 bf 8 7
489 1433 bf 9 7 497 1433 bf 9 7 506 1433 bf 8 7 515 1433 bf 9 7 532 1433 bf 9 7 375 1440 bf 9 7 384 1440 bf 8 7 393 1440 bf 9 7 401 1440 bf 9 7 410 1440 bf 8 7 428 1440 bf 9 7 480 1440 bf 8 7 489 1440 bf 9 6 375 1447 bf 9 6 384 1447 bf 9 6 401 1447
bf 9 6 410 1447 bf 9 6 419 1447 bf 9 6 436 1447 bf 9 7 384 1453 bf 8 7 393 1453 bf 9 7 445 1453 bf 9 7 462 1453 bf 9 7 480 1453 bf 9 7 384 1460 bf 8 7 393 1460 bf 9 7 401 1460 bf 8 7 428 1460 bf 9 7 462 1460 bf 9 7 497 1460 bf 8 7 393 1467 bf 9 7
410 1467 bf 9 7 419 1467 bf 8 6 393 1474 bf 9 6 401 1474 bf 9 6 410 1474 bf 8 7 393 1480 bf 9 7 401 1480 bf 9 7 410 1480 bf 9 7 462 1480 bf 9 7 819 1480 bf 9 7 401 1487 bf 9 7 410 1487 bf 9 7 419 1487 bf 9 7 471 1487 bf 9 7 480 1487 bf 9 7 410 1494
bf 9 7 462 1494 bf 8 7 602 1494 bf 9 6 410 1501 bf 8 6 489 1501 bf 9 7 410 1507 bf 9 7 419 1507 bf 9 7 471 1507 bf 9 7 480 1507 bf 9 7 419 1514 bf 9 7 436 1514 bf 9 7 462 1514 bf 9 7 480 1514 bf 9 7 419 1521 bf 8 7 428 1521 bf 9 7 436 1521 bf 9 7
462 1521 bf 9 6 419 1528 bf 8 6 428 1528 bf 9 6 462 1528 bf 8 7 428 1534 bf 9 7 436 1534 bf 8 7 454 1534 bf 9 7 471 1534 bf 8 7 428 1541 bf 9 7 436 1541 bf 9 7 471 1541 bf 9 7 436 1548 bf 8 7 454 1548 bf 9 7 471 1548 bf 9 6 436 1555 bf 9 6 445 1555
bf 9 7 445 1561 bf 8 7 454 1561 bf 9 7 462 1561 bf 9 7 445 1568 bf 8 7 454 1568 bf 8 7 454 1575 bf 9 7 462 1575 bf 8 6 454 1582 bf 8 7 454 1588 bf 9 7 462 1588 bf 8 7 454 1595 bf 9 7 462 1595 bf 9 7 471 1595 bf 9 7 462 1602 bf 9 7 471 1602 bf 9 6
471 1609 bf 9 7 471 1622 bf 9 7 480 1622 bf 9 7 480 1629 bf 9 7 506 1629 bf 8 6 489 1636 bf 8 7 489 1642 bf 8 7 489 1649 bf 1 1 1 c black 132 981 m 870 X s
gsave 1088 844 23 896 C 569.206 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 1001 m -20 Y s 149 991 m -10 Y s 166 991 m -10 Y s 184 991 m -10 Y s 201 991 m -10 Y s 219 1001 m -20 Y s 236 991 m
-10 Y s 253 991 m -10 Y s 271 991 m -10 Y s 288 991 m -10 Y s 306 1001 m -20 Y s 323 991 m -10 Y s 341 991 m -10 Y s 358 991 m -10 Y s 375 991 m -10 Y s 393 1001 m -20 Y s 410 991 m -10 Y s 428 991 m -10 Y s 445 991 m -10 Y s 462 991 m -10 Y s 480
1001 m -20 Y s 497 991 m -10 Y s 515 991 m -10 Y s 532 991 m -10 Y s 550 991 m -10 Y s 567 1001 m -20 Y s 584 991 m -10 Y s 602 991 m -10 Y s 619 991 m -10 Y s 637 991 m -10 Y s 654 1001 m -20 Y s 671 991 m -10 Y s 689 991 m -10 Y s 706 991 m -10 Y
s 724 991 m -10 Y s 741 1001 m -20 Y s 759 991 m -10 Y s 776 991 m -10 Y s 793 991 m -10 Y s 811 991 m -10 Y s 828 1001 m -20 Y s 846 991 m -10 Y s 863 991 m -10 Y s 880 991 m -10 Y s 898 991 m -10 Y s 915 1001 m -20 Y s 933 991 m -10 Y s 950 991 m
-10 Y s 967 991 m -10 Y s 985 991 m -10 Y s 1002 1001 m -20 Y s
gsave 1088 844 23 896 C 120.672 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 182.146 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 268.665 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 355.185 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 441.704 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 23 896 C 530.5 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 23 896 C 617.019 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 23 896 C 703.539 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 23 896 C 790.058 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 23 896 C 876.577 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 23 896 C 956.266 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 1656 m 870 X s 132 1636 m 20 Y s 149 1646 m 10 Y s 166 1646 m 10 Y s 184 1646 m 10 Y s 201 1646 m 10 Y s 219 1636 m 20 Y s 236 1646 m 10
Y s 253 1646 m 10 Y s 271 1646 m 10 Y s 288 1646 m 10 Y s 306 1636 m 20 Y s 323 1646 m 10 Y s 341 1646 m 10 Y s 358 1646 m 10 Y s 375 1646 m 10 Y s 393 1636 m 20 Y s 410 1646 m 10 Y s 428 1646 m 10 Y s 445 1646 m 10 Y s 462 1646 m 10 Y s 480 1636 m
20 Y s 497 1646 m 10 Y s 515 1646 m 10 Y s 532 1646 m 10 Y s 550 1646 m 10 Y s 567 1636 m 20 Y s 584 1646 m 10 Y s 602 1646 m 10 Y s 619 1646 m 10 Y s 637 1646 m 10 Y s 654 1636 m 20 Y s 671 1646 m 10 Y s 689 1646 m 10 Y s 706 1646 m 10 Y s 724 1646
m 10 Y s 741 1636 m 20 Y s 759 1646 m 10 Y s 776 1646 m 10 Y s 793 1646 m 10 Y s 811 1646 m 10 Y s 828 1636 m 20 Y s 846 1646 m 10 Y s 863 1646 m 10 Y s 880 1646 m 10 Y s 898 1646 m 10 Y s 915 1636 m 20 Y s 933 1646 m 10 Y s 950 1646 m 10 Y s 967
1646 m 10 Y s 985 1646 m 10 Y s 1002 1636 m 20 Y s 132 981 m 675 Y s
gsave 1088 844 23 896 C 54.6438 1400.25 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 158 981 m -26 X s 145 997 m -13 X s 145 1013 m -13 X s 145 1029 m -13 X s 145 1045 m -13 X s 158 1061 m -26 X s 145 1077 m -13 X
s 145 1093 m -13 X s 145 1109 m -13 X s 145 1125 m -13 X s 158 1142 m -26 X s 145 1158 m -13 X s 145 1174 m -13 X s 145 1190 m -13 X s 145 1206 m -13 X s 158 1222 m -26 X s 145 1238 m -13 X s 145 1254 m -13 X s 145 1270 m -13 X s 145 1286 m -13 X s
158 1302 m -26 X s 145 1318 m -13 X s 145 1334 m -13 X s 145 1350 m -13 X s 145 1366 m -13 X s 158 1383 m -26 X s 145 1399 m -13 X s 145 1415 m -13 X s 145 1431 m -13 X s 145 1447 m -13 X s 158 1463 m -26 X s 145 1479 m -13 X s 145 1495 m -13 X s
145 1511 m -13 X s 145 1527 m -13 X s 158 1543 m -26 X s 145 1559 m -13 X s 145 1575 m -13 X s 145 1591 m -13 X s 145 1608 m -13 X s 158 1624 m -26 X s 158 1624 m -26 X s 145 1640 m -13 X s 145 1656 m -13 X s
gsave 1088 844 23 896 C 107.011 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 72.8584 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 844 23 896 C 54.6438 1129.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 54.6438 1208.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 844 23 896 C 54.6438 1288.68 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 54.6438 1370.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 844 23 896 C 54.6438 1450.34 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 54.6438 1530.03 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 844 23 896 C 54.6438 1611.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 1002 981 m 675 Y s 976 981 m 26 X s 989 997 m 13 X s 989 1013 m 13 X s 989 1029 m 13 X s 989 1045 m 13 X s 976 1061 m 26 X s 989 1077 m 13 X
s 989 1093 m 13 X s 989 1109 m 13 X s 989 1125 m 13 X s 976 1142 m 26 X s 989 1158 m 13 X s 989 1174 m 13 X s 989 1190 m 13 X s 989 1206 m 13 X s 976 1222 m 26 X s 989 1238 m 13 X s 989 1254 m 13 X s 989 1270 m 13 X s 989 1286 m 13 X s 976 1302 m 26
X s 989 1318 m 13 X s 989 1334 m 13 X s 989 1350 m 13 X s 989 1366 m 13 X s 976 1383 m 26 X s 989 1399 m 13 X s 989 1415 m 13 X s 989 1431 m 13 X s 989 1447 m 13 X s 976 1463 m 26 X s 989 1479 m 13 X s 989 1495 m 13 X s 989 1511 m 13 X s 989 1527 m
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gsave 1088 844 1157 896 C 1402.52 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
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gsave 1088 844 1157 896 C 2010.44 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
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gsave 1088 844 1157 896 C 2194.86 1124.75 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
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1 c 9 7 419 628 bf 9 7 436 669 bf 9 7 445 682 bf 1 1 1 c black 132 102 m 870 X s
gsave 1088 843 23 18 C 569.206 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 122 m -20 Y s 149 112 m -10 Y s 166 112 m -10 Y s 184 112 m -10 Y s 201 112 m -10 Y s 219 122 m -20 Y s 236 112 m -10 Y
s 253 112 m -10 Y s 271 112 m -10 Y s 288 112 m -10 Y s 306 122 m -20 Y s 323 112 m -10 Y s 341 112 m -10 Y s 358 112 m -10 Y s 375 112 m -10 Y s 393 122 m -20 Y s 410 112 m -10 Y s 428 112 m -10 Y s 445 112 m -10 Y s 462 112 m -10 Y s 480 122 m -20
Y s 497 112 m -10 Y s 515 112 m -10 Y s 532 112 m -10 Y s 550 112 m -10 Y s 567 122 m -20 Y s 584 112 m -10 Y s 602 112 m -10 Y s 619 112 m -10 Y s 637 112 m -10 Y s 654 122 m -20 Y s 671 112 m -10 Y s 689 112 m -10 Y s 706 112 m -10 Y s 724 112 m
-10 Y s 741 122 m -20 Y s 759 112 m -10 Y s 776 112 m -10 Y s 793 112 m -10 Y s 811 112 m -10 Y s 828 122 m -20 Y s 846 112 m -10 Y s 863 112 m -10 Y s 880 112 m -10 Y s 898 112 m -10 Y s 915 122 m -20 Y s 933 112 m -10 Y s 950 112 m -10 Y s 967 112
m -10 Y s 985 112 m -10 Y s 1002 122 m -20 Y s
gsave 1088 843 23 18 C 120.672 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 23 18 C 182.146 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 23 18 C 268.665 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 23 18 C 355.185 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 23 18 C 441.704 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 843 23 18 C 530.5 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 843 23 18 C 617.019 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 843 23 18 C 703.539 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 843 23 18 C 790.058 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 843 23 18 C 876.577 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 843 23 18 C 956.266 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 777 m 870 X s 132 757 m 20 Y s 149 767 m 10 Y s 166 767 m 10 Y s 184 767 m 10 Y s 201 767 m 10 Y s 219 757 m 20 Y s 236 767 m 10 Y s 253
767 m 10 Y s 271 767 m 10 Y s 288 767 m 10 Y s 306 757 m 20 Y s 323 767 m 10 Y s 341 767 m 10 Y s 358 767 m 10 Y s 375 767 m 10 Y s 393 757 m 20 Y s 410 767 m 10 Y s 428 767 m 10 Y s 445 767 m 10 Y s 462 767 m 10 Y s 480 757 m 20 Y s 497 767 m 10 Y
