From cb184869475952517a9a22f7e655253d9a1571cf Mon Sep 17 00:00:00 2001
From: Kamil Sedlak <kamil.sedlak@psi.ch>
Date: Fri, 6 May 2011 15:16:49 +0000
Subject: [PATCH] 6.5.2011  Kamil Sedlak 1) Adding/improving the simulation of
 light signals and APD 2) Many small changes and improvements 3) Adding manual
 to musrSimAna to the svn repository 4) Adding some example files for musrSim

---
 doc/musrSim.pdf                     |   Bin 237450 -> 309649 bytes
 doc/musrSim.tex                     |   181 +-
 doc/musrSimAna.pdf                  |   Bin 0 -> 316209 bytes
 doc/musrSimAna.tex                  |   745 ++
 include/musrRootOutput.hh           |    67 +
 include/musrScintSD.hh              |    19 +-
 musrSimAna/201.v1190                |   160 +
 musrSimAna/201a.v1190               |   158 +
 musrSimAna/musrAnalysis.cxx         |    11 +-
 musrSimAna/musrAnalysis.hh          |     4 +
 musrSimAna/musrTH.cxx               |    12 +-
 musrSimAna/musrTH.hh                |     3 +-
 run/101.mac                         |    95 +-
 run/102.mac                         |    90 +-
 run/110.mac                         |   241 +
 run/APDpulseShapeFile_2011_1e_Z.txt | 10006 ++++++++++++++++++++++++++
 run/visDawn101.mac                  |     2 +-
 run/visDawn102.mac                  |    70 +
 run/vis_201.mac                     |    12 +-
 src/musrDetectorConstruction.cc     |     3 +
 src/musrRootOutput.cc               |   139 +-
 src/musrScintSD.cc                  |    97 +-
 22 files changed, 11942 insertions(+), 173 deletions(-)
 create mode 100644 doc/musrSimAna.pdf
 create mode 100644 doc/musrSimAna.tex
 create mode 100644 musrSimAna/201.v1190
 create mode 100644 musrSimAna/201a.v1190
 create mode 100644 run/110.mac
 create mode 100644 run/APDpulseShapeFile_2011_1e_Z.txt
 create mode 100644 run/visDawn102.mac

diff --git a/doc/musrSim.pdf b/doc/musrSim.pdf
index 915785f1eb9dc2331121cd552de9a9ac07033b51..1067b5a2ab6d0271a8c33a54aed5f65cedbabc34 100644
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diff --git a/doc/musrSim.tex b/doc/musrSim.tex
index 926ae3b..7c4cf9b 100644
--- a/doc/musrSim.tex
+++ b/doc/musrSim.tex
@@ -23,7 +23,7 @@
 %\title{GEANT Simulation Program for the
 %$\mathbf{\mu}$SR Instruments}
 
-\author{Kamil Sedl\'ak$^1$, Toni Shiroka$^1$, Zaher Salman$^1$, Tom Lancaster$^2$, Thomas Prokscha$^1$, Taofiq Paraiso$^1$}
+\author{Kamil Sedl\'ak$^1$, Toni Shiroka$^1$, Zaher Salman$^1$, Jose Rodriguez$^1$, Tom Lancaster$^2$, Thomas Prokscha$^1$, Taofiq Paraiso$^1$}
 
 \address{{$^1$ Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland}\\
 $^2$ Clarendon Laboratory, Department of Physics, Oxford University, Parks Road, Oxford OX1 3PU, UK}
@@ -1292,6 +1292,176 @@ scintillator tiles.}
 illustrates a simple geometry made of an electron source and two blocks
 of scintilator tiles with the dimensions of $3 \times 3 \times 2\,$mm,
 which is defined in the macro file ``101.mac''.
+The primary particles are electrons with the energy of 2.15\,MeV shooted
+into the first scintillator.  There the electron can be scattered, and therefore
+it may or may not hit the second scintillator.  We have used the command\\[2ex]
+{\tt /musr/command storeOnlyEventsWithHitInDetID 11}\\[2ex]
+and therefore only the events, in which there was some energy deposited
+in the second collimator, will be saved into the output Root file.
