progress saved stm_study report

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2017-03-31 13:55:39 -04:00
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@@ -191,6 +191,16 @@ bunches, is:
\frac{0.27}{1695\times 10^{-9}} = \SI{159e3}{\Hz} \frac{0.27}{1695\times 10^{-9}} = \SI{159e3}{\Hz}
\end{equation} \end{equation}
\section{Timing of hits on STM detector}
\label{sec:timing_of_hits_on_stm_detector}
\section{Signal to background ratio}
\label{sec:signal_to_background_ratio}
Muonic X-rays and probabilities in the simulation are not correct, see
\cref{sec:muonic_x_rays_in_geant4}.
%%%% Appendices
\appendix \appendix
\section{How to run the simulation and analyze data} \section{How to run the simulation and analyze data}
\label{sec:how_to_run_the_simulation_and_analyze_data} \label{sec:how_to_run_the_simulation_and_analyze_data}
@@ -199,7 +209,6 @@ bunches, is:
\label{sec:muonic_x_rays_in_geant4} \label{sec:muonic_x_rays_in_geant4}
The muonic energy levels and transition probabilities were calculated using The muonic energy levels and transition probabilities were calculated using
a simple model described by Mukhopadhyay~\cite{Mukhopadhyay.1977}. a simple model described by Mukhopadhyay~\cite{Mukhopadhyay.1977}.
\begin{itemize} \begin{itemize}
\item Energy of K-shell electrons are precisely corrected based on \item Energy of K-shell electrons are precisely corrected based on
that of hydrogen atom, taking finite size of the nucleus into account: that of hydrogen atom, taking finite size of the nucleus into account:
@@ -238,9 +247,10 @@ a simple model described by Mukhopadhyay~\cite{Mukhopadhyay.1977}.
firstline=123, firstline=123,
lastline=125]{c++}{listings/G4EmCaptureCascade.cc} lastline=125]{c++}{listings/G4EmCaptureCascade.cc}
\end{mdframed} \end{mdframed}
\end{itemize} \end{itemize}
Above listings are from the Geant4 source file:
\url{source/processes/hadronic/stopping/src/G4EmCaptureCascade.cc}
\bibliographystyle{h-physrev} \bibliographystyle{h-physrev}
\bibliography{stm_study} \bibliography{stm_study}