s 515 767 m 10 Y s 532 767 m 10 Y s 550 767 m 10 Y s 567 757 m 20 Y s 584 767 m 10 Y s 602 767 m 10 Y s 619 767 m 10 Y s 637 767 m 10 Y s 654 757 m 20 Y s 671 767 m 10 Y s 689 767 m 10 Y s 706 767 m 10 Y s 724 767 m 10 Y s 741 757 m 20 Y s 759 767 m
10 Y s 776 767 m 10 Y s 793 767 m 10 Y s 811 767 m 10 Y s 828 757 m 20 Y s 846 767 m 10 Y s 863 767 m 10 Y s 880 767 m 10 Y s 898 767 m 10 Y s 915 757 m 20 Y s 933 767 m 10 Y s 950 767 m 10 Y s 967 767 m 10 Y s 985 767 m 10 Y s 1002 757 m 20 Y s 132
102 m 675 Y s
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214 m -13 X s 145 231 m -13 X s 145 247 m -13 X s 158 263 m -26 X s 145 279 m -13 X s 145 295 m -13 X s 145 311 m -13 X s 145 327 m -13 X s 158 343 m -26 X s 145 359 m -13 X s 145 375 m -13 X s 145 391 m -13 X s 145 407 m -13 X s 158 423 m -26 X s
145 439 m -13 X s 145 455 m -13 X s 145 472 m -13 X s 145 488 m -13 X s 158 504 m -26 X s 145 520 m -13 X s 145 536 m -13 X s 145 552 m -13 X s 145 568 m -13 X s 158 584 m -26 X s 145 600 m -13 X s 145 616 m -13 X s 145 632 m -13 X s 145 648 m -13 X
s 158 664 m -26 X s 145 680 m -13 X s 145 697 m -13 X s 145 713 m -13 X s 145 729 m -13 X s 158 745 m -26 X s 158 745 m -26 X s 145 761 m -13 X s 145 777 m -13 X s
gsave 1088 843 23 18 C 107.011 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 23 18 C 72.8584 170.762 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 843 23 18 C 54.6438 250.451 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 23 18 C 54.6438 330.139 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 843 23 18 C 54.6438 409.828 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 23 18 C 54.6438 491.794 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 843 23 18 C 54.6438 571.483 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 23 18 C 54.6438 651.172 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 843 23 18 C 54.6438 733.137 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 1002 102 m 675 Y s 976 102 m 26 X s 989 118 m 13 X s 989 134 m 13 X s 989 150 m 13 X s 989 166 m 13 X s 976 182 m 26 X s 989 198 m 13 X s 989
214 m 13 X s 989 231 m 13 X s 989 247 m 13 X s 976 263 m 26 X s 989 279 m 13 X s 989 295 m 13 X s 989 311 m 13 X s 989 327 m 13 X s 976 343 m 26 X s 989 359 m 13 X s 989 375 m 13 X s 989 391 m 13 X s 989 407 m 13 X s 976 423 m 26 X s 989 439 m 13 X
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203 bf 0 0.546666 1 c 49 34 1008 237 bf 0 0.733333 1 c 49 33 1008 271 bf 0 1 0.986667 c 49 34 1008 304 bf 0 1 0.8 c 49 34 1008 338 bf 0 1 0.52 c 49 34 1008 372 bf 0 1 0.333333 c 49 33 1008 406 bf 0 1 0.0533333 c 49 34 1008 439 bf 0.133333 1 0 c 49
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34 1008 743 bf black 1057 102 m 675 Y s 1031 102 m 26 X s 1031 172 m 26 X s 1031 243 m 26 X s 1031 313 m 26 X s 1031 383 m 26 X s 1031 453 m 26 X s 1031 524 m 26 X s 1031 594 m 26 X s 1031 664 m 26 X s 1031 735 m 26 X s 1031 735 m 26 X s
gsave 1088 843 23 18 C 1061 88.7961 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 23 18 C 1061 161.654 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5) show NC gr
gsave 1088 843 23 18 C 1061 229.959 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 843 23 18 C 1061 300.541 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (15) show NC gr
gsave 1088 843 23 18 C 1061 371.122 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (20) show NC gr
gsave 1088 843 23 18 C 1061 441.704 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (25) show NC gr
gsave 1088 843 23 18 C 1061 512.285 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (30) show NC gr
gsave 1088 843 23 18 C 1061 580.59 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (35) show NC gr
gsave 1088 843 23 18 C 1061 651.172 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (40) show NC gr
gsave 1088 843 23 18 C 1061 721.753 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (45) show NC gr 1 1 1 c 445 42 34 815 bf black 34 815 m 445 X s 479 815 m 42 Y s 479 857 m -445 X s 34 857 m -42 Y s 1 1 1 c black
gsave 1088 843 23 18 C 68.3047 824.21 t 0 r /Helvetica-Bold findfont 34.204 sf 0 0 m (Protons and deuterons) show NC gr 1 1 1 c 1088 843 1157 18 bf black 1 1 1 c 871 675 1265 102 bf black 871 675 1265 102 bl 1 1 1 c 871 675 1265 102 bf black 871
675 1265 102 bl 1 1 1 c 0 0.0800001 1 c 9 7 1265 102 bf 9 6 1265 109 bf 0.386667 0 1 c 9 6 1274 109 bf 8 6 1292 109 bf 9 6 1788 109 bf 8 6 2006 109 bf 0.2 0 1 c 9 7 1265 115 bf 0 0.546666 1 c 9 7 1274 115 bf 0.386667 0 1 c 9 7 2110 115 bf 0 1
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1901 169 bf 9 7 1918 169 bf 9 7 1962 169 bf 9 7 1988 169 bf 9 7 1997 169 bf 8 7 2006 169 bf 0.2 0 1 c 9 7 2014 169 bf 0.386667 0 1 c 8 7 2032 169 bf 9 7 2040 169 bf 9 7 2049 169 bf 9 7 2075 169 bf 8 7 2093 169 bf 9 7 2101 169 bf 9 7 2110 169 bf 8 7
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9 7 1953 176 bf 9 7 1962 176 bf 8 7 1971 176 bf 0.2 0 1 c 9 7 1988 176 bf 0.386667 0 1 c 8 7 2006 176 bf 0.2 0 1 c 9 7 2014 176 bf 0.386667 0 1 c 9 7 2023 176 bf 8 7 2032 176 bf 0.2 0 1 c 9 7 2040 176 bf 9 7 2049 176 bf 0.386667 0 1 c 9 7 2058 176
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bf 0 0.266667 1 c 8 7 1318 210 bf 0.386667 0 1 c 9 7 1326 210 bf 9 7 1474 210 bf 9 7 1692 210 bf 8 7 1701 210 bf 9 7 1718 210 bf 8 7 1736 210 bf 9 7 1744 210 bf 9 7 1753 210 bf 0.2 0 1 c 8 7 1762 210 bf 0.386667 0 1 c 9 7 1770 210 bf 9 7 1779 210 bf
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9 6 1927 217 bf 9 6 1936 217 bf 8 6 1945 217 bf 0.386667 0 1 c 9 6 1953 217 bf 0.2 0 1 c 9 6 1962 217 bf 8 6 1971 217 bf 9 6 1979 217 bf 9 6 1988 217 bf 0 0.0800001 1 c 9 6 1997 217 bf 0.386667 0 1 c 8 6 2006 217 bf 9 6 2014 217 bf 0.2 0 1 c 9 6
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0.386667 0 1 c 8 7 1588 358 bf 0.2 0 1 c 9 7 1596 358 bf 0.386667 0 1 c 9 7 1622 358 bf 9 7 1666 358 bf 9 7 1692 358 bf 8 7 1701 358 bf 9 7 1709 358 bf 9 7 1727 358 bf 0.2 0 1 c 8 7 1736 358 bf 0.386667 0 1 c 9 7 1744 358 bf 8 7 1762 358 bf 9 7 1770
358 bf 0.2 0 1 c 9 7 1779 358 bf 0.386667 0 1 c 9 7 1805 358 bf 8 7 1823 358 bf 9 7 1831 358 bf 9 7 1849 358 bf 9 7 1901 358 bf 8 7 1910 358 bf 9 7 1918 358 bf 9 7 1936 358 bf 0 1 0.333333 c 8 7 1405 365 bf 0.386667 0 1 c 9 7 1431 365 bf 9 7 1483
365 bf 0.2 0 1 c 9 7 1492 365 bf 0 0.0800001 1 c 8 7 1501 365 bf 9 7 1509 365 bf 0.2 0 1 c 9 7 1518 365 bf 0 0.0800001 1 c 8 7 1527 365 bf 0.2 0 1 c 9 7 1535 365 bf 0 0.0800001 1 c 9 7 1544 365 bf 0.2 0 1 c 8 7 1553 365 bf 9 7 1561 365 bf 0.386667 0
1 c 9 7 1570 365 bf 9 7 1605 365 bf 8 7 1614 365 bf 9 7 1631 365 bf 9 7 1657 365 bf 9 7 1666 365 bf 8 7 1701 365 bf 0.2 0 1 c 9 7 1709 365 bf 0.386667 0 1 c 9 7 1718 365 bf 9 7 1727 365 bf 8 7 1736 365 bf 9 7 1744 365 bf 8 7 1762 365 bf 9 7 1770 365
bf 9 7 1779 365 bf 9 7 1805 365 bf 9 7 1814 365 bf 8 7 1823 365 bf 9 7 1831 365 bf 9 7 1840 365 bf 0.2 0 1 c 8 7 1858 365 bf 0.386667 0 1 c 9 7 1901 365 bf 8 7 1910 365 bf 9 7 1962 365 bf 0 1 0.333333 c 8 7 1405 372 bf 0 1 0.986667 c 9 7 1413 372 bf
0 0.0800001 1 c 9 7 1492 372 bf 8 7 1501 372 bf 0.2 0 1 c 9 7 1509 372 bf 9 7 1518 372 bf 0 0.0800001 1 c 8 7 1527 372 bf 9 7 1535 372 bf 9 7 1544 372 bf 8 7 1553 372 bf 0.386667 0 1 c 9 7 1561 372 bf 9 7 1579 372 bf 8 7 1588 372 bf 9 7 1596 372 bf
9 7 1605 372 bf 8 7 1614 372 bf 9 7 1622 372 bf 9 7 1640 372 bf 9 7 1657 372 bf 9 7 1666 372 bf 9 7 1692 372 bf 0.2 0 1 c 8 7 1701 372 bf 0.386667 0 1 c 9 7 1709 372 bf 9 7 1718 372 bf 9 7 1727 372 bf 0.2 0 1 c 9 7 1753 372 bf 0.386667 0 1 c 8 7
1762 372 bf 9 7 1779 372 bf 8 7 1797 372 bf 9 7 1814 372 bf 9 7 1866 372 bf 9 7 1875 372 bf 8 7 1884 372 bf 9 7 1901 372 bf 8 7 1910 372 bf 9 7 1988 372 bf 8 6 1405 379 bf 1 0.653333 0 c 9 6 1413 379 bf 0.386667 0 1 c 9 6 1448 379 bf 8 6 1466 379 bf
9 6 1474 379 bf 0.2 0 1 c 9 6 1483 379 bf 0 0.0800001 1 c 8 6 1501 379 bf 9 6 1509 379 bf 0 0.266667 1 c 9 6 1518 379 bf 0 0.0800001 1 c 8 6 1527 379 bf 9 6 1535 379 bf 0.386667 0 1 c 9 6 1544 379 bf 0.2 0 1 c 8 6 1553 379 bf 0.386667 0 1 c 9 6 1561
379 bf 9 6 1579 379 bf 8 6 1588 379 bf 9 6 1596 379 bf 8 6 1614 379 bf 9 6 1631 379 bf 9 6 1640 379 bf 9 6 1666 379 bf 8 6 1675 379 bf 0.2 0 1 c 9 6 1683 379 bf 0.386667 0 1 c 9 6 1692 379 bf 0.2 0 1 c 9 6 1709 379 bf 0.386667 0 1 c 9 6 1718 379 bf
9 6 1753 379 bf 8 6 1762 379 bf 8 6 1797 379 bf 9 6 1814 379 bf 8 6 1823 379 bf 9 6 1831 379 bf 9 6 1849 379 bf 8 6 1884 379 bf 9 6 1918 379 bf 8 6 1971 379 bf 0.133333 1 0 c 9 7 1413 385 bf 0 0.266667 1 c 9 7 1422 385 bf 0.2 0 1 c 9 7 1483 385 bf
0.386667 0 1 c 9 7 1492 385 bf 0 0.0800001 1 c 8 7 1501 385 bf 0 0.266667 1 c 9 7 1509 385 bf 0 0.0800001 1 c 9 7 1518 385 bf 0.2 0 1 c 8 7 1527 385 bf 9 7 1535 385 bf 9 7 1544 385 bf 0.386667 0 1 c 8 7 1553 385 bf 0.2 0 1 c 9 7 1561 385 bf 0.386667
0 1 c 9 7 1596 385 bf 9 7 1631 385 bf 9 7 1640 385 bf 8 7 1649 385 bf 0.2 0 1 c 9 7 1657 385 bf 0.386667 0 1 c 9 7 1666 385 bf 8 7 1675 385 bf 9 7 1683 385 bf 9 7 1692 385 bf 8 7 1701 385 bf 9 7 1718 385 bf 9 7 1727 385 bf 9 7 1805 385 bf 8 7 1823
385 bf 9 7 1831 385 bf 9 7 1840 385 bf 8 7 1858 385 bf 9 7 1875 385 bf 8 7 1884 385 bf 9 7 1892 385 bf 9 7 1901 385 bf 9 7 1918 385 bf 0.413333 1 0 c 9 7 1422 392 bf 0.2 0 1 c 9 7 1483 392 bf 0.386667 0 1 c 9 7 1492 392 bf 0.2 0 1 c 8 7 1501 392 bf