+
+To run this example, do the following:
+\begin{enumerate}
+\item Change to the directory {\tt musrSim/run/}
+\item If the subdirectory {\tt data} does not exist, create it.
+\item Run your Geant4 initialisation script (typically something like \\
+  {\tt source /home/install/geant4.9.4/env.sh}\\
+  where the path to the {\tt env.sh} script depends on the directory where Geant4 
+  is installed on your computer.
+\item Execute the command {\tt musrSim 101.mac}
+\item The example file {\tt 101.mac} will try to visualise the events using the
+  Dawn graphics program.  To simulate some data (without the visualisation),
+  uncomment the line {\tt /vis/disable}, comment the line 
+  {\tt /control/execute visDawn101.mac} and change number of generated events
+  to e.g.\ 1000  (by command {\tt /run/beamOn 1000}).
+\item Look at the output using Root, e.g.\ by commands \\
+  {\tt \$ root} \\
+  {\tt root [0] TFile* f2=new TFile("data/musr\_101.root") } \\
+  {\tt root [1]  .ls } \\
+  {\tt root [2] t1->Print() } \\
+  {\tt root [3] t1->Draw("det\_edep","det\_ID==10") }  \emph{\small //energy deposited in the first scintillator}\\
+  {\tt root [4] t1->Draw("det\_edep","det\_ID==11") }  \emph{\small //energy deposited in the second scintillator}\\
+  {\tt root [5] t1->Draw("det\_time\_start[0]-det\_time\_start[1]")}  \emph{\small //T.O.F. between the two scint.} \\
+  {\tt root [6] .q}\\
+  Note that the hits in one event are ordered according to the deposited energy, and therefore the
+  first hit sometimes corresponds to the hit in scintillator counter 10, sometimes to the hit in counter 11.
+  Therefore the histogram created by the command {\tt t1->Draw("det\_time\_start[0]-det\_time\_start[1]")}
+  has two peaks -- at a positive and at a negative time.
+\end{enumerate}
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Example 2 -- Sr decay electrons passing through two scintillator tiles (102.mac)}
+This example is very similar to the previous one.  The only difference is that initial
+particles are decay electrons from a $^{90}$Sr source.  Because $^{90}$Sr decays to $^{90}$Y,
+which in turn also decays emitting an electron, we have in fact two decay electrons per event
+(two emission spectra from the strontium source).
+The data for the strontium and yttrium decay are taken
+from the Geant4 data files, namely\\
+{\tt /home/install/data\_geant4.9.4/RadioactiveDecay3.3/z38.a90}~~~~ and\\
+{\tt /home/install/data\_geant4.9.4/RadioactiveDecay3.3/z39.a90}. \\
+There is, however, one problem in musrSim -- it has to handle times with picoseond precission,
+and the \emph{double} precision used in the c{\tt ++} program is then not enough to deal with 
+the $^{90}$Sr decay time of 29 years.  
+For this reason, one has to modify the decay times in the two data files, i.e.\
+in the file {\tt z38.a90}, one should replace the line\\
+\hspace*{1cm}{\tt P~~~~~~~0.0000~~~9.0820e+08}\\ 
+by the line\\
+\hspace*{1cm}{\tt P~~~~~~~0.0000~~~9.0820e-08}\\[2ex]
+and in the file {\tt z39.a90}, one should replace the lines\\
+\hspace*{1cm}{\tt P~~~~~~~0.0000~~~2.3080e+05}\\
+\hspace*{1cm}{\tt P~~~~~682.0300~~~1.1480e+04}\\
+by the lines\\
+\hspace*{1cm}{\tt P~~~~~~~0.0000~~~2.3080e-05}\\
+\hspace*{1cm}{\tt P~~~~~682.0300~~~1.1480e-04}\\
+This way, the decay times are reasonably short, and musrSim can handle them.
+
+Another complication comes from the fact, that the decay electrons are emitted
+isotropically from the Sr source.  In principle, it is possible to restrict the
+emission angles in the GPS (General Particle Source), but we have not done this
+intentionally, because we did not want to exclude events in which the decay electron
+enters a counter after scattering in the air.  In the end only a very small fraction
+of events hits the second counter, and is written out to the output file.  
