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diff --git a/Master/texmf-dist/doc/latex/latex-web-companion/ch2/latexexa.aux b/Master/texmf-dist/doc/latex/latex-web-companion/ch2/latexexa.aux new file mode 100644 index 00000000000..7df7d7030da --- /dev/null +++ b/Master/texmf-dist/doc/latex/latex-web-companion/ch2/latexexa.aux @@ -0,0 +1,55 @@ +\relax +\ifx\hyper@anchor\@undefined +\global \let \oldcontentsline\contentsline +\gdef \contentsline#1#2#3#4{\oldcontentsline{#1}{#2}{#3}} +\global \let \oldnewlabel\newlabel +\gdef \newlabel#1#2{\newlabelxx{#1}#2} +\gdef \newlabelxx#1#2#3#4#5#6{\oldnewlabel{#1}{{#2}{#3}}} +\AtEndDocument{\let \contentsline\oldcontentsline +\let \newlabel\oldnewlabel} +\else +\global \let \hyper@last\relax +\fi + +\@writefile{toc}{\contentsline {section}{\numberline {1}Introduction}{1}{section.1}} +\citation{bib-LAND} +\@writefile{toc}{\contentsline {section}{\numberline {2}Landau theory}{2}{section.2}} +\newlabel{sec:phys332-1}{{2}{2}{Landau theory\relax }{section.2}{}} +\@writefile{brf}{\backcite{bib-LAND}{{2}{2}{section.2}}} +\citation{bib-TALM} +\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces The variable $\xi /I_0$ can be used to measure the validity range of the Landau theory. It depends on the type and energy of the particle, $Z$, $A$ and the ionisation potential of the material and the layer thickness. }}{3}{figure.1}} +\newlabel{fg:phys332-1}{{1}{3}{Introduction\relax }{figure.1}{}} +\@writefile{toc}{\contentsline {subsection}{\numberline {2.1}Restrictions}{3}{subsection.2.1}} +\@writefile{brf}{\backcite{bib-TALM}{{3}{2}{Item.4}}} +\citation{bib-VAVI} +\citation{bib-SCH1} +\citation{bib-SELT} +\@writefile{toc}{\contentsline {section}{\numberline {3}Vavilov theory}{5}{section.3}} +\newlabel{vavref}{{3}{5}{Vavilov theory\relax }{section.3}{}} +\@writefile{brf}{\backcite{bib-VAVI}{{5}{3}{section.3}}} +\@writefile{brf}{\backcite{bib-SCH1}{{5}{3}{section.3}}} +\@writefile{toc}{\contentsline {section}{\numberline {4}Gaussian Theory}{5}{section.4}} +\@writefile{brf}{\backcite{bib-SELT}{{5}{4}{section.4}}} +\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Energy loss distribution for a 3 GeV electron in Argon as given by standard \texttt {GEANT}. The width of the layers is given in centimeters.}}{6}{figure.2}} +\newlabel{fg:phys332-2}{{2}{6}{Urb\'an model\relax }{figure.2}{}} +\@writefile{toc}{\contentsline {section}{\numberline {5}Urb\'an model}{6}{section.5}} +\newlabel{urban}{{5}{6}{Urb\'an model\relax }{section.5}{}} +\newlabel{eq:sigex}{{2}{6}{Urb\'an model\relax }{equation.2}{}} +\newlabel{eq:sigion}{{3}{6}{Urb\'an model\relax }{equation.3}{}} +\newlabel{eq:fisum}{{4}{7}{Urb\'an model\relax }{equation.4}{}} +\newlabel{eq:flnsum}{{5}{7}{Urb\'an model\relax }{equation.4}{}} +\@writefile{toc}{\contentsline {subsection}{\numberline {5.1}Fast simulation for $n_3 \geq 16$}{8}{subsection.5.1}} +\newlabel{eq:phys332-5}{{13}{8}{Fast simulation for $n_3 \geq 16$\relax }{equation.13}{}} +\newlabel{eq:phys332-1}{{16}{8}{Fast simulation for $n_3 \geq 16$\relax }{equation.16}{}} +\newlabel{eq:phys332-2}{{17}{8}{Fast simulation for $n_3 \geq 16$\relax }{equation.16}{}} +\newlabel{eq:phys332-3}{{18}{8}{Fast simulation for $n_3 \geq 16$\relax }{equation.18}{}} +\newlabel{eq:phys332-4}{{19}{8}{Fast simulation for $n_3 \geq 16$\relax }{equation.18}{}} +\newlabel{eq:phys332-6}{{22}{9}{Fast simulation for $n_3 \geq 16$\relax }{equation.22}{}} +\newlabel{eq:phys332-7}{{23}{9}{Fast simulation for $n_3 \geq 16$\relax }{equation.22}{}} +\newlabel{eq:phys332-8}{{24}{9}{Fast simulation for $n_3 \geq 16$\relax }{equation.22}{}} +\bibcite{bib-LAND}{1} +\bibcite{bib-SCH1}{2} +\bibcite{bib-SELT}{3} +\bibcite{bib-TALM}{4} +\bibcite{bib-VAVI}{5} +\@writefile{toc}{\contentsline {subsection}{\numberline {5.2}Special sampling for lower part of the spectrum}{10}{subsection.5.2}} |