0 0.266667 1 c 9 7 1509 392 bf 0 0.0800001 1 c 9 7 1518 392 bf 8 7 1527 392 bf 0.2 0 1 c 9 7 1535 392 bf 0.386667 0 1 c 9 7 1544 392 bf 0.2 0 1 c 8 7 1553 392 bf 0.386667 0 1 c 9 7 1631 392 bf 8 7 1649 392 bf 9 7 1657 392 bf 8 7 1675 392 bf 9 7 1683
392 bf 8 7 1701 392 bf 8 7 1736 392 bf 9 7 1744 392 bf 9 7 1831 392 bf 8 7 1884 392 bf 9 7 1892 392 bf 0.413333 1 0 c 9 7 1422 399 bf 0.2 0 1 c 9 7 1431 399 bf 0.386667 0 1 c 9 7 1474 399 bf 9 7 1483 399 bf 9 7 1492 399 bf 8 7 1501 399 bf 0.2 0 1 c
9 7 1518 399 bf 8 7 1527 399 bf 0.386667 0 1 c 9 7 1535 399 bf 0.2 0 1 c 8 7 1553 399 bf 0.386667 0 1 c 9 7 1561 399 bf 8 7 1588 399 bf 9 7 1605 399 bf 9 7 1631 399 bf 8 7 1649 399 bf 9 7 1666 399 bf 8 7 1675 399 bf 9 7 1683 399 bf 9 7 1709 399 bf 9
7 1770 399 bf 0.2 0 1 c 9 7 1779 399 bf 0.386667 0 1 c 9 7 1788 399 bf 8 7 1797 399 bf 9 7 1840 399 bf 8 7 1858 399 bf 8 7 1884 399 bf 0 0.733333 1 c 9 6 1422 406 bf 0 1 0.52 c 9 6 1431 406 bf 0.386667 0 1 c 9 6 1448 406 bf 8 6 1466 406 bf 0
0.0800001 1 c 9 6 1483 406 bf 9 6 1492 406 bf 8 6 1501 406 bf 9 6 1509 406 bf 0.2 0 1 c 9 6 1518 406 bf 0.386667 0 1 c 8 6 1527 406 bf 8 6 1588 406 bf 9 6 1596 406 bf 9 6 1605 406 bf 8 6 1614 406 bf 0.2 0 1 c 9 6 1631 406 bf 0.386667 0 1 c 8 6 1649
406 bf 9 6 1666 406 bf 8 6 1675 406 bf 8 6 1736 406 bf 9 6 1788 406 bf 9 6 1814 406 bf 8 6 1823 406 bf 9 6 1840 406 bf 9 6 1849 406 bf 9 6 1892 406 bf 8 6 1945 406 bf 0.88 1 0 c 9 7 1431 412 bf 0.386667 0 1 c 8 7 1440 412 bf 8 7 1466 412 bf 0
0.0800001 1 c 9 7 1474 412 bf 0.386667 0 1 c 9 7 1483 412 bf 0 0.0800001 1 c 9 7 1492 412 bf 0.2 0 1 c 8 7 1501 412 bf 0.386667 0 1 c 9 7 1509 412 bf 9 7 1518 412 bf 0.2 0 1 c 9 7 1535 412 bf 0.386667 0 1 c 9 7 1605 412 bf 8 7 1614 412 bf 9 7 1622
412 bf 9 7 1631 412 bf 9 7 1640 412 bf 8 7 1649 412 bf 9 7 1657 412 bf 9 7 1666 412 bf 9 7 1683 412 bf 8 7 1701 412 bf 9 7 1709 412 bf 9 7 1718 412 bf 9 7 1753 412 bf 8 7 1797 412 bf 9 7 1805 412 bf 8 7 1823 412 bf 9 7 1831 412 bf 9 7 1840 412 bf 9
7 1866 412 bf 9 7 1892 412 bf 0.413333 1 0 c 9 7 1431 419 bf 0 1 0.986667 c 8 7 1440 419 bf 0.386667 0 1 c 9 7 1474 419 bf 0.2 0 1 c 9 7 1492 419 bf 0 0.0800001 1 c 8 7 1501 419 bf 0.386667 0 1 c 9 7 1509 419 bf 0.2 0 1 c 9 7 1518 419 bf 0.386667 0
1 c 8 7 1527 419 bf 9 7 1535 419 bf 9 7 1605 419 bf 8 7 1614 419 bf 9 7 1622 419 bf 9 7 1631 419 bf 8 7 1649 419 bf 9 7 1657 419 bf 9 7 1666 419 bf 9 7 1692 419 bf 9 7 1718 419 bf 9 7 1744 419 bf 9 7 1779 419 bf 9 7 1788 419 bf 9 7 1840 419 bf 0.2 0
1 c 9 7 1431 426 bf 1 0.466667 0 c 8 7 1440 426 bf 0.386667 0 1 c 9 7 1457 426 bf 0.2 0 1 c 8 7 1466 426 bf 0.386667 0 1 c 9 7 1474 426 bf 0.2 0 1 c 9 7 1483 426 bf 0.386667 0 1 c 9 7 1492 426 bf 0 0.0800001 1 c 8 7 1501 426 bf 0.2 0 1 c 9 7 1509
426 bf 9 7 1518 426 bf 0.386667 0 1 c 9 7 1535 426 bf 9 7 1544 426 bf 8 7 1553 426 bf 9 7 1570 426 bf 9 7 1596 426 bf 9 7 1605 426 bf 8 7 1614 426 bf 9 7 1622 426 bf 9 7 1631 426 bf 8 7 1649 426 bf 9 7 1657 426 bf 8 7 1675 426 bf 9 7 1683 426 bf 9 7
1692 426 bf 8 7 1736 426 bf 9 7 1770 426 bf 9 7 1779 426 bf 9 7 1805 426 bf 9 7 1901 426 bf 0 1 0.0533333 c 8 6 1440 433 bf 0 0.0800001 1 c 9 6 1448 433 bf 0.386667 0 1 c 8 6 1466 433 bf 9 6 1474 433 bf 0 0.0800001 1 c 9 6 1483 433 bf 0.2 0 1 c 9 6
1492 433 bf 0.386667 0 1 c 8 6 1501 433 bf 9 6 1509 433 bf 9 6 1518 433 bf 8 6 1527 433 bf 8 6 1553 433 bf 9 6 1579 433 bf 9 6 1605 433 bf 8 6 1614 433 bf 9 6 1622 433 bf 9 6 1631 433 bf 9 6 1640 433 bf 8 6 1649 433 bf 9 6 1692 433 bf 8 6 1701 433
bf 9 6 1709 433 bf 8 6 1736 433 bf 9 6 1753 433 bf 8 6 1762 433 bf 0.2 0 1 c 8 7 1440 439 bf 0.88 1 0 c 9 7 1448 439 bf 0.386667 0 1 c 8 7 1466 439 bf 0.2 0 1 c 9 7 1474 439 bf 0.386667 0 1 c 9 7 1483 439 bf 0.2 0 1 c 9 7 1492 439 bf 0.386667 0 1 c
8 7 1501 439 bf 0.2 0 1 c 9 7 1509 439 bf 0.386667 0 1 c 8 7 1588 439 bf 9 7 1596 439 bf 9 7 1605 439 bf 8 7 1614 439 bf 0.2 0 1 c 9 7 1622 439 bf 0.386667 0 1 c 9 7 1640 439 bf 8 7 1649 439 bf 9 7 1683 439 bf 9 7 1744 439 bf 9 7 1753 439 bf 9 7
1770 439 bf 9 7 1788 439 bf 8 7 1858 439 bf 9 7 1918 439 bf 0.6 1 0 c 9 7 1448 446 bf 0.386667 0 1 c 9 7 1457 446 bf 8 7 1466 446 bf 0 0.0800001 1 c 9 7 1474 446 bf 9 7 1483 446 bf 0.386667 0 1 c 9 7 1492 446 bf 8 7 1501 446 bf 9 7 1509 446 bf 9 7
1518 446 bf 8 7 1527 446 bf 9 7 1535 446 bf 9 7 1561 446 bf 9 7 1570 446 bf 8 7 1588 446 bf 9 7 1605 446 bf 0.2 0 1 c 8 7 1614 446 bf 0.386667 0 1 c 9 7 1622 446 bf 9 7 1631 446 bf 9 7 1640 446 bf 8 7 1649 446 bf 9 7 1657 446 bf 9 7 1718 446 bf 9 7
1805 446 bf 0 1 0.8 c 9 7 1448 453 bf 0 1 0.52 c 9 7 1457 453 bf 0.386667 0 1 c 8 7 1466 453 bf 0.2 0 1 c 9 7 1474 453 bf 0.386667 0 1 c 9 7 1483 453 bf 9 7 1492 453 bf 0.2 0 1 c 8 7 1501 453 bf 0.386667 0 1 c 9 7 1518 453 bf 9 7 1535 453 bf 9 7
1579 453 bf 8 7 1588 453 bf 9 7 1605 453 bf 9 7 1622 453 bf 9 7 1631 453 bf 1 0 0 c 9 6 1457 460 bf 0.386667 0 1 c 8 6 1466 460 bf 0.2 0 1 c 9 6 1474 460 bf 9 6 1483 460 bf 0 0.0800001 1 c 9 6 1492 460 bf 0.2 0 1 c 8 6 1501 460 bf 0.386667 0 1 c 9 6
1509 460 bf 9 6 1518 460 bf 8 6 1553 460 bf 9 6 1570 460 bf 9 6 1579 460 bf 8 6 1588 460 bf 9 6 1596 460 bf 9 6 1605 460 bf 0.2 0 1 c 8 6 1614 460 bf 0.386667 0 1 c 9 6 1666 460 bf 9 6 1814 460 bf 0 1 0.333333 c 9 7 1457 466 bf 0 0.546666 1 c 8 7
1466 466 bf 0.386667 0 1 c 9 7 1474 466 bf 0.2 0 1 c 9 7 1483 466 bf 0.386667 0 1 c 9 7 1492 466 bf 8 7 1501 466 bf 9 7 1509 466 bf 9 7 1518 466 bf 8 7 1588 466 bf 9 7 1596 466 bf 9 7 1622 466 bf 9 7 1640 466 bf 8 7 1736 466 bf 0.2 0 1 c 9 7 1753
466 bf 0.386667 0 1 c 9 7 1457 473 bf 0.88 1 0 c 8 7 1466 473 bf 0.386667 0 1 c 9 7 1474 473 bf 9 7 1483 473 bf 9 7 1492 473 bf 8 7 1501 473 bf 9 7 1518 473 bf 8 7 1527 473 bf 9 7 1544 473 bf 8 7 1553 473 bf 9 7 1561 473 bf 0.2 0 1 c 9 7 1570 473 bf
0.386667 0 1 c 9 7 1579 473 bf 8 7 1588 473 bf 9 7 1596 473 bf 9 7 1622 473 bf 9 7 1631 473 bf 9 7 1640 473 bf 8 7 1675 473 bf 9 7 1683 473 bf 9 7 1709 473 bf 9 7 1718 473 bf 8 7 1736 473 bf 0 1 0.52 c 8 7 1466 480 bf 0.2 0 1 c 9 7 1474 480 bf
0.386667 0 1 c 9 7 1483 480 bf 0.2 0 1 c 9 7 1492 480 bf 0.386667 0 1 c 8 7 1501 480 bf 9 7 1570 480 bf 8 7 1588 480 bf 9 7 1596 480 bf 9 7 1683 480 bf 9 7 1718 480 bf 0 0.0800001 1 c 8 6 1466 487 bf 0.413333 1 0 c 9 6 1474 487 bf 0.386667 0 1 c 9 6
1483 487 bf 9 6 1492 487 bf 9 6 1518 487 bf 8 6 1553 487 bf 9 6 1561 487 bf 9 6 1579 487 bf 8 6 1588 487 bf 9 6 1631 487 bf 8 6 1675 487 bf 8 6 1701 487 bf 9 6 1709 487 bf 9 6 1718 487 bf 8 6 1736 487 bf 0.133333 1 0 c 9 7 1474 493 bf 0.2 0 1 c 9 7
1483 493 bf 0.386667 0 1 c 9 7 1492 493 bf 0.2 0 1 c 9 7 1509 493 bf 0.386667 0 1 c 9 7 1518 493 bf 8 7 1527 493 bf 9 7 1561 493 bf 9 7 1579 493 bf 0.2 0 1 c 8 7 1588 493 bf 0.386667 0 1 c 9 7 1605 493 bf 8 7 1675 493 bf 0 1 0.986667 c 9 7 1474 500
bf 0 0.546666 1 c 9 7 1483 500 bf 0.386667 0 1 c 8 7 1501 500 bf 9 7 1535 500 bf 8 7 1553 500 bf 9 7 1561 500 bf 9 7 1579 500 bf 8 7 1588 500 bf 9 7 1596 500 bf 9 7 1605 500 bf 8 7 1614 500 bf 9 7 1631 500 bf 9 7 1657 500 bf 9 7 1666 500 bf 8 7 1701
500 bf 9 7 1709 500 bf 9 7 1744 500 bf 0 1 0.52 c 9 7 1483 507 bf 0.386667 0 1 c 9 7 1492 507 bf 8 7 1501 507 bf 9 7 1518 507 bf 8 7 1553 507 bf 9 7 1561 507 bf 9 7 1579 507 bf 8 7 1588 507 bf 9 7 1605 507 bf 9 7 1631 507 bf 9 7 1640 507 bf 0
0.266667 1 c 9 6 1483 514 bf 0 0.0800001 1 c 9 6 1492 514 bf 0.386667 0 1 c 8 6 1501 514 bf 9 6 1509 514 bf 9 6 1561 514 bf 9 6 1570 514 bf 9 6 1579 514 bf 9 6 1718 514 bf 0.2 0 1 c 9 7 1483 520 bf 0 0.733333 1 c 9 7 1492 520 bf 0.386667 0 1 c 8 7
1501 520 bf 9 7 1544 520 bf 8 7 1553 520 bf 9 7 1561 520 bf 0.2 0 1 c 9 7 1570 520 bf 0.386667 0 1 c 9 7 1579 520 bf 8 7 1588 520 bf 8 7 1649 520 bf 9 7 1666 520 bf 9 7 1692 520 bf 0 0.0800001 1 c 9 7 1492 527 bf 0.386667 0 1 c 8 7 1501 527 bf 9 7
1535 527 bf 9 7 1544 527 bf 8 7 1553 527 bf 9 7 1561 527 bf 0.2 0 1 c 9 7 1579 527 bf 0.386667 0 1 c 8 7 1588 527 bf 8 7 1614 527 bf 9 7 1622 527 bf 0.2 0 1 c 9 7 1640 527 bf 0.386667 0 1 c 9 7 1683 527 bf 9 7 1492 534 bf 0 0.0800001 1 c 8 7 1501
534 bf 0.386667 0 1 c 8 7 1553 534 bf 9 7 1561 534 bf 9 7 1579 534 bf 9 7 1622 534 bf 9 7 1640 534 bf 8 7 1649 534 bf 9 7 1666 534 bf 8 7 1675 534 bf 0 0.546666 1 c 8 6 1501 541 bf 0.386667 0 1 c 9 6 1535 541 bf 8 6 1553 541 bf 9 6 1570 541 bf 0
0.733333 1 c 8 7 1501 547 bf 0.386667 0 1 c 9 7 1509 547 bf 8 7 1527 547 bf 9 7 1535 547 bf 8 7 1553 547 bf 9 7 1561 547 bf 9 7 1570 547 bf 9 7 1622 547 bf 9 7 1657 547 bf 0 0.546666 1 c 9 7 1509 554 bf 0.386667 0 1 c 9 7 1535 554 bf 9 7 1544 554 bf
9 7 1596 554 bf 9 7 1622 554 bf 9 7 1631 554 bf 9 7 1640 554 bf 8 7 1649 554 bf 9 7 1666 554 bf 0 0.546666 1 c 9 7 1509 561 bf 0.386667 0 1 c 9 7 1518 561 bf 8 7 1527 561 bf 9 7 1535 561 bf 9 7 1544 561 bf 9 7 1561 561 bf 8 7 1614 561 bf 9 7 1622
561 bf 9 6 1509 568 bf 0 0.0800001 1 c 9 6 1518 568 bf 0.386667 0 1 c 9 6 1535 568 bf 9 6 1544 568 bf 8 6 1553 568 bf 9 6 1570 568 bf 0 0.266667 1 c 9 7 1518 574 bf 0.386667 0 1 c 8 7 1527 574 bf 9 7 1579 574 bf 9 7 1596 574 bf 8 7 1614 574 bf 0.2 0
1 c 9 7 1518 581 bf 0 0.546666 1 c 8 7 1527 581 bf 0.386667 0 1 c 9 7 1535 581 bf 9 7 1561 581 bf 9 7 1596 581 bf 9 7 1631 581 bf 0 0.266667 1 c 8 7 1527 588 bf 0.386667 0 1 c 9 7 1544 588 bf 8 7 1553 588 bf 8 6 1527 595 bf 9 6 1535 595 bf 9 6 1544
595 bf 8 7 1527 601 bf 0 0.0800001 1 c 9 7 1535 601 bf 0.386667 0 1 c 9 7 1544 601 bf 9 7 1596 601 bf 9 7 1953 601 bf 0 0.0800001 1 c 9 7 1535 608 bf 0.386667 0 1 c 9 7 1544 608 bf 8 7 1553 608 bf 9 7 1605 608 bf 8 7 1614 608 bf 0 0.0800001 1 c 9 7