+(In any case -- the events in which electron does not enter any counter are simulated in a much
+shorter time than the ``interesting'' events.)
+
+The example {\tt 102.mac} is based on the results published in~\cite{kkkkk}.
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Example 3 -- Simulation of the light transport (103.mac)}
+This example is similar to example~1, and extended by the simulation of light (``optical
+photons'').  The light simulation slows down the execution of musrSim dramatically.
+
+The simulation of light is a new feature in musrSim, and it is being tested.  Once
+this is finished, we will improve this example.  However, it seems to be running fine
+in its current implementation, so you can start using it.  A lot of usefull information
+about the optical photons is given in chapter ``Optical Photon Processes'' in
+the Geant4 User Manual~\cite{geantUserManual}.\\
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Example 4 -- GPD instrument (201.mac)}
+%
+The General Purpose Decay-Channel Spectrometer (GPD) 
+instrument~\cite{GPD} at PSI, more or less as implemented in reality in the year 2010, is exemplified in
+run {\tt 201.mac}.  GPD instrument is optimised for the measurements of pressuarised samples 
+in a special pressure cells.
+The detector system is relatively simple -- it consist of a rectangular muon counter (10x10x2\,mm),
+two backward positron counters, three forward positron counters, cylidrical sample in a cylindrical
+sample holder, two lead collimators, one copper collimator, GPD magnet, and some additional ``dead'' material.
+The GPD geometry is illustrated in Fig.~\ref{fig:vis_201_1}-\ref{fig:vis_201_4},
+where some of the elements present in the simulation (beampipe, magnet, aluminium profiles) are not displayed
+for simplicity.
+The most important parameters of the simulation are summarised in table~\ref{dimensions}.
+%
+\begin{figure}[tbp]\centering
+\epsfig{file=pict/vis_201_1.eps,width=0.5\linewidth,%
+bbllx=70pt,bblly=270pt,bburx=455pt,bbury=640pt,clip=}
+\caption{3D view at the GPD detector system (run 201). Blue colour indicates the positron counters,
+magenta stands for collimators, red is the muon counter. GPD magnet, some Aluminium U-profiles and beampipe 
+are not shown in the plot, however they are included in the simulation.}
+\label{fig:vis_201_1}
+\end{figure}
+%
+%
+\begin{figure}[tbp]\centering
+\epsfig{file=pict/vis_201_2.eps,width=0.8\linewidth,%
+bbllx=90pt,bblly=310pt,bburx=450pt,bbury=525pt,clip=}
+\caption{Side view of the GPD detector.}
+\label{fig:vis_201_2}
+\end{figure}
+%
+%
+\begin{figure}[tbp]\centering
+\epsfig{file=pict/vis_201_3.eps,width=0.4\linewidth,%
+bbllx=210pt,bblly=320pt,bburx=380pt,bbury=525pt,clip=}
+\caption{Front view of the GPD detector.}
+\label{fig:vis_201_3}
+\end{figure}
+%
+%
+\begin{figure}[tbp]\centering
+\epsfig{file=pict/vis_201_4.eps,width=0.9\linewidth,%
+bbllx=70pt,bblly=309pt,bburx=485pt,bbury=513pt,clip=}
+\caption{Top view of the GPD detector.}
+\label{fig:vis_201_4}
+\end{figure}
+%
+
+
+\begin{table}[htbp]\centering
+\renewcommand{\arraystretch}{1.05}
+  \begin{tabular}{|l|c|c|}
+    \hline
+    \lower 1mm \hbox{\textbf{Component}}  & \lower 1mm \hbox{\textbf{Dimension}} &  \lower 1mm \hbox{\textbf{Material}} \\[5pt]
+    \hline
+    positron counter scintillator        & $26 \times 90 \times 5$\,mm   & plastic vinyltoluene \\
+    middle forw. positron counter scint. & $14 \times 90 \times 5$\,mm   & plastic vinyltoluene \\
+    muon counter                         & $10 \times 10 \times 2$\,mm   & plastic vinyltoluene \\
+    sample                               & R=3.5\,mm, L=14\,mm           & Cu \\
+    sample cell                          & R=12\,mm, L=100\,mm           & Cu \\
+    Cu collimator                & $80 \times 120 \times (\sim 20 - 30)$\,mm             & Cu  \\
