From 0e33b140eaac835f2ad15003a4c55f2c7bfbccb5 Mon Sep 17 00:00:00 2001
From: Nam Tran <thnam.me@gmail.com>
Date: Fri, 31 Mar 2017 13:55:39 -0400
Subject: [PATCH] progress saved stm_study report

---
 stm_study_201611/stm_study.tex | 16 +++++++++++++---
 1 file changed, 13 insertions(+), 3 deletions(-)

diff --git a/stm_study_201611/stm_study.tex b/stm_study_201611/stm_study.tex
index 3834972..7f0004f 100644
--- a/stm_study_201611/stm_study.tex
+++ b/stm_study_201611/stm_study.tex
@@ -191,6 +191,16 @@ bunches, is:
   \frac{0.27}{1695\times 10^{-9}} = \SI{159e3}{\Hz}
 \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
 \section{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}
 The muonic energy levels and transition probabilities were calculated using
 a simple model described by Mukhopadhyay~\cite{Mukhopadhyay.1977}.
-
 \begin{itemize}
   \item Energy of K-shell electrons are precisely corrected based on
     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,
           lastline=125]{c++}{listings/G4EmCaptureCascade.cc}
       \end{mdframed}
-
-
 \end{itemize}
+Above listings are from the Geant4 source file:
+\url{source/processes/hadronic/stopping/src/G4EmCaptureCascade.cc}
+
 
 \bibliographystyle{h-physrev}
 \bibliography{stm_study}