1544 615 bf 0.386667 0 1 c 9 7 1596 615 bf 8 7 1736 615 bf 0 0.266667 1 c 9 6 1544 622 bf 0.386667 0 1 c 9 6 1622 622 bf 8 7 1553 628 bf 9 7 1605 628 bf 8 7 1614 628 bf 0.2 0 1 c 8 7 1553 635 bf 0.386667 0 1 c 9 7 1570 635 bf 9 7 1596 635 bf 8 7
1614 635 bf 0.2 0 1 c 8 7 1553 642 bf 0.386667 0 1 c 9 7 1561 642 bf 9 7 1570 642 bf 9 7 1596 642 bf 9 6 1561 649 bf 9 6 1596 649 bf 9 7 1561 655 bf 9 7 1570 655 bf 8 7 1588 655 bf 9 7 1605 655 bf 9 7 1570 662 bf 9 7 1605 662 bf 0.2 0 1 c 9 7 1570
669 bf 0.386667 0 1 c 8 7 1588 669 bf 9 7 1605 669 bf 9 6 1570 676 bf 9 7 1579 682 bf 8 7 1588 682 bf 9 7 1596 682 bf 9 7 1579 689 bf 8 7 1588 689 bf 8 7 1588 696 bf 9 7 1596 696 bf 8 6 1588 703 bf 9 7 1596 709 bf 8 7 1588 716 bf 8 7 1614 750 bf 1 1
1 c black 1265 102 m 871 X s
gsave 1088 843 1157 18 C 1703.06 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 1265 122 m -20 Y s 1283 112 m -10 Y s 1300 112 m -10 Y s 1318 112 m -10 Y s 1335 112 m -10 Y s 1352 122 m -20 Y s 1370
112 m -10 Y s 1387 112 m -10 Y s 1405 112 m -10 Y s 1422 112 m -10 Y s 1440 122 m -20 Y s 1457 112 m -10 Y s 1474 112 m -10 Y s 1492 112 m -10 Y s 1509 112 m -10 Y s 1527 122 m -20 Y s 1544 112 m -10 Y s 1561 112 m -10 Y s 1579 112 m -10 Y s 1596
112 m -10 Y s 1614 122 m -20 Y s 1631 112 m -10 Y s 1649 112 m -10 Y s 1666 112 m -10 Y s 1683 112 m -10 Y s 1701 122 m -20 Y s 1718 112 m -10 Y s 1736 112 m -10 Y s 1753 112 m -10 Y s 1770 112 m -10 Y s 1788 122 m -20 Y s 1805 112 m -10 Y s 1823
112 m -10 Y s 1840 112 m -10 Y s 1858 112 m -10 Y s 1875 122 m -20 Y s 1892 112 m -10 Y s 1910 112 m -10 Y s 1927 112 m -10 Y s 1945 112 m -10 Y s 1962 122 m -20 Y s 1979 112 m -10 Y s 1997 112 m -10 Y s 2014 112 m -10 Y s 2032 112 m -10 Y s 2049
122 m -20 Y s 2067 112 m -10 Y s 2084 112 m -10 Y s 2101 112 m -10 Y s 2119 112 m -10 Y s 2136 122 m -20 Y s
gsave 1088 843 1157 18 C 1254.53 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 843 1157 18 C 1316 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 843 1157 18 C 1402.52 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 843 1157 18 C 1489.04 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 843 1157 18 C 1575.56 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 843 1157 18 C 1664.36 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 843 1157 18 C 1750.88 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 843 1157 18 C 1837.4 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 843 1157 18 C 1923.92 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 843 1157 18 C 2010.44 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 843 1157 18 C 2090.12 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 1265 777 m 871 X s 1265 757 m 20 Y s 1283 767 m 10 Y s 1300 767 m 10 Y s 1318 767 m 10 Y s 1335 767 m 10 Y s 1352 757 m 20 Y s 1370 767 m
10 Y s 1387 767 m 10 Y s 1405 767 m 10 Y s 1422 767 m 10 Y s 1440 757 m 20 Y s 1457 767 m 10 Y s 1474 767 m 10 Y s 1492 767 m 10 Y s 1509 767 m 10 Y s 1527 757 m 20 Y s 1544 767 m 10 Y s 1561 767 m 10 Y s 1579 767 m 10 Y s 1596 767 m 10 Y s 1614 757
m 20 Y s 1631 767 m 10 Y s 1649 767 m 10 Y s 1666 767 m 10 Y s 1683 767 m 10 Y s 1701 757 m 20 Y s 1718 767 m 10 Y s 1736 767 m 10 Y s 1753 767 m 10 Y s 1770 767 m 10 Y s 1788 757 m 20 Y s 1805 767 m 10 Y s 1823 767 m 10 Y s 1840 767 m 10 Y s 1858
767 m 10 Y s 1875 757 m 20 Y s 1892 767 m 10 Y s 1910 767 m 10 Y s 1927 767 m 10 Y s 1945 767 m 10 Y s 1962 757 m 20 Y s 1979 767 m 10 Y s 1997 767 m 10 Y s 2014 767 m 10 Y s 2032 767 m 10 Y s 2049 757 m 20 Y s 2067 767 m 10 Y s 2084 767 m 10 Y s
2101 767 m 10 Y s 2119 767 m 10 Y s 2136 757 m 20 Y s 1265 102 m 675 Y s
gsave 1088 843 1157 18 C 1188.5 521.393 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 1292 102 m -27 X s 1278 118 m -13 X s 1278 134 m -13 X s 1278 150 m -13 X s 1278 166 m -13 X s 1292 182 m -27 X s 1278 198 m -13
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%%EOF

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%%Title: PID115-70keV.eps: c1
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%%CreationDate: Tue Jun 5 22:51:29 2012
%%EndComments
%%BeginProlog
80 dict begin
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/box {m dup 0 exch d exch 0 d 0 exch neg d cl} def
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/K {{pop pop 0 moveto} exch kshow} bind def
/ita {/ang 15 def gsave [1 0 ang dup sin exch cos div 1 0 0] concat} def
/mp {newpath /y exch def /x exch def} def
/side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def
/mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def
/mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def
/mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def
/m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26{mt s} def
/m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def
/m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def
/m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d 0 w3 neg d w3 neg 0 d cl s } def
/m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t 4 {side} repeat cl fill gr} def
/m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t 4 {side} repeat cl s gr} def
/m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d x w2 sub y w2 add m w w neg d x w2 sub y w2 sub m w w d s} def
/m32 {mp x y w2 sub m w2 w d w neg 0 d cl s} def
/m33 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl f} def
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/m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def
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/Bookman-LightItalic /Helvetica-Narrow /Helvetica-Narrow-Bold /Helvetica-Narrow-BoldOblique /Helvetica-Narrow-Oblique /NewCenturySchlbk-Roman /NewCenturySchlbk-Bold /NewCenturySchlbk-BoldItalic /NewCenturySchlbk-Italic /Palatino-Bold
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%%BeginSetup
%%EndSetup
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988 bf 9 6 271 988 bf 8 6 280 988 bf 9 6 288 988 bf 9 6 297 988 bf 8 6 306 988 bf 9 6 314 988 bf 9 6 323 988 bf 9 6 332 988 bf 8 6 341 988 bf 9 6 349 988 bf 9 6 358 988 bf 8 6 367 988 bf 9 6 375 988 bf 9 6 384 988 bf 8 6 393 988 bf 9 6 401 988 bf 9
6 410 988 bf 9 6 419 988 bf 8 6 428 988 bf 9 6 436 988 bf 9 6 445 988 bf 8 6 454 988 bf 9 6 462 988 bf 9 6 471 988 bf 8 6 489 988 bf 9 6 497 988 bf 9 6 523 988 bf 9 6 654 988 bf 9 6 793 988 bf 9 6 828 988 bf 8 7 132 994 bf 9 7 140 994 bf 9 7 149 994
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1001 bf 9 7 332 1001 bf 8 7 341 1001 bf 9 7 349 1001 bf 9 7 358 1001 bf 8 7 367 1001 bf 9 7 375 1001 bf 9 7 445 1001 bf 9 7 480 1001 bf 9 7 506 1001 bf 9 7 541 1001 bf 9 7 567 1001 bf 9 7 750 1001 bf 9 7 140 1008 bf 9 7 149 1008 bf 8 7 158 1008 bf 9
7 166 1008 bf 9 7 175 1008 bf 8 7 184 1008 bf 9 7 192 1008 bf 9 7 201 1008 bf 9 7 210 1008 bf 8 7 219 1008 bf 9 7 227 1008 bf 9 7 236 1008 bf 8 7 245 1008 bf 9 7 253 1008 bf 9 7 262 1008 bf 9 7 271 1008 bf 8 7 280 1008 bf 9 7 288 1008 bf 9 7 297
1008 bf 8 7 341 1008 bf 9 7 358 1008 bf 9 7 375 1008 bf 8 7 515 1008 bf 9 7 593 1008 bf 9 7 645 1008 bf 9 7 680 1008 bf 9 7 750 1008 bf 9 6 140 1015 bf 9 6 149 1015 bf 8 6 158 1015 bf 9 6 166 1015 bf 9 6 175 1015 bf 8 6 184 1015 bf 9 6 192 1015 bf 9
6 201 1015 bf 9 6 210 1015 bf 8 6 219 1015 bf 9 6 227 1015 bf 9 6 236 1015 bf 8 6 245 1015 bf 9 6 262 1015 bf 9 6 271 1015 bf 9 6 297 1015 bf 9 6 314 1015 bf 8 6 341 1015 bf 8 6 367 1015 bf 9 6 436 1015 bf 9 6 462 1015 bf 9 6 471 1015 bf 8 6 663
1015 bf 9 6 837 1015 bf 9 6 863 1015 bf 9 6 889 1015 bf 9 6 924 1015 bf 9 7 149 1021 bf 8 7 158 1021 bf 9 7 166 1021 bf 9 7 175 1021 bf 9 7 192 1021 bf 9 7 201 1021 bf 9 7 210 1021 bf 9 7 227 1021 bf 9 7 236 1021 bf 8 7 245 1021 bf 9 7 253 1021 bf 9
7 262 1021 bf 8 7 280 1021 bf 8 7 306 1021 bf 9 7 314 1021 bf 9 7 349 1021 bf 9 7 358 1021 bf 9 7 471 1021 bf 9 7 706 1021 bf 9 7 767 1021 bf 9 7 837 1021 bf 9 7 880 1021 bf 8 7 933 1021 bf 9 7 967 1021 bf 8 7 994 1021 bf 9 7 149 1028 bf 8 7 158
1028 bf 9 7 166 1028 bf 9 7 175 1028 bf 8 7 184 1028 bf 9 7 192 1028 bf 9 7 210 1028 bf 8 7 219 1028 bf 9 7 227 1028 bf 9 7 236 1028 bf 8 7 245 1028 bf 9 7 262 1028 bf 9 7 271 1028 bf 8 7 367 1028 bf 9 7 375 1028 bf 9 7 384 1028 bf 8 7 550 1028 bf 8
7 576 1028 bf 9 7 828 1028 bf 9 7 863 1028 bf 9 7 898 1028 bf 9 7 967 1028 bf 8 7 994 1028 bf 8 7 158 1035 bf 9 7 166 1035 bf 9 7 192 1035 bf 9 7 201 1035 bf 9 7 227 1035 bf 8 7 341 1035 bf 9 7 358 1035 bf 9 7 384 1035 bf 8 7 393 1035 bf 9 7 401
1035 bf 9 7 628 1035 bf 9 7 828 1035 bf 8 6 158 1042 bf 9 6 166 1042 bf 9 6 175 1042 bf 8 6 184 1042 bf 9 6 192 1042 bf 9 6 201 1042 bf 8 6 219 1042 bf 8 6 245 1042 bf 9 6 253 1042 bf 9 6 271 1042 bf 8 6 280 1042 bf 9 6 297 1042 bf 8 6 306 1042 bf 9
6 314 1042 bf 9 6 323 1042 bf 9 6 332 1042 bf 9 6 349 1042 bf 8 6 515 1042 bf 9 6 941 1042 bf 9 7 166 1048 bf 8 7 184 1048 bf 9 7 253 1048 bf 9 7 262 1048 bf 9 7 271 1048 bf 8 7 280 1048 bf 9 7 288 1048 bf 8 7 306 1048 bf 9 7 323 1048 bf 8 7 341
1048 bf 9 7 541 1048 bf 8 7 698 1048 bf 8 7 846 1048 bf 8 7 933 1048 bf 9 7 941 1048 bf 9 7 985 1048 bf 8 7 994 1048 bf 9 7 166 1055 bf 9 7 175 1055 bf 9 7 210 1055 bf 8 7 245 1055 bf 9 7 253 1055 bf 9 7 262 1055 bf 9 7 271 1055 bf 9 7 297 1055 bf 8
7 306 1055 bf 9 7 323 1055 bf 9 7 332 1055 bf 8 7 785 1055 bf 9 7 837 1055 bf 8 7 872 1055 bf 9 7 880 1055 bf 9 7 889 1055 bf 9 7 898 1055 bf 9 7 915 1055 bf 9 7 941 1055 bf 9 7 950 1055 bf 8 7 959 1055 bf 9 7 967 1055 bf 9 7 976 1055 bf 9 7 985