+    Cu collimator opening                & $5 \times 12$\,mm          &    \\
+    Pb collimator                        & $140 \times 140 \times 30$ & Pb \\
+    Pb collimator opening                & $4 \times 10$\,mm          &    \\
+    Collimator 1                         & R=100\,mm, L=30\,mm        & Pb \\
+    Collimator 1 opening                 & R$_{opening}$=8\,mm        &    \\
+    distance sample -- Pb collimator     & 90\,mm (centre -- centre)  &    \\
+    distance sample -- collimator1       & 250\,mm (centre -- centre) &    \\
+    distance sample -- beampipe window   & 600\,mm                    &    \\ \hline
+    muon initial momentum                & $100 \pm 3$\,MeV/c         &    \\
+    muon initial $z$-coordinate          & -1.0\,m with respect to sample &    \\
+    muon initial $x$ and $y$ coordinate  & Gaussian smearing, $\sigma_x=\sigma_y=25$\,mm & \\
+    magnetic field                       & 300 gauss                  &    \\
+    \hline
+  \end{tabular}
+  \caption{Main parameters of the simulation.}
+  \label{dimensions}
+\end{table}
+%
+A non-standard feature of this simulation is the muon momentum, which is $~sim$100\,MeV/c.
+The copper collimator used in GPD has a bit complicate shape, which required to use subtraction
+of logical volumes in Geant\,4.  This operation can not be specified through the macro file,
+and therefore a special kind of volume called {\tt GPDcollimator} has been hard-coded into
+the source code (namely in the routine {\tt musrDetectorConstruction.cc}), and it is
+then activated in the macro file using the command \\[2ex]
+{\tt /musr/command construct GPDcollimator \ldots}\\[2ex]
+%
+The results of this GPD simulation are described in the \emph{musrSimAna} manual~\cite{musrSimAna}.
 
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 
@@ -1332,7 +1502,7 @@ in~\cite{Aktas:2004px}.
 \bibitem{AlexeyTestAPD} A.~Stoykov {\it et al.}, ``First experience with G-APDs in $\mu$SR instrumentation'',
 	NDIP08, to be published in Nucl. Instrum. Meth. A.
 
-\bibitem{geant} S.~Agostinelli, et al., Nucl. Instr. and Meth. A 506 (2003) 250.\\ %-303. \\
+\bibitem{geant} S.~Agostinelli {\it et al.}, Nucl. Instr. and Meth. A 506 (2003) 250.\\ %-303. \\
                 J.~Allison, et al., IEEE Trans. Nucl.\ Sci.\  53 (2006) 270. %-278.
 \bibitem{root} R.~Brun, F.~Rademakers ``ROOT - An Object Oriented Data Analysis Framework'',
 %Proceedings AIHENP'96 Workshop, Lausanne, Sep. 1996, 
@@ -1357,9 +1527,12 @@ A.~Aktas {\it et al.}  [H1 Collaboration],
 Submitted to Eur.\,Phys.\,J.\,{\bf C}, [hep-ex/0401010].
 %%CITATION = HEP-EX 0401010;%%
 
+\bibitem{GPD}
+http://lmu.web.psi.ch/facilities/gpd/gpd.html
 
-
+\bibitem{musrSimAna}
+K.Sedlak, ``Manual of musrSimAna''.
 
 \end{thebibliography}
 
-\end{document}
+\end{document}
\ No newline at end of file
diff --git a/doc/musrSimAna.pdf b/doc/musrSimAna.pdf
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diff --git a/doc/musrSimAna.tex b/doc/musrSimAna.tex
new file mode 100644
index 0000000..5b27c71
--- /dev/null
+++ b/doc/musrSimAna.tex
@@ -0,0 +1,745 @@
+\documentclass[twoside]{dis04}
+\usepackage{epsfig}
+\def\runauthor{PSI}
+\def\shorttitle{musrSimAna}
+\begin{document}
+
+\newcommand{\musr}{\ensuremath{\mu}SR}
+\newcommand{\musrSim}{\emph{musrSim}}
+\newcommand{\musrSimAna}{\emph{musrSimAna}}
+\title{Manual of musrSimAna}
+\author{Kamil Sedl\'ak$^1$}
+
+\address{{$^1$ Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland}}
+
+\maketitle
+
+\abstracts{
+``musrSimAna'' is an analysis program, which helps the user to analyse and interpret the output of the
+``musrSim'' simulation.}
+
+%========================================================================================================
+\section{Introduction}
+\label{introduction}
+The purpose of the \musrSimAna\ program is to analyse the Root tree, the output 
+of the \musrSim\ program.
