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