1055 bf 8 7 994 1055 bf 9 7 166 1062 bf 9 7 175 1062 bf 9 7 192 1062 bf 9 7 227 1062 bf 8 7 245 1062 bf 9 7 253 1062 bf 9 7 262 1062 bf 8 7 280 1062 bf 9 7 297 1062 bf 8 7 306 1062 bf 9 7 314 1062 bf 8 7 393 1062 bf 8 7 428 1062 bf 8 7 602 1062 bf 9
7 706 1062 bf 9 7 793 1062 bf 8 7 811 1062 bf 9 7 828 1062 bf 8 7 872 1062 bf 9 7 880 1062 bf 9 7 889 1062 bf 9 7 898 1062 bf 8 7 907 1062 bf 9 7 915 1062 bf 9 7 924 1062 bf 8 7 933 1062 bf 9 7 941 1062 bf 9 7 950 1062 bf 8 7 959 1062 bf 9 7 967
1062 bf 9 7 976 1062 bf 9 7 985 1062 bf 8 7 994 1062 bf 9 6 175 1069 bf 8 6 184 1069 bf 9 6 192 1069 bf 8 6 245 1069 bf 9 6 253 1069 bf 9 6 271 1069 bf 9 6 288 1069 bf 8 6 306 1069 bf 9 6 384 1069 bf 9 6 715 1069 bf 9 6 741 1069 bf 9 6 776 1069 bf 9
6 837 1069 bf 9 6 854 1069 bf 9 6 863 1069 bf 8 6 872 1069 bf 9 6 880 1069 bf 9 6 889 1069 bf 9 6 898 1069 bf 8 6 907 1069 bf 9 6 915 1069 bf 9 6 924 1069 bf 8 6 933 1069 bf 9 6 941 1069 bf 9 6 950 1069 bf 8 6 959 1069 bf 9 6 967 1069 bf 9 6 976
1069 bf 9 6 985 1069 bf 8 6 994 1069 bf 9 7 175 1075 bf 8 7 184 1075 bf 8 7 245 1075 bf 9 7 262 1075 bf 9 7 271 1075 bf 9 7 323 1075 bf 9 7 567 1075 bf 8 7 759 1075 bf 9 7 767 1075 bf 9 7 776 1075 bf 9 7 793 1075 bf 9 7 802 1075 bf 8 7 811 1075 bf 9
7 819 1075 bf 9 7 828 1075 bf 9 7 837 1075 bf 8 7 846 1075 bf 9 7 854 1075 bf 9 7 863 1075 bf 8 7 872 1075 bf 9 7 880 1075 bf 9 7 889 1075 bf 9 7 898 1075 bf 8 7 907 1075 bf 9 7 915 1075 bf 9 7 924 1075 bf 8 7 933 1075 bf 9 7 941 1075 bf 9 7 950
1075 bf 8 7 959 1075 bf 9 7 967 1075 bf 9 7 976 1075 bf 9 7 985 1075 bf 8 7 994 1075 bf 8 7 184 1082 bf 9 7 192 1082 bf 9 7 236 1082 bf 9 7 253 1082 bf 9 7 262 1082 bf 8 7 280 1082 bf 8 7 306 1082 bf 9 7 332 1082 bf 9 7 349 1082 bf 8 7 367 1082 bf 8
7 393 1082 bf 9 7 567 1082 bf 9 7 689 1082 bf 8 7 698 1082 bf 9 7 715 1082 bf 8 7 724 1082 bf 9 7 732 1082 bf 9 7 741 1082 bf 9 7 750 1082 bf 8 7 759 1082 bf 9 7 767 1082 bf 9 7 776 1082 bf 8 7 785 1082 bf 9 7 793 1082 bf 9 7 802 1082 bf 8 7 811
1082 bf 9 7 819 1082 bf 9 7 828 1082 bf 9 7 837 1082 bf 8 7 846 1082 bf 9 7 854 1082 bf 9 7 863 1082 bf 8 7 872 1082 bf 9 7 880 1082 bf 9 7 889 1082 bf 9 7 898 1082 bf 8 7 907 1082 bf 9 7 915 1082 bf 9 7 924 1082 bf 8 7 933 1082 bf 9 7 941 1082 bf 9
7 950 1082 bf 8 7 959 1082 bf 9 7 976 1082 bf 9 7 985 1082 bf 8 7 994 1082 bf 8 7 184 1089 bf 9 7 192 1089 bf 9 7 227 1089 bf 8 7 245 1089 bf 9 7 271 1089 bf 9 7 297 1089 bf 9 7 349 1089 bf 9 7 523 1089 bf 9 7 628 1089 bf 9 7 689 1089 bf 8 7 698
1089 bf 9 7 706 1089 bf 9 7 715 1089 bf 8 7 724 1089 bf 9 7 732 1089 bf 9 7 741 1089 bf 9 7 750 1089 bf 8 7 759 1089 bf 9 7 767 1089 bf 9 7 776 1089 bf 8 7 785 1089 bf 9 7 793 1089 bf 9 7 802 1089 bf 8 7 811 1089 bf 9 7 819 1089 bf 9 7 828 1089 bf 9
7 837 1089 bf 8 7 846 1089 bf 9 7 854 1089 bf 9 7 863 1089 bf 8 7 872 1089 bf 9 7 880 1089 bf 9 7 889 1089 bf 9 7 898 1089 bf 8 7 907 1089 bf 9 7 915 1089 bf 8 7 933 1089 bf 9 7 941 1089 bf 9 7 950 1089 bf 8 7 959 1089 bf 9 7 976 1089 bf 9 7 985
1089 bf 8 6 184 1096 bf 9 6 192 1096 bf 9 6 201 1096 bf 9 6 227 1096 bf 9 6 236 1096 bf 8 6 245 1096 bf 8 6 280 1096 bf 9 6 332 1096 bf 8 6 393 1096 bf 9 6 645 1096 bf 9 6 654 1096 bf 8 6 663 1096 bf 9 6 671 1096 bf 9 6 680 1096 bf 9 6 689 1096 bf 8
6 698 1096 bf 9 6 706 1096 bf 9 6 715 1096 bf 8 6 724 1096 bf 9 6 732 1096 bf 9 6 741 1096 bf 9 6 750 1096 bf 8 6 759 1096 bf 9 6 767 1096 bf 9 6 776 1096 bf 8 6 785 1096 bf 9 6 793 1096 bf 9 6 802 1096 bf 8 6 811 1096 bf 9 6 819 1096 bf 9 6 828
1096 bf 9 6 837 1096 bf 8 6 846 1096 bf 9 6 854 1096 bf 9 6 863 1096 bf 8 6 872 1096 bf 9 6 880 1096 bf 9 6 889 1096 bf 9 6 898 1096 bf 8 6 907 1096 bf 9 6 915 1096 bf 9 6 924 1096 bf 9 6 941 1096 bf 8 6 959 1096 bf 9 7 192 1102 bf 9 7 201 1102 bf 9
7 227 1102 bf 8 7 341 1102 bf 9 7 462 1102 bf 8 7 576 1102 bf 9 7 584 1102 bf 8 7 602 1102 bf 9 7 619 1102 bf 9 7 628 1102 bf 8 7 637 1102 bf 9 7 645 1102 bf 9 7 654 1102 bf 8 7 663 1102 bf 9 7 671 1102 bf 9 7 680 1102 bf 9 7 689 1102 bf 8 7 698
1102 bf 9 7 706 1102 bf 9 7 715 1102 bf 8 7 724 1102 bf 9 7 732 1102 bf 9 7 741 1102 bf 9 7 750 1102 bf 8 7 759 1102 bf 9 7 767 1102 bf 9 7 776 1102 bf 8 7 785 1102 bf 9 7 793 1102 bf 9 7 802 1102 bf 8 7 811 1102 bf 9 7 819 1102 bf 9 7 828 1102 bf 9
7 854 1102 bf 9 7 863 1102 bf 9 7 898 1102 bf 9 7 985 1102 bf 9 7 192 1109 bf 9 7 201 1109 bf 8 7 219 1109 bf 9 7 262 1109 bf 9 7 332 1109 bf 9 7 410 1109 bf 9 7 567 1109 bf 9 7 584 1109 bf 9 7 593 1109 bf 8 7 602 1109 bf 9 7 610 1109 bf 9 7 619
1109 bf 9 7 628 1109 bf 8 7 637 1109 bf 9 7 645 1109 bf 9 7 654 1109 bf 8 7 663 1109 bf 9 7 671 1109 bf 9 7 680 1109 bf 9 7 689 1109 bf 8 7 698 1109 bf 9 7 706 1109 bf 9 7 715 1109 bf 8 7 724 1109 bf 9 7 732 1109 bf 9 7 741 1109 bf 9 7 750 1109 bf 8
7 759 1109 bf 9 7 767 1109 bf 9 7 776 1109 bf 9 7 793 1109 bf 9 7 802 1109 bf 9 7 819 1109 bf 9 7 837 1109 bf 9 7 889 1109 bf 9 7 201 1116 bf 9 7 210 1116 bf 9 7 253 1116 bf 9 7 314 1116 bf 9 7 401 1116 bf 8 7 550 1116 bf 9 7 567 1116 bf 8 7 576
1116 bf 9 7 584 1116 bf 9 7 593 1116 bf 8 7 602 1116 bf 9 7 610 1116 bf 9 7 619 1116 bf 9 7 628 1116 bf 8 7 637 1116 bf 9 7 645 1116 bf 9 7 654 1116 bf 8 7 663 1116 bf 9 7 671 1116 bf 9 7 680 1116 bf 9 7 689 1116 bf 8 7 698 1116 bf 9 7 706 1116 bf 9
7 715 1116 bf 8 7 724 1116 bf 9 7 732 1116 bf 9 7 741 1116 bf 9 7 750 1116 bf 8 7 759 1116 bf 9 7 767 1116 bf 9 7 776 1116 bf 9 7 793 1116 bf 9 7 802 1116 bf 8 7 811 1116 bf 9 7 819 1116 bf 9 7 828 1116 bf 9 7 837 1116 bf 9 7 985 1116 bf 9 6 201
1123 bf 9 6 210 1123 bf 8 6 219 1123 bf 9 6 227 1123 bf 9 6 253 1123 bf 8 6 280 1123 bf 9 6 288 1123 bf 9 6 532 1123 bf 8 6 550 1123 bf 9 6 558 1123 bf 9 6 567 1123 bf 8 6 576 1123 bf 9 6 584 1123 bf 9 6 593 1123 bf 8 6 602 1123 bf 9 6 610 1123 bf 9
6 619 1123 bf 9 6 628 1123 bf 8 6 637 1123 bf 9 6 645 1123 bf 9 6 654 1123 bf 8 6 663 1123 bf 9 6 671 1123 bf 9 6 680 1123 bf 9 6 689 1123 bf 8 6 698 1123 bf 9 6 706 1123 bf 8 6 724 1123 bf 9 6 732 1123 bf 9 6 741 1123 bf 9 6 750 1123 bf 8 6 785
1123 bf 8 6 907 1123 bf 8 6 933 1123 bf 9 6 967 1123 bf 9 6 976 1123 bf 9 6 985 1123 bf 8 6 994 1123 bf 9 7 210 1129 bf 9 7 227 1129 bf 8 7 245 1129 bf 9 7 253 1129 bf 9 7 323 1129 bf 9 7 523 1129 bf 9 7 532 1129 bf 8 7 550 1129 bf 9 7 558 1129 bf 9
7 567 1129 bf 8 7 576 1129 bf 9 7 584 1129 bf 9 7 593 1129 bf 8 7 602 1129 bf 9 7 610 1129 bf 9 7 619 1129 bf 9 7 628 1129 bf 8 7 637 1129 bf 9 7 645 1129 bf 9 7 654 1129 bf 8 7 663 1129 bf 9 7 671 1129 bf 9 7 680 1129 bf 9 7 689 1129 bf 9 7 715
1129 bf 9 7 741 1129 bf 8 7 846 1129 bf 9 7 889 1129 bf 9 7 898 1129 bf 9 7 915 1129 bf 9 7 924 1129 bf 9 7 950 1129 bf 8 7 959 1129 bf 9 7 967 1129 bf 9 7 985 1129 bf 8 7 994 1129 bf 9 7 210 1136 bf 8 7 219 1136 bf 9 7 297 1136 bf 8 7 489 1136 bf 9
7 506 1136 bf 8 7 515 1136 bf 9 7 523 1136 bf 9 7 532 1136 bf 9 7 541 1136 bf 8 7 550 1136 bf 9 7 558 1136 bf 9 7 567 1136 bf 8 7 576 1136 bf 9 7 584 1136 bf 9 7 593 1136 bf 8 7 602 1136 bf 9 7 610 1136 bf 9 7 619 1136 bf 9 7 628 1136 bf 8 7 637
1136 bf 9 7 645 1136 bf 9 7 654 1136 bf 8 7 663 1136 bf 9 7 671 1136 bf 9 7 680 1136 bf 9 7 689 1136 bf 9 7 706 1136 bf 9 7 715 1136 bf 9 7 750 1136 bf 9 7 767 1136 bf 9 7 828 1136 bf 9 7 854 1136 bf 9 7 863 1136 bf 9 7 889 1136 bf 9 7 898 1136 bf 9
7 915 1136 bf 9 7 924 1136 bf 9 7 941 1136 bf 9 7 950 1136 bf 9 7 967 1136 bf 9 7 976 1136 bf 9 7 985 1136 bf 9 7 210 1143 bf 8 7 219 1143 bf 9 7 236 1143 bf 9 7 349 1143 bf 8 7 454 1143 bf 9 7 480 1143 bf 8 7 489 1143 bf 9 7 497 1143 bf 9 7 506
1143 bf 8 7 515 1143 bf 9 7 523 1143 bf 9 7 532 1143 bf 9 7 541 1143 bf 8 7 550 1143 bf 9 7 558 1143 bf 9 7 567 1143 bf 8 7 576 1143 bf 9 7 584 1143 bf 9 7 593 1143 bf 8 7 602 1143 bf 9 7 610 1143 bf 9 7 619 1143 bf 9 7 628 1143 bf 9 7 645 1143 bf 9
7 654 1143 bf 8 7 698 1143 bf 9 7 802 1143 bf 9 7 828 1143 bf 9 7 854 1143 bf 9 7 863 1143 bf 8 7 872 1143 bf 9 7 880 1143 bf 9 7 898 1143 bf 8 7 907 1143 bf 9 7 915 1143 bf 8 7 933 1143 bf 9 7 950 1143 bf 8 7 994 1143 bf 8 6 219 1150 bf 9 6 227
1150 bf 8 6 245 1150 bf 9 6 471 1150 bf 9 6 480 1150 bf 8 6 489 1150 bf 9 6 497 1150 bf 9 6 506 1150 bf 8 6 515 1150 bf 9 6 523 1150 bf 9 6 532 1150 bf 9 6 541 1150 bf 8 6 550 1150 bf 9 6 558 1150 bf 9 6 567 1150 bf 8 6 576 1150 bf 9 6 584 1150 bf 9
6 593 1150 bf 8 6 602 1150 bf 9 6 610 1150 bf 9 6 619 1150 bf 9 6 628 1150 bf 8 6 637 1150 bf 9 6 654 1150 bf 9 6 689 1150 bf 9 6 767 1150 bf 8 6 785 1150 bf 9 6 819 1150 bf 9 6 828 1150 bf 9 6 837 1150 bf 8 6 846 1150 bf 9 6 854 1150 bf 9 6 863
1150 bf 8 6 872 1150 bf 9 6 880 1150 bf 9 6 889 1150 bf 9 6 898 1150 bf 9 6 915 1150 bf 9 6 924 1150 bf 8 6 933 1150 bf 8 6 959 1150 bf 9 6 967 1150 bf 8 7 219 1156 bf 9 7 227 1156 bf 9 7 262 1156 bf 9 7 462 1156 bf 9 7 471 1156 bf 9 7 480 1156 bf 8
7 489 1156 bf 9 7 497 1156 bf 9 7 506 1156 bf 8 7 515 1156 bf 9 7 523 1156 bf 9 7 532 1156 bf 9 7 541 1156 bf 8 7 550 1156 bf 9 7 558 1156 bf 9 7 567 1156 bf 8 7 576 1156 bf 9 7 584 1156 bf 9 7 593 1156 bf 8 7 602 1156 bf 9 7 610 1156 bf 9 7 619
1156 bf 9 7 645 1156 bf 8 7 663 1156 bf 9 7 671 1156 bf 9 7 741 1156 bf 9 7 750 1156 bf 9 7 776 1156 bf 8 7 785 1156 bf 9 7 802 1156 bf 8 7 811 1156 bf 9 7 819 1156 bf 9 7 828 1156 bf 9 7 837 1156 bf 9 7 854 1156 bf 8 7 872 1156 bf 9 7 880 1156 bf 9
7 889 1156 bf 9 7 898 1156 bf 8 7 933 1156 bf 9 7 967 1156 bf 9 7 227 1163 bf 9 7 253 1163 bf 8 7 454 1163 bf 9 7 462 1163 bf 9 7 471 1163 bf 9 7 480 1163 bf 8 7 489 1163 bf 9 7 497 1163 bf 9 7 506 1163 bf 8 7 515 1163 bf 9 7 523 1163 bf 9 7 532