+In general, the event-by-event information stored in the Root tree can be easily used only for
+a very quick and rough tests -- e.g.\ to see, where the muons stop and decay irrespective
+of whether they were triggered in the M-counter or not, or to have an idea what energy
+spectrum was deposited in a given counter.  Typically, however, one is more interested
+to study \musr\ signal amplitude, time-independent background, or where the muons decay
+only for the ``stopped'' muons (e.g.\ muons triggered by M-counter and not detected
+by a veto counter), or only for triggered muons which actually stopped in a cryostat
+rather than in a sample.  Such a study requires some kind of analysis program, which
+loops over all events stored in the Root tree (output of \musrSim), and implements the
+logic of the required \musr\ experiment.
+
+One way to do such analysis is to start from a Root command {\tt MakeClass(``MyAnalysis'')},
+which creates some sort of skeleton c++ class for the given Root tree.  This allows the user
+to make his/her own and very specific analysis program tailored to his/her needs.  On the other
+hand, it requires special program for each detector set-up.
+
+A second possibility is to use \musrSimAna, which is intended to be a general analysis 
+program for \musr\ instruments. 
+At the moment, however, \musrSimAna\ is tuned to the needs of continuous muon beam facilities.
+Some modifications might be necessary for the pulsed muon beams.
+
+As in the case of \musrSim, the user of \musrSimAna\ specifies all parameters
+required by the analysis in an input text file (steering file).  The initial structure
+of the steering file was taken over from the TDC setup files used by real \musr\ instruments 
+at PSI~\cite{acquisitionProkscha,TDCsetup}.  This setup file defines the ``logic'' of a given experiment,
+namely the coincidences and anti-coincidences of different counters and veto detectors, as well as some
+timing parameters.
+The setup file for the case of simulation had to be extended by the definitions of
+histograms, cuts, fitting, etc.  The description of the setup file will be
+presented in chapter~\ref{howToAnalyse}-\ref{description}, the chapter~\ref{sec:GPD}
+illustrates the whole concept of \musrSimAna\ on the example of an existing \musr\ instrument.
+
+
+
+\section{The main components of the \musrSimAna\ setup file}
+\label{howToAnalyse}
+The parameters for the analysis are stored in the setup file ``{\tt RUNxxx.v1190}'', whose name 
+typically consists of the run number ({\tt RUN}), 
+some further identifier ({\tt xxx}), and ends with ``{\tt .v1190}''. 
+One of the following commands can be used to execute \musrSimAna: \\[1em]
+{\tt
+\$> musrSimAna RUN RUNxxx \\
+\$> musrSimAna RUN RUNxxx nographic > data/RUN.RUNxxx.out
+}\\[1em]
+where the first {\tt RUN} stands for the run number (more precisely, it specifies 
+the \musrSim\ output, which is expected to be stored as ``{\tt data/musr\_RUN.root}'')
+and {\tt RUNxxx} specifies the \musrSimAna\ setup file without the ending, which is
+expected to be stored in the current directory.  The output file of \musrSimAna,
+containing the result histograms, will be stored as ``{\tt data/his\_RUN\_RUNxxx.v1190.root}''.
+
+The syntax of the setup file in \musrSimAna\ is based on the experimental one, 
+defined in~\cite{TDCsetup}.
+At the beginning of this file, some timing parameters are defined:\\[1em]
+\begin{tabular}{ll}
+{\tt RESOLUTION=100 } & \emph{\ldots one TDC bin corresponds to 100\,ps} \\[0.7em]
+{\tt MCOINCIDENCEW=50 } & \emph{\ldots time interval (in TDC bins) to find coincidences with M-counter} \\
+{\tt PCOINCIDENCEW=50 } & \emph{\ldots time interval (in TDC bins) to find coincidences with P-counter} \\
+{\tt VCOINCIDENCEW=100 } & \emph{\ldots time interval (in TDC bins) to find anti-coincidences with M-counter} \\[0.7em]
+{\tt MUONRATEFACTOR=0.089 } & \emph{\ldots will be described in section~\ref{sec:eventMixing}} \\[0.7em]
+{\tt DATAWINDOWMIN=-2.0 } & \emph{\ldots data interval (in $\mu$s) in which positrons are detected} \\
+{\tt DATAWINDOWMAX=10.0 } &  \\[0.7em]
+{\tt PILEUPWINDOWMIN=-10.0 } & \emph{\ldots the pileup interval (in $\mu$s)  for muons} \\
+{\tt PILEUPWINDOWMAX=10.0 } & \\[1em]
+\end{tabular}
+%
+A good event has exactly one hit in the M-counter within the pile-up window, and exactly
+one hit in the positron counters within the data window.  Both windows are defined relative to $t_0$,
+which is the time of the currently analysed M-counter hit.
+
+The coincidence and anti-coincidence logic between the different counters
+(the detector logic) is also specified in the setup file.
+An example may look like this:\\
+\begin{verbatim}
+102; "M up";         M; 0.4;  2005; -401;
+  1; "B1";           P; 0.4;  2005;   21 -401; B1; 1485; 1515; 50995;
+  2; "B2";           P; 0.4;  2005;   22 -401; B2; 1485; 1515; 50995;
+ 11; "F1";           P; 0.4;  2005; -401 -21 -22; F11; 1485; 1515; 50995;
+ 12; "F2";           P; 0.4;  2005; -401 -21 -22; F12; 1485; 1515; 50995;
+ 13; "F3";           P; 0.4;  2005; -401 -21 -22; F13; 1485; 1515; 50995;
+ 21; "Coinc B1"      K; 0.4;  2005;
+ 22; "Coinc B2"      K; 0.4;  2005;
+401; "Active Veto"   V; 0.1;  2005;
+\end{verbatim}
+\mbox{} \\
+%
+In each row, the first number stands for the detector ID (defined in the steering file
+of the \musrSim), the second variable is the name of the counter,
+the third variable identifies the type of the counter (M = muon, P = positron,
+K = coincidence and V = veto counters, respectively), the forth variable is the threshold in MeV applied
+to the energy deposited in the counter, the fifth variable is a time delay (in units
+of bin-width) applied to the given counter, the sixth set of parameters defines
+which other detectors have to be in coincidence (positive ID) or anti-coincidence
+(negative ID) with the given counter, and in the case of positron counters, the
+last four parameters define a special histogram for the given counter. (Note
+that this histogram is used for a compatibility with the experimental steering file, however
+there is a different and more powerful way of how to define histograms, which is 
+defined later). The only difference with respect to the experimental steering
+file is the presence of threshold definition in the fourth column.
+In the example above, the M-counter is the volume which has ID 102 in the simulation,
+and a valid hit has to have energy in the counter above 0.4\,MeV, and no signal
+above 0.1\,MeV in the ``Active Veto'' (ID=401) within a time interval defined by 
+{\tt VCOINCIDENCEW}.  The detailed description of *.v1190 steering files can be found 
+in chapter~\ref{description} and in~\cite{TDCsetup}.
+
+
+
+The main output of the simulation is generated in the form of histograms.
+The histograms are defined in the steering file. For example, the following
+line defines 1-dimensional histogram of the $z$-position of where the muons stop and decay:\\[1em]
+{\tt
+musrTH1D hMuDecayPosZ "Where the muons stop;z[mm];N" 100 -5. 5. muDecayPosZ
+}\\[1em]
+This histogram has 100 bins, spans from -5\,mm to 5\,mm, and the variable filled
+in the histogram is {\tt muDecayPosZ}.