1163 bf 9 7 541 1163 bf 8 7 550 1163 bf 9 7 558 1163 bf 9 7 567 1163 bf 8 7 576 1163 bf 9 7 593 1163 bf 8 7 637 1163 bf 9 7 654 1163 bf 8 7 663 1163 bf 9 7 689 1163 bf 9 7 732 1163 bf 9 7 750 1163 bf 8 7 759 1163 bf 9 7 767 1163 bf 8 7 785 1163 bf 9
7 793 1163 bf 9 7 802 1163 bf 8 7 811 1163 bf 9 7 819 1163 bf 9 7 828 1163 bf 9 7 837 1163 bf 8 7 846 1163 bf 9 7 854 1163 bf 8 7 872 1163 bf 9 7 880 1163 bf 8 7 907 1163 bf 9 7 227 1170 bf 9 7 236 1170 bf 9 7 436 1170 bf 9 7 445 1170 bf 8 7 454
1170 bf 9 7 462 1170 bf 9 7 471 1170 bf 9 7 480 1170 bf 8 7 489 1170 bf 9 7 497 1170 bf 9 7 506 1170 bf 8 7 515 1170 bf 9 7 523 1170 bf 9 7 532 1170 bf 9 7 541 1170 bf 8 7 550 1170 bf 8 7 576 1170 bf 9 7 584 1170 bf 9 7 610 1170 bf 8 7 637 1170 bf 9
7 645 1170 bf 9 7 689 1170 bf 8 7 698 1170 bf 9 7 715 1170 bf 8 7 724 1170 bf 9 7 732 1170 bf 9 7 741 1170 bf 9 7 750 1170 bf 8 7 759 1170 bf 9 7 767 1170 bf 9 7 776 1170 bf 8 7 785 1170 bf 9 7 793 1170 bf 9 7 819 1170 bf 9 7 828 1170 bf 8 7 846
1170 bf 8 7 994 1170 bf 9 6 227 1177 bf 9 6 236 1177 bf 9 6 419 1177 bf 8 6 428 1177 bf 9 6 436 1177 bf 9 6 445 1177 bf 8 6 454 1177 bf 9 6 462 1177 bf 9 6 471 1177 bf 9 6 480 1177 bf 8 6 489 1177 bf 9 6 497 1177 bf 9 6 506 1177 bf 8 6 515 1177 bf 9
6 523 1177 bf 9 6 532 1177 bf 9 6 541 1177 bf 8 6 550 1177 bf 9 6 567 1177 bf 9 6 593 1177 bf 9 6 680 1177 bf 8 6 698 1177 bf 9 6 706 1177 bf 9 6 715 1177 bf 8 6 724 1177 bf 9 6 732 1177 bf 9 6 741 1177 bf 9 6 750 1177 bf 8 6 759 1177 bf 9 6 767
1177 bf 9 6 776 1177 bf 8 6 785 1177 bf 9 6 793 1177 bf 9 6 802 1177 bf 8 6 811 1177 bf 9 6 950 1177 bf 8 6 959 1177 bf 9 7 236 1183 bf 8 7 245 1183 bf 9 7 419 1183 bf 8 7 428 1183 bf 9 7 436 1183 bf 9 7 445 1183 bf 8 7 454 1183 bf 9 7 462 1183 bf 9
7 471 1183 bf 9 7 480 1183 bf 8 7 489 1183 bf 9 7 497 1183 bf 9 7 506 1183 bf 8 7 515 1183 bf 9 7 523 1183 bf 9 7 532 1183 bf 8 7 550 1183 bf 8 7 637 1183 bf 9 7 689 1183 bf 8 7 698 1183 bf 9 7 706 1183 bf 9 7 715 1183 bf 8 7 724 1183 bf 9 7 732
1183 bf 9 7 741 1183 bf 9 7 750 1183 bf 9 7 767 1183 bf 9 7 802 1183 bf 8 7 811 1183 bf 9 7 828 1183 bf 9 7 915 1183 bf 9 7 941 1183 bf 9 7 950 1183 bf 9 7 976 1183 bf 9 7 985 1183 bf 8 7 994 1183 bf 9 7 236 1190 bf 8 7 245 1190 bf 9 7 410 1190 bf 9
7 419 1190 bf 8 7 428 1190 bf 9 7 436 1190 bf 9 7 445 1190 bf 8 7 454 1190 bf 9 7 462 1190 bf 9 7 471 1190 bf 9 7 480 1190 bf 8 7 489 1190 bf 9 7 497 1190 bf 9 7 506 1190 bf 8 7 515 1190 bf 9 7 523 1190 bf 9 7 532 1190 bf 9 7 558 1190 bf 8 7 576
1190 bf 8 7 637 1190 bf 8 7 663 1190 bf 9 7 671 1190 bf 9 7 680 1190 bf 9 7 689 1190 bf 8 7 698 1190 bf 9 7 706 1190 bf 9 7 715 1190 bf 8 7 724 1190 bf 9 7 732 1190 bf 9 7 750 1190 bf 8 7 759 1190 bf 9 7 767 1190 bf 9 7 776 1190 bf 9 7 793 1190 bf 9
7 915 1190 bf 9 7 941 1190 bf 9 7 985 1190 bf 8 7 245 1197 bf 9 7 401 1197 bf 9 7 410 1197 bf 9 7 419 1197 bf 8 7 428 1197 bf 9 7 436 1197 bf 9 7 445 1197 bf 8 7 454 1197 bf 9 7 462 1197 bf 9 7 471 1197 bf 9 7 480 1197 bf 8 7 489 1197 bf 9 7 497
1197 bf 9 7 506 1197 bf 9 7 523 1197 bf 9 7 558 1197 bf 9 7 628 1197 bf 8 7 637 1197 bf 9 7 645 1197 bf 9 7 654 1197 bf 8 7 663 1197 bf 9 7 671 1197 bf 9 7 680 1197 bf 9 7 689 1197 bf 8 7 698 1197 bf 9 7 706 1197 bf 9 7 715 1197 bf 9 7 732 1197 bf 9
7 750 1197 bf 9 7 837 1197 bf 8 7 907 1197 bf 9 7 915 1197 bf 8 7 933 1197 bf 8 6 245 1204 bf 9 6 253 1204 bf 8 6 393 1204 bf 9 6 401 1204 bf 9 6 410 1204 bf 9 6 419 1204 bf 8 6 428 1204 bf 9 6 436 1204 bf 9 6 445 1204 bf 8 6 454 1204 bf 9 6 462
1204 bf 9 6 480 1204 bf 8 6 489 1204 bf 9 6 497 1204 bf 9 6 506 1204 bf 9 6 610 1204 bf 9 6 619 1204 bf 9 6 628 1204 bf 8 6 637 1204 bf 9 6 645 1204 bf 9 6 654 1204 bf 8 6 663 1204 bf 9 6 671 1204 bf 9 6 689 1204 bf 8 6 698 1204 bf 9 6 863 1204 bf 8
6 872 1204 bf 9 6 889 1204 bf 8 6 907 1204 bf 9 6 924 1204 bf 9 6 950 1204 bf 8 6 959 1204 bf 8 7 245 1210 bf 9 7 253 1210 bf 8 7 393 1210 bf 9 7 401 1210 bf 9 7 410 1210 bf 9 7 419 1210 bf 8 7 428 1210 bf 9 7 436 1210 bf 9 7 445 1210 bf 8 7 454
1210 bf 9 7 462 1210 bf 9 7 480 1210 bf 8 7 489 1210 bf 8 7 515 1210 bf 9 7 593 1210 bf 8 7 602 1210 bf 9 7 610 1210 bf 9 7 619 1210 bf 9 7 628 1210 bf 8 7 637 1210 bf 9 7 645 1210 bf 9 7 654 1210 bf 8 7 663 1210 bf 9 7 671 1210 bf 9 7 680 1210 bf 9
7 689 1210 bf 9 7 715 1210 bf 9 7 741 1210 bf 9 7 828 1210 bf 8 7 846 1210 bf 9 7 854 1210 bf 9 7 863 1210 bf 8 7 907 1210 bf 9 7 924 1210 bf 9 7 253 1217 bf 9 7 262 1217 bf 9 7 384 1217 bf 8 7 393 1217 bf 9 7 401 1217 bf 9 7 410 1217 bf 9 7 419
1217 bf 8 7 428 1217 bf 9 7 445 1217 bf 8 7 454 1217 bf 9 7 462 1217 bf 9 7 480 1217 bf 9 7 497 1217 bf 8 7 515 1217 bf 9 7 584 1217 bf 9 7 593 1217 bf 8 7 602 1217 bf 9 7 610 1217 bf 9 7 619 1217 bf 9 7 628 1217 bf 8 7 637 1217 bf 9 7 645 1217 bf 9
7 654 1217 bf 8 7 663 1217 bf 9 7 671 1217 bf 9 7 689 1217 bf 9 7 776 1217 bf 9 7 802 1217 bf 9 7 828 1217 bf 9 7 889 1217 bf 9 7 253 1224 bf 9 7 262 1224 bf 9 7 384 1224 bf 8 7 393 1224 bf 9 7 401 1224 bf 9 7 410 1224 bf 9 7 419 1224 bf 9 7 436
1224 bf 9 7 445 1224 bf 8 7 454 1224 bf 9 7 462 1224 bf 9 7 480 1224 bf 9 7 506 1224 bf 9 7 593 1224 bf 8 7 602 1224 bf 9 7 610 1224 bf 9 7 619 1224 bf 9 7 628 1224 bf 8 7 637 1224 bf 9 7 645 1224 bf 9 7 654 1224 bf 8 7 663 1224 bf 9 7 715 1224 bf 9
7 767 1224 bf 8 7 785 1224 bf 9 7 793 1224 bf 9 7 819 1224 bf 9 7 863 1224 bf 9 6 262 1231 bf 9 6 271 1231 bf 9 6 375 1231 bf 9 6 384 1231 bf 8 6 393 1231 bf 9 6 401 1231 bf 9 6 410 1231 bf 9 6 419 1231 bf 9 6 445 1231 bf 8 6 454 1231 bf 9 6 471
1231 bf 9 6 480 1231 bf 9 6 497 1231 bf 8 6 576 1231 bf 9 6 584 1231 bf 9 6 593 1231 bf 8 6 602 1231 bf 9 6 610 1231 bf 9 6 619 1231 bf 9 6 628 1231 bf 8 6 637 1231 bf 9 6 767 1231 bf 9 6 802 1231 bf 8 6 811 1231 bf 8 6 846 1231 bf 9 7 262 1237 bf 9
7 271 1237 bf 8 7 367 1237 bf 9 7 375 1237 bf 9 7 384 1237 bf 8 7 393 1237 bf 9 7 401 1237 bf 9 7 410 1237 bf 9 7 419 1237 bf 9 7 436 1237 bf 9 7 445 1237 bf 9 7 462 1237 bf 9 7 471 1237 bf 8 7 489 1237 bf 9 7 532 1237 bf 9 7 558 1237 bf 9 7 567
1237 bf 8 7 576 1237 bf 9 7 584 1237 bf 9 7 593 1237 bf 8 7 602 1237 bf 9 7 610 1237 bf 9 7 628 1237 bf 9 7 671 1237 bf 9 7 715 1237 bf 8 7 724 1237 bf 9 7 741 1237 bf 9 7 776 1237 bf 8 7 785 1237 bf 9 7 793 1237 bf 9 7 802 1237 bf 9 7 819 1237 bf 9
7 828 1237 bf 9 7 271 1244 bf 9 7 297 1244 bf 8 7 367 1244 bf 9 7 375 1244 bf 9 7 384 1244 bf 8 7 393 1244 bf 9 7 401 1244 bf 9 7 410 1244 bf 9 7 419 1244 bf 8 7 428 1244 bf 9 7 436 1244 bf 8 7 454 1244 bf 9 7 471 1244 bf 8 7 489 1244 bf 9 7 523
1244 bf 8 7 550 1244 bf 9 7 558 1244 bf 9 7 567 1244 bf 8 7 576 1244 bf 9 7 584 1244 bf 9 7 593 1244 bf 9 7 610 1244 bf 9 7 619 1244 bf 9 7 645 1244 bf 8 7 698 1244 bf 8 7 724 1244 bf 9 7 732 1244 bf 9 7 741 1244 bf 8 7 759 1244 bf 9 7 767 1244 bf 8
7 785 1244 bf 9 7 793 1244 bf 9 7 802 1244 bf 9 7 271 1251 bf 8 7 280 1251 bf 9 7 358 1251 bf 8 7 367 1251 bf 9 7 375 1251 bf 9 7 384 1251 bf 8 7 393 1251 bf 9 7 401 1251 bf 9 7 410 1251 bf 9 7 419 1251 bf 9 7 436 1251 bf 9 7 532 1251 bf 9 7 541
1251 bf 8 7 550 1251 bf 9 7 558 1251 bf 9 7 567 1251 bf 8 7 576 1251 bf 9 7 584 1251 bf 8 7 602 1251 bf 8 7 698 1251 bf 9 7 706 1251 bf 9 7 715 1251 bf 8 7 724 1251 bf 9 7 732 1251 bf 9 7 750 1251 bf 9 7 767 1251 bf 8 7 785 1251 bf 8 6 280 1258 bf 8
6 367 1258 bf 9 6 375 1258 bf 9 6 384 1258 bf 8 6 393 1258 bf 9 6 401 1258 bf 9 6 410 1258 bf 8 6 428 1258 bf 8 6 454 1258 bf 9 6 523 1258 bf 9 6 532 1258 bf 9 6 541 1258 bf 8 6 550 1258 bf 9 6 567 1258 bf 8 6 576 1258 bf 9 6 584 1258 bf 9 6 628
1258 bf 9 6 680 1258 bf 9 6 689 1258 bf 8 6 698 1258 bf 9 6 732 1258 bf 9 6 741 1258 bf 8 7 280 1264 bf 9 7 288 1264 bf 9 7 358 1264 bf 8 7 367 1264 bf 9 7 375 1264 bf 9 7 384 1264 bf 8 7 393 1264 bf 9 7 401 1264 bf 9 7 419 1264 bf 8 7 428 1264 bf 9
7 436 1264 bf 9 7 445 1264 bf 9 7 480 1264 bf 8 7 489 1264 bf 8 7 515 1264 bf 9 7 523 1264 bf 9 7 532 1264 bf 9 7 558 1264 bf 9 7 567 1264 bf 9 7 584 1264 bf 9 7 689 1264 bf 8 7 698 1264 bf 9 7 706 1264 bf 9 7 715 1264 bf 8 7 724 1264 bf 9 7 741
1264 bf 8 7 759 1264 bf 8 7 280 1271 bf 9 7 288 1271 bf 8 7 306 1271 bf 9 7 358 1271 bf 8 7 367 1271 bf 9 7 375 1271 bf 9 7 384 1271 bf 8 7 393 1271 bf 9 7 410 1271 bf 9 7 419 1271 bf 8 7 428 1271 bf 9 7 471 1271 bf 9 7 497 1271 bf 9 7 506 1271 bf 8
7 515 1271 bf 9 7 523 1271 bf 9 7 532 1271 bf 9 7 541 1271 bf 8 7 550 1271 bf 9 7 584 1271 bf 9 7 654 1271 bf 8 7 663 1271 bf 9 7 671 1271 bf 9 7 680 1271 bf 9 7 689 1271 bf 8 7 698 1271 bf 9 7 715 1271 bf 8 7 724 1271 bf 9 7 741 1271 bf 9 7 288
1278 bf 9 7 297 1278 bf 9 7 349 1278 bf 9 7 358 1278 bf 8 7 367 1278 bf 9 7 375 1278 bf 8 7 393 1278 bf 9 7 401 1278 bf 8 7 428 1278 bf 9 7 506 1278 bf 8 7 515 1278 bf 9 7 532 1278 bf 9 7 541 1278 bf 9 7 567 1278 bf 9 7 654 1278 bf 8 7 663 1278 bf 9
7 671 1278 bf 9 7 689 1278 bf 8 7 698 1278 bf 9 7 706 1278 bf 9 7 750 1278 bf 9 6 288 1285 bf 9 6 297 1285 bf 9 6 349 1285 bf 9 6 358 1285 bf 8 6 367 1285 bf 9 6 375 1285 bf 9 6 384 1285 bf 8 6 393 1285 bf 9 6 410 1285 bf 9 6 419 1285 bf 9 6 497
1285 bf 9 6 506 1285 bf 8 6 515 1285 bf 9 6 523 1285 bf 9 6 541 1285 bf 9 6 558 1285 bf 9 6 654 1285 bf 9 6 680 1285 bf 8 6 698 1285 bf 9 7 297 1291 bf 9 7 349 1291 bf 9 7 358 1291 bf 8 7 367 1291 bf 9 7 375 1291 bf 9 7 384 1291 bf 8 7 393 1291 bf 9
7 401 1291 bf 9 7 410 1291 bf 8 7 428 1291 bf 9 7 480 1291 bf 8 7 489 1291 bf 9 7 497 1291 bf 9 7 506 1291 bf 8 7 515 1291 bf 9 7 523 1291 bf 9 7 532 1291 bf 9 7 654 1291 bf 9 7 671 1291 bf 9 7 706 1291 bf 9 7 297 1298 bf 8 7 306 1298 bf 9 7 349