+In fact, this line does not create one histogram, but an array of histograms -- one
+histogram for each ``condition''.  An example of five conditions reads:\\[1em]
+{\tt
+condition 1 oncePerEvent \\
+condition 2 muonDecayedInSample\_gen \\
+condition 4 muonTriggered\_det \\
+condition 6 goodEvent\_det \\
+condition 9 pileupEvent 
+}\\[1em]
+where integer numbers (1,2,4,6 and 9) denote the condition number, and the string at the end
+describes the condition -- e.g.\ ``{\tt muonDecayedInSample\_gen}'' specifies that muon
+has stopped and decayed in the sample, and ``{\tt muonTriggered\_det}'' specifies that
+there had to be a good muon candidate triggered in the M-counter.  
+The ending ``{\tt \_gen}'' indicates that the variable used in the condition 
+was ``generated'', i.e.\ it is known in the simulation, but can not be directly 
+measured experimentally.
+On the other hand the ending ``{\tt \_det}'' specifies that the given condition
+is based on measurable variables, as e.g.\ energy deposits in a counter.
+
+There can be up to
+30 conditions requested, and for each of them a separate histogram will be filled.
+In the output file of \musrSimAna, the histograms corresponding to the previous 
+set of conditions would be saved as
+{\tt hMuDecayPosZ\_1, hMuDecayPosZ\_2, hMuDecayPosZ\_4, hMuDecayPosZ\_6, hMuDecayPosZ\_9}.
+The {\tt hMuDecayPosZ\_1} shows where the muons stop irrespective whether they were
+detected or not. The {\tt hMuDecayPosZ\_6} contains ``good'' muons, i.e.\ muons that would
+be saved in the final histograms in the experiment.  The  {\tt hMuDecayPosZ\_9} shows
+the muons, which contribute to the time-independent background.  Note that there are always
+two muons, $\mu_1$ and $\mu_2$, contributing to the time-independent background, and {\tt hMuDecayPosZ\_9}
+shows the one ($\mu_1$) that started the M-counter. More to this topic is presented
+in chapter~\ref{sec:eventMixing}. Here we just mention that in order 
+to see the $z$-coordinate of the second muon ($\mu_2$),
+which was not triggered by the M-counter but whose decay positron hit the positron counter,
+the histogram {\tt hpileup\_muDecayPosZ\_9} must be used:\\[1em]
+{\tt
+musrTH1D hpileup\_muDecayPosZ "Pileup muons;z[mm];N" 100 -5.0 5. pileup\_muDecayPosZ
+}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Event mixing -- an unavoidable complication}
+\label{sec:eventMixing}
+The output of \musrSim\ is stored in a Root tree named ``{\tt t1}''.  One event corresponds
+to one simulated muon, and it is saved as one row of the tree.  The only information that
+relates one event (muon) to any other one is the variable {\tt timeToNextEvent}, 
+which is a randomly generated time difference between two subsequent events.
+
+The \musrSimAna\ allows one to study the ``time-independent background'', which is
+due to mixing of two different events. A simple example of the event mixing affecting 
+the \musr\ measurement is the following:  the first muon, $\mu_1$, hits the M-counter,
+and subsequently stops and decays in the sample, however the decay positron escapes
+undetected -- most likely because of the limited angular acceptance of positron counters.
+The second muon, $\mu_2$,  arrives around the same time, misses the M-counter, 
+and stops and decays in a collimator wall or elsewhere. 
+Its decay positron hits a positron counter.  Thus there are good-looking muon and positron
+hits,  which however arise from two uncorrelated muons. 
+This fake (background) event is experimentally treated as a good event,
+and contributes to the time-independent background.
+
+Events can be mixed in \musrSimAna, allowing us to study sources of
+the time-independent background.
+%\emph{MusrSimAna} loops over the events and checks whether the conditions defining 
+%the detector logic in the steering file have been fulfilled.  However, to take event
+%mixing properly into account, the conditions have to be veryfied on several subsequent
+%events.  Therefore, at the beginning of the analysis of
+Before analysing  a given event, arrays of hits are filled
+for all counters (M, positron, veto, coincidence counters), which store the hits occurring in the
+future up to the time equal to $ 3\, \cdot $ pileup window or $ 3\, \cdot $ data window,
+whatever is larger\footnote{The data and pile-up windows defined by parameters 
+{\tt DATAWINDOWMIN, DATAWINDOWMAX, PILEUPWINDOWMIN} and {\tt PILEUPWINDOWMAX} 
+are applied later on in the analysis.}. 