1298 bf 9 7 358 1298 bf 8 7 367 1298 bf 9 7 375 1298 bf 9 7 384 1298 bf 8 7 393 1298 bf 9 7 401 1298 bf 9 7 480 1298 bf 8 7 489 1298 bf 9 7 506 1298 bf 9 7 523 1298 bf 8 7 602 1298 bf 9 7 610 1298 bf 9 7 619 1298 bf 9 7 628 1298 bf 8 7 637 1298 bf 9
7 645 1298 bf 8 7 663 1298 bf 9 7 297 1305 bf 8 7 306 1305 bf 8 7 341 1305 bf 9 7 349 1305 bf 9 7 358 1305 bf 8 7 367 1305 bf 9 7 375 1305 bf 9 7 384 1305 bf 8 7 393 1305 bf 9 7 401 1305 bf 8 7 454 1305 bf 9 7 471 1305 bf 9 7 480 1305 bf 8 7 489
1305 bf 9 7 497 1305 bf 9 7 506 1305 bf 9 7 541 1305 bf 8 7 550 1305 bf 8 7 602 1305 bf 9 7 619 1305 bf 9 7 628 1305 bf 9 7 645 1305 bf 8 6 306 1312 bf 9 6 314 1312 bf 9 6 349 1312 bf 9 6 358 1312 bf 8 6 367 1312 bf 9 6 375 1312 bf 9 6 384 1312 bf 9
6 436 1312 bf 9 6 462 1312 bf 9 6 471 1312 bf 9 6 480 1312 bf 8 6 489 1312 bf 9 6 497 1312 bf 9 6 506 1312 bf 9 6 593 1312 bf 9 6 610 1312 bf 9 6 619 1312 bf 9 6 628 1312 bf 9 6 645 1312 bf 8 7 306 1318 bf 9 7 314 1318 bf 8 7 341 1318 bf 9 7 349
1318 bf 9 7 358 1318 bf 8 7 367 1318 bf 9 7 462 1318 bf 9 7 471 1318 bf 9 7 480 1318 bf 8 7 489 1318 bf 8 7 515 1318 bf 8 7 576 1318 bf 8 7 602 1318 bf 9 7 610 1318 bf 8 7 637 1318 bf 9 7 654 1318 bf 9 7 314 1325 bf 9 7 323 1325 bf 8 7 341 1325 bf 9
7 349 1325 bf 9 7 358 1325 bf 9 7 375 1325 bf 9 7 384 1325 bf 9 7 401 1325 bf 9 7 471 1325 bf 9 7 480 1325 bf 8 7 489 1325 bf 9 7 497 1325 bf 9 7 523 1325 bf 9 7 593 1325 bf 9 7 610 1325 bf 9 7 628 1325 bf 9 7 671 1325 bf 9 7 776 1325 bf 9 7 793
1325 bf 9 7 802 1325 bf 9 7 314 1332 bf 9 7 323 1332 bf 8 7 341 1332 bf 9 7 349 1332 bf 9 7 358 1332 bf 8 7 367 1332 bf 9 7 375 1332 bf 9 7 384 1332 bf 8 7 393 1332 bf 9 7 445 1332 bf 9 7 462 1332 bf 9 7 471 1332 bf 9 7 480 1332 bf 8 7 489 1332 bf 9
7 497 1332 bf 9 7 593 1332 bf 9 6 314 1339 bf 9 6 323 1339 bf 8 6 341 1339 bf 9 6 349 1339 bf 9 6 358 1339 bf 8 6 454 1339 bf 9 6 462 1339 bf 8 6 489 1339 bf 8 6 576 1339 bf 9 6 584 1339 bf 9 6 619 1339 bf 9 7 323 1345 bf 9 7 332 1345 bf 8 7 341
1345 bf 9 7 349 1345 bf 9 7 358 1345 bf 9 7 375 1345 bf 9 7 384 1345 bf 8 7 393 1345 bf 9 7 419 1345 bf 8 7 454 1345 bf 9 7 462 1345 bf 9 7 471 1345 bf 9 7 558 1345 bf 9 7 567 1345 bf 8 7 576 1345 bf 9 7 584 1345 bf 9 7 593 1345 bf 8 7 602 1345 bf 9
7 323 1352 bf 9 7 332 1352 bf 8 7 341 1352 bf 9 7 349 1352 bf 9 7 358 1352 bf 8 7 367 1352 bf 9 7 375 1352 bf 8 7 393 1352 bf 9 7 445 1352 bf 8 7 454 1352 bf 9 7 462 1352 bf 9 7 471 1352 bf 8 7 489 1352 bf 9 7 584 1352 bf 9 7 593 1352 bf 9 7 332
1359 bf 8 7 341 1359 bf 9 7 349 1359 bf 8 7 367 1359 bf 9 7 375 1359 bf 9 7 419 1359 bf 9 7 436 1359 bf 9 7 445 1359 bf 8 7 454 1359 bf 9 7 462 1359 bf 9 7 558 1359 bf 8 7 576 1359 bf 9 7 584 1359 bf 9 7 593 1359 bf 9 6 332 1366 bf 8 6 341 1366 bf 9
6 349 1366 bf 9 6 375 1366 bf 9 6 384 1366 bf 9 6 436 1366 bf 9 6 445 1366 bf 8 6 454 1366 bf 9 6 462 1366 bf 8 6 550 1366 bf 8 7 341 1372 bf 9 7 349 1372 bf 9 7 358 1372 bf 8 7 367 1372 bf 8 7 428 1372 bf 9 7 436 1372 bf 9 7 445 1372 bf 9 7 462
1372 bf 9 7 558 1372 bf 8 7 341 1379 bf 9 7 349 1379 bf 8 7 367 1379 bf 8 7 393 1379 bf 9 7 419 1379 bf 8 7 428 1379 bf 9 7 436 1379 bf 9 7 445 1379 bf 9 7 462 1379 bf 9 7 532 1379 bf 9 7 541 1379 bf 8 7 341 1386 bf 9 7 349 1386 bf 9 7 358 1386 bf 8
7 367 1386 bf 9 7 384 1386 bf 8 7 393 1386 bf 9 7 436 1386 bf 9 7 445 1386 bf 9 7 532 1386 bf 8 7 550 1386 bf 9 6 349 1393 bf 9 6 358 1393 bf 9 6 375 1393 bf 8 6 428 1393 bf 9 6 436 1393 bf 9 6 445 1393 bf 9 7 349 1399 bf 9 7 358 1399 bf 8 7 367
1399 bf 9 7 419 1399 bf 8 7 428 1399 bf 9 7 436 1399 bf 9 7 506 1399 bf 9 7 523 1399 bf 9 7 558 1399 bf 9 7 358 1406 bf 8 7 367 1406 bf 9 7 410 1406 bf 8 7 428 1406 bf 9 7 445 1406 bf 9 7 506 1406 bf 8 7 515 1406 bf 9 7 358 1413 bf 8 7 367 1413 bf 9
7 375 1413 bf 9 7 384 1413 bf 9 7 401 1413 bf 9 7 410 1413 bf 9 7 419 1413 bf 8 7 428 1413 bf 9 7 436 1413 bf 9 7 462 1413 bf 9 7 506 1413 bf 8 7 515 1413 bf 9 7 584 1413 bf 8 6 367 1420 bf 9 6 401 1420 bf 9 6 419 1420 bf 8 6 428 1420 bf 9 6 436
1420 bf 8 6 489 1420 bf 9 6 497 1420 bf 8 6 515 1420 bf 9 6 523 1420 bf 8 7 367 1426 bf 9 7 375 1426 bf 9 7 410 1426 bf 9 7 419 1426 bf 8 7 428 1426 bf 9 7 793 1426 bf 9 7 375 1433 bf 8 7 393 1433 bf 8 7 489 1433 bf 9 7 497 1433 bf 9 7 506 1433 bf 9
7 523 1433 bf 9 7 375 1440 bf 9 7 384 1440 bf 9 7 410 1440 bf 9 7 419 1440 bf 9 7 480 1440 bf 8 7 489 1440 bf 9 7 497 1440 bf 9 6 375 1447 bf 9 6 384 1447 bf 9 6 401 1447 bf 9 6 410 1447 bf 9 6 419 1447 bf 9 7 384 1453 bf 9 7 497 1453 bf 8 7 576
1453 bf 9 7 384 1460 bf 8 7 393 1460 bf 9 7 401 1460 bf 9 7 410 1460 bf 9 7 419 1460 bf 9 7 462 1460 bf 8 7 393 1467 bf 9 7 401 1467 bf 9 7 410 1467 bf 9 7 471 1467 bf 8 7 489 1467 bf 8 6 393 1474 bf 9 6 401 1474 bf 9 6 462 1474 bf 9 6 471 1474 bf 9
6 480 1474 bf 9 7 401 1480 bf 9 7 410 1480 bf 9 7 462 1480 bf 9 7 480 1480 bf 9 7 401 1487 bf 9 7 410 1487 bf 9 7 419 1487 bf 9 7 462 1487 bf 9 7 401 1494 bf 9 7 410 1494 bf 9 7 462 1494 bf 9 7 480 1494 bf 9 7 828 1494 bf 9 6 410 1501 bf 8 6 454
1501 bf 9 7 410 1507 bf 9 7 419 1507 bf 9 7 471 1507 bf 9 7 419 1514 bf 8 7 454 1514 bf 9 7 480 1514 bf 9 7 419 1521 bf 8 7 428 1521 bf 9 7 436 1521 bf 9 7 462 1521 bf 9 7 471 1521 bf 8 6 428 1528 bf 8 6 454 1528 bf 9 6 462 1528 bf 8 7 428 1534 bf 9
7 436 1534 bf 9 7 445 1534 bf 8 7 454 1534 bf 9 7 462 1534 bf 8 7 428 1541 bf 9 7 436 1541 bf 9 7 436 1548 bf 9 7 445 1548 bf 8 7 454 1548 bf 9 6 436 1555 bf 9 6 445 1555 bf 9 7 436 1561 bf 9 7 445 1561 bf 8 7 454 1561 bf 9 7 462 1561 bf 9 7 445
1568 bf 8 7 454 1568 bf 9 7 445 1575 bf 8 7 454 1575 bf 8 6 454 1582 bf 8 7 454 1588 bf 9 7 462 1588 bf 9 7 462 1595 bf 9 7 471 1602 bf 9 6 471 1609 bf 9 7 471 1615 bf 9 7 480 1629 bf 8 6 489 1636 bf 8 7 489 1642 bf 8 7 515 1642 bf 8 7 489 1649 bf 1
1 1 c black 132 981 m 870 X s
gsave 1088 844 23 896 C 569.206 903.899 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 1001 m -20 Y s 149 991 m -10 Y s 166 991 m -10 Y s 184 991 m -10 Y s 201 991 m -10 Y s 219 1001 m -20 Y s 236 991 m
-10 Y s 253 991 m -10 Y s 271 991 m -10 Y s 288 991 m -10 Y s 306 1001 m -20 Y s 323 991 m -10 Y s 341 991 m -10 Y s 358 991 m -10 Y s 375 991 m -10 Y s 393 1001 m -20 Y s 410 991 m -10 Y s 428 991 m -10 Y s 445 991 m -10 Y s 462 991 m -10 Y s 480
1001 m -20 Y s 497 991 m -10 Y s 515 991 m -10 Y s 532 991 m -10 Y s 550 991 m -10 Y s 567 1001 m -20 Y s 584 991 m -10 Y s 602 991 m -10 Y s 619 991 m -10 Y s 637 991 m -10 Y s 654 1001 m -20 Y s 671 991 m -10 Y s 689 991 m -10 Y s 706 991 m -10 Y
s 724 991 m -10 Y s 741 1001 m -20 Y s 759 991 m -10 Y s 776 991 m -10 Y s 793 991 m -10 Y s 811 991 m -10 Y s 828 1001 m -20 Y s 846 991 m -10 Y s 863 991 m -10 Y s 880 991 m -10 Y s 898 991 m -10 Y s 915 1001 m -20 Y s 933 991 m -10 Y s 950 991 m
-10 Y s 967 991 m -10 Y s 985 991 m -10 Y s 1002 1001 m -20 Y s
gsave 1088 844 23 896 C 120.672 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 182.146 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 268.665 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 355.185 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 441.704 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 23 896 C 530.5 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 23 896 C 617.019 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (6000) show NC gr
gsave 1088 844 23 896 C 703.539 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (7000) show NC gr
gsave 1088 844 23 896 C 790.058 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (8000) show NC gr
gsave 1088 844 23 896 C 876.577 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (9000) show NC gr
gsave 1088 844 23 896 C 956.266 951.712 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 1656 m 870 X s 132 1636 m 20 Y s 149 1646 m 10 Y s 166 1646 m 10 Y s 184 1646 m 10 Y s 201 1646 m 10 Y s 219 1636 m 20 Y s 236 1646 m 10
Y s 253 1646 m 10 Y s 271 1646 m 10 Y s 288 1646 m 10 Y s 306 1636 m 20 Y s 323 1646 m 10 Y s 341 1646 m 10 Y s 358 1646 m 10 Y s 375 1646 m 10 Y s 393 1636 m 20 Y s 410 1646 m 10 Y s 428 1646 m 10 Y s 445 1646 m 10 Y s 462 1646 m 10 Y s 480 1636 m
20 Y s 497 1646 m 10 Y s 515 1646 m 10 Y s 532 1646 m 10 Y s 550 1646 m 10 Y s 567 1636 m 20 Y s 584 1646 m 10 Y s 602 1646 m 10 Y s 619 1646 m 10 Y s 637 1646 m 10 Y s 654 1636 m 20 Y s 671 1646 m 10 Y s 689 1646 m 10 Y s 706 1646 m 10 Y s 724 1646
m 10 Y s 741 1636 m 20 Y s 759 1646 m 10 Y s 776 1646 m 10 Y s 793 1646 m 10 Y s 811 1646 m 10 Y s 828 1636 m 20 Y s 846 1646 m 10 Y s 863 1646 m 10 Y s 880 1646 m 10 Y s 898 1646 m 10 Y s 915 1636 m 20 Y s 933 1646 m 10 Y s 950 1646 m 10 Y s 967
1646 m 10 Y s 985 1646 m 10 Y s 1002 1636 m 20 Y s 132 981 m 675 Y s
gsave 1088 844 23 896 C 54.6438 1400.25 t 90 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1 \(keV\)) show NC gr 158 981 m -26 X s 145 997 m -13 X s 145 1013 m -13 X s 145 1029 m -13 X s 145 1045 m -13 X s 158 1061 m -26 X s 145 1077 m -13 X
s 145 1093 m -13 X s 145 1109 m -13 X s 145 1125 m -13 X s 158 1142 m -26 X s 145 1158 m -13 X s 145 1174 m -13 X s 145 1190 m -13 X s 145 1206 m -13 X s 158 1222 m -26 X s 145 1238 m -13 X s 145 1254 m -13 X s 145 1270 m -13 X s 145 1286 m -13 X s
158 1302 m -26 X s 145 1318 m -13 X s 145 1334 m -13 X s 145 1350 m -13 X s 145 1366 m -13 X s 158 1383 m -26 X s 145 1399 m -13 X s 145 1415 m -13 X s 145 1431 m -13 X s 145 1447 m -13 X s 158 1463 m -26 X s 145 1479 m -13 X s 145 1495 m -13 X s
145 1511 m -13 X s 145 1527 m -13 X s 158 1543 m -26 X s 145 1559 m -13 X s 145 1575 m -13 X s 145 1591 m -13 X s 145 1608 m -13 X s 158 1624 m -26 X s 158 1624 m -26 X s 145 1640 m -13 X s 145 1656 m -13 X s
gsave 1088 844 23 896 C 107.011 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 72.8584 1049.62 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (500) show NC gr
gsave 1088 844 23 896 C 54.6438 1129.3 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 54.6438 1208.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1500) show NC gr
gsave 1088 844 23 896 C 54.6438 1288.68 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 54.6438 1370.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2500) show NC gr
gsave 1088 844 23 896 C 54.6438 1450.34 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 54.6438 1530.03 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3500) show NC gr
gsave 1088 844 23 896 C 54.6438 1611.99 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr 1002 981 m 675 Y s 976 981 m 26 X s 989 997 m 13 X s 989 1013 m 13 X s 989 1029 m 13 X s 989 1045 m 13 X s 976 1061 m 26 X s 989 1077 m 13 X
s 989 1093 m 13 X s 989 1109 m 13 X s 989 1125 m 13 X s 976 1142 m 26 X s 989 1158 m 13 X s 989 1174 m 13 X s 989 1190 m 13 X s 989 1206 m 13 X s 976 1222 m 26 X s 989 1238 m 13 X s 989 1254 m 13 X s 989 1270 m 13 X s 989 1286 m 13 X s 976 1302 m 26
X s 989 1318 m 13 X s 989 1334 m 13 X s 989 1350 m 13 X s 989 1366 m 13 X s 976 1383 m 26 X s 989 1399 m 13 X s 989 1415 m 13 X s 989 1431 m 13 X s 989 1447 m 13 X s 976 1463 m 26 X s 989 1479 m 13 X s 989 1495 m 13 X s 989 1511 m 13 X s 989 1527 m
13 X s 976 1543 m 26 X s 989 1559 m 13 X s 989 1575 m 13 X s 989 1591 m 13 X s 989 1608 m 13 X s 976 1624 m 26 X s 976 1624 m 26 X s 989 1640 m 13 X s 989 1656 m 13 X s 0.386667 0 1 c 49 34 1008 981 bf 0.2 0 1 c 49 33 1008 1015 bf 0 0.0800001 1 c 49
34 1008 1048 bf 0 0.266667 1 c 49 34 1008 1082 bf 0 0.546666 1 c 49 34 1008 1116 bf 0 0.733333 1 c 49 33 1008 1150 bf 0 1 0.986667 c 49 34 1008 1183 bf 0 1 0.8 c 49 34 1008 1217 bf 0 1 0.52 c 49 34 1008 1251 bf 0 1 0.333333 c 49 33 1008 1285 bf 0 1
0.0533333 c 49 34 1008 1318 bf 0.133333 1 0 c 49 34 1008 1352 bf 0.413333 1 0 c 49 34 1008 1386 bf 0.6 1 0 c 49 33 1008 1420 bf 0.88 1 0 c 49 34 1008 1453 bf 1 0.933333 0 c 49 34 1008 1487 bf 1 0.653333 0 c 49 34 1008 1521 bf 1 0.466667 0 c 49 33
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gsave 1088 844 23 896 C 1061 967.65 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (0) show NC gr
gsave 1088 844 23 896 C 1061 1081.49 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (1000) show NC gr
gsave 1088 844 23 896 C 1061 1195.33 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
gsave 1088 844 23 896 C 1061 1309.17 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (3000) show NC gr
gsave 1088 844 23 896 C 1061 1423.01 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
gsave 1088 844 23 896 C 1061 1536.86 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (5000) show NC gr
gsave 1088 844 23 896 C 1108.81 1678.02 t 0 r /Helvetica-Bold findfont 20.5224 sf 0 0 m (3) show NC gr
gsave 1088 844 23 896 C 1074.66 1659.8 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10) show NC gr
gsave 1088 844 23 896 C 1056.45 1659.8 t 0 r /Symbol findfont 31.9238 sf 0 0 m (<EFBFBD>) show NC gr 1 1 1 c 240 47 34 1689 bf black 34 1689 m 240 X s 274 1689 m 47 Y s 274 1736 m -240 X s 34 1736 m -47 Y s 1 1 1 c black
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1265 981 bl 1 1 1 c 0 0.0800001 1 c 9 7 1265 981 bf 0 0.733333 1 c 9 6 1265 988 bf 0.2 0 1 c 9 7 1265 994 bf 0 0.0800001 1 c 9 7 1274 994 bf 0 1 0.8 c 9 7 1274 1001 bf 0 0.0800001 1 c 9 7 1274 1008 bf 9 7 1283 1008 bf 0.386667 0 1 c 9 7 1814 1008 bf
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bf 0.2 0 1 c 8 7 2067 1062 bf 0 0.0800001 1 c 9 7 2075 1062 bf 0 0.546666 1 c 9 7 2084 1062 bf 0 0.266667 1 c 8 7 2093 1062 bf 0.2 0 1 c 9 7 2101 1062 bf 9 7 2110 1062 bf 0 0.0800001 1 c 8 7 2119 1062 bf 0.386667 0 1 c 9 7 2127 1062 bf 0 1 0.52 c 9
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8 6 2032 1069 bf 0 0.546666 1 c 9 6 2040 1069 bf 9 6 2049 1069 bf 9 6 2058 1069 bf 8 6 2067 1069 bf 0 0.0800001 1 c 9 6 2075 1069 bf 9 6 2084 1069 bf 0 0.266667 1 c 8 6 2093 1069 bf 0 0.0800001 1 c 9 6 2101 1069 bf 9 6 2110 1069 bf 0 0.266667 1 c 8
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bf 0 0.0800001 1 c 8 7 2006 1075 bf 0 0.733333 1 c 9 7 2014 1075 bf 0 1 0.52 c 9 7 2023 1075 bf 0 0.733333 1 c 8 7 2032 1075 bf 0 0.0800001 1 c 9 7 2040 1075 bf 9 7 2049 1075 bf 0 0.546666 1 c 9 7 2058 1075 bf 0 0.0800001 1 c 8 7 2067 1075 bf
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1884 1082 bf 0 0.0800001 1 c 9 7 1892 1082 bf 9 7 1901 1082 bf 8 7 1910 1082 bf 9 7 1918 1082 bf 9 7 1927 1082 bf 0 0.266667 1 c 9 7 1936 1082 bf 0 0.733333 1 c 8 7 1945 1082 bf 9 7 1953 1082 bf 0 1 0.8 c 9 7 1962 1082 bf 0 0.266667 1 c 8 7 1971
1082 bf 0 0.546666 1 c 9 7 1979 1082 bf 9 7 1988 1082 bf 0 0.266667 1 c 9 7 1997 1082 bf 0 0.546666 1 c 8 7 2006 1082 bf 0.2 0 1 c 9 7 2014 1082 bf 0.386667 0 1 c 9 7 2023 1082 bf 0 0.546666 1 c 8 7 2032 1082 bf 0.386667 0 1 c 9 7 2040 1082 bf 9 7
2049 1082 bf 0.2 0 1 c 9 7 2058 1082 bf 8 7 2067 1082 bf 0.386667 0 1 c 9 7 2075 1082 bf 9 7 2084 1082 bf 0 0.0800001 1 c 8 7 2093 1082 bf 0.2 0 1 c 9 7 2110 1082 bf 0.386667 0 1 c 8 7 2119 1082 bf 9 7 2127 1082 bf 0 0.733333 1 c 8 7 1318 1089 bf 0
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615 bf 0.2 0 1 c 9 6 410 622 bf 0.386667 0 1 c 9 7 410 628 bf 9 7 445 682 bf 1 1 1 c black 132 102 m 870 X s
gsave 1088 843 23 18 C 569.206 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 132 122 m -20 Y s 149 112 m -10 Y s 166 112 m -10 Y s 184 112 m -10 Y s 201 112 m -10 Y s 219 122 m -20 Y s 236 112 m -10 Y
s 253 112 m -10 Y s 271 112 m -10 Y s 288 112 m -10 Y s 306 122 m -20 Y s 323 112 m -10 Y s 341 112 m -10 Y s 358 112 m -10 Y s 375 112 m -10 Y s 393 122 m -20 Y s 410 112 m -10 Y s 428 112 m -10 Y s 445 112 m -10 Y s 462 112 m -10 Y s 480 122 m -20
Y s 497 112 m -10 Y s 515 112 m -10 Y s 532 112 m -10 Y s 550 112 m -10 Y s 567 122 m -20 Y s 584 112 m -10 Y s 602 112 m -10 Y s 619 112 m -10 Y s 637 112 m -10 Y s 654 122 m -20 Y s 671 112 m -10 Y s 689 112 m -10 Y s 706 112 m -10 Y s 724 112 m
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m -10 Y s 985 112 m -10 Y s 1002 122 m -20 Y s
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gsave 1088 843 23 18 C 268.665 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (2000) show NC gr
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gsave 1088 843 23 18 C 441.704 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (4000) show NC gr
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gsave 1088 843 23 18 C 956.266 72.8584 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (10000) show NC gr 132 777 m 870 X s 132 757 m 20 Y s 149 767 m 10 Y s 166 767 m 10 Y s 184 767 m 10 Y s 201 767 m 10 Y s 219 757 m 20 Y s 236 767 m 10 Y s 253
767 m 10 Y s 271 767 m 10 Y s 288 767 m 10 Y s 306 757 m 20 Y s 323 767 m 10 Y s 341 767 m 10 Y s 358 767 m 10 Y s 375 767 m 10 Y s 393 757 m 20 Y s 410 767 m 10 Y s 428 767 m 10 Y s 445 767 m 10 Y s 462 767 m 10 Y s 480 757 m 20 Y s 497 767 m 10 Y
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102 m 675 Y s
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214 m -13 X s 145 231 m -13 X s 145 247 m -13 X s 158 263 m -26 X s 145 279 m -13 X s 145 295 m -13 X s 145 311 m -13 X s 145 327 m -13 X s 158 343 m -26 X s 145 359 m -13 X s 145 375 m -13 X s 145 391 m -13 X s 145 407 m -13 X s 158 423 m -26 X s
145 439 m -13 X s 145 455 m -13 X s 145 472 m -13 X s 145 488 m -13 X s 158 504 m -26 X s 145 520 m -13 X s 145 536 m -13 X s 145 552 m -13 X s 145 568 m -13 X s 158 584 m -26 X s 145 600 m -13 X s 145 616 m -13 X s 145 632 m -13 X s 145 648 m -13 X
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214 m 13 X s 989 231 m 13 X s 989 247 m 13 X s 976 263 m 26 X s 989 279 m 13 X s 989 295 m 13 X s 989 311 m 13 X s 989 327 m 13 X s 976 343 m 26 X s 989 359 m 13 X s 989 375 m 13 X s 989 391 m 13 X s 989 407 m 13 X s 976 423 m 26 X s 989 439 m 13 X
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13 X s 989 697 m 13 X s 989 713 m 13 X s 989 729 m 13 X s 976 745 m 26 X s 976 745 m 26 X s 989 761 m 13 X s 989 777 m 13 X s 0.386667 0 1 c 49 34 1008 102 bf 0.2 0 1 c 49 33 1008 136 bf 0 0.0800001 1 c 49 34 1008 169 bf 0 0.266667 1 c 49 34 1008
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gsave 1088 843 23 18 C 1061 521.393 t 0 r /Helvetica-Bold findfont 31.9238 sf 0 0 m (25) show NC gr
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bf 8 6 1588 703 bf 9 7 1605 723 bf 1 1 1 c black 1265 102 m 871 X s
gsave 1088 843 1157 18 C 1703.06 25.0451 t 0 r /Helvetica-Bold findfont 38.7646 sf 0 0 m (EdepSi1+EdepSi2 \(keV\)) show NC gr 1265 122 m -20 Y s 1283 112 m -10 Y s 1300 112 m -10 Y s 1318 112 m -10 Y s 1335 112 m -10 Y s 1352 122 m -20 Y s 1370
112 m -10 Y s 1387 112 m -10 Y s 1405 112 m -10 Y s 1422 112 m -10 Y s 1440 122 m -20 Y s 1457 112 m -10 Y s 1474 112 m -10 Y s 1492 112 m -10 Y s 1509 112 m -10 Y s 1527 122 m -20 Y s 1544 112 m -10 Y s 1561 112 m -10 Y s 1579 112 m -10 Y s 1596
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