+There is one such array for every counter.  After this initial filling,
+there might be several hits in every array, originating from one or more events.
+
+
+The fraction of the time-independent background to good events depends on the incoming muon rate
+measured by the trigger, possibly in the anti-coincidence with a backward veto detector, if
+used in the experiment.  
+Typically, the experimentalists set the incoming muon rate (rate of \emph{stopped muons})
+to $\sim 30\,000\,\mu/s$.  The same should be done in the simulation.
+However, the rate of stopped muons is known only after the analysis is done,
+because, for example, many simulated muons stop and decay in collimators or elsewhere 
+in the beam-pipe without producing any signal in the M-counter.
+Therefore the simulation is normally started with an initial rate of generated muons
+of $30\,000\,\mu/s$, which in practise can correspond to much lower rate of \emph{stopped muons}.
+The rate of stopped muons is calculated at the end of the \musrSimAna\ execution, and
+it is printed out in the \musrSimAna\ output.  The user can use this information and rescale the
+initial muon rate by changing parameter {\tt MUONRATEFACTOR} in the {\tt *.v1190} setup file. 
+This is done without the necessity to re-run the CPU consuming 
+simulation -- only the \musrSimAna\ has to be repeated.  The complete simulation and analysis
+chain therefore usually consists of three steps:
+%
+\begin{enumerate}
+  \item \musrSim\  (takes typically 10 hours).
+  \item \musrSimAna\  with {\tt MUONRATEFACTOR=1.0} (takes typically 10 minutes).
+  \item \musrSimAna\  with {\tt MUONRATEFACTOR} determined in step 2.
+\end{enumerate}
+%
+The {\tt MUONRATEFACTOR} specifies a multiplicative factor applied to
+the variable {\tt timeToNextEvent} 
+(the randomly generated time difference between two subsequent events).
+
+{\bf IMPORTANT NOTE:} In order to get the pile-up effects correctly analysed by \musrSimAna, 
+it is probably necessary to run the \musrSim\ with no event reweighting (i.e.\
+the command ``{\tt /musr/command logicalVolumeToBeReweighted \ldots}'' must {\bf not} be used).
+All events should/have to be (?) saved in the Root tree
+(i.e.\ the command ``{\tt /musr/command storeOnlyEventsWithHits false}'' must be used).
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\section{Detailed list of steering file parameters}
+\label{description}
+\begin{description}
+%   \item{\bf INSTRUMENT=\emph{string}} \\ 
+%         ignored
+%   \item{\bf DESCRIPTION=\emph{string}} \\ 
+%        ignored
+%   \item{\bf TYPE=\emph{string}} \\ 
+%         ignored
+   \item{\bf RESOLUTION=\emph{value}} \\ 
+         width of the TDC bin in picoseconds.
+   \item{\bf MDELAY=\emph{value}} \\ 
+         currently not used (probably not needed in the case of simulation).
+   \item{\bf PDELAY=\emph{value}} \\ 
+         currently not used (probably not needed in the case of simulation).
+   \item{\bf MCOINCIDENCEW=\emph{value}} \\ 
+         time window for the coincidences of the coincidence detectors (``K'')
+         with the M-counter. The \emph{value} is given in TDC bins (see {\tt RESOLUTION} above).
+   \item{\bf PCOINCIDENCEW=\emph{value}} \\ 
+         time window for the coincidences of the coincidence detectors (``K'')
+         with positron counters. The \emph{value} is given in TDC bins.
+   \item{\bf VCOINCIDENCEW=\emph{value}} \\ 
+         time window for the coincidences of the anti-coincidence detectors (``V'')
+         with any other counter. The \emph{value} is given in TDC bins.
+   \item{\bf MUONRATEFACTOR=\emph{value}} \\ 
+         a multiplicative factor which is used to rescale time differences between subsequent muons.
+	 Setting \emph{value} larger than 1 artificially prolongs the time difference between
+	 two subsequently generated muons, and therefore decreases the incoming muon rate 
+         (number of muons per second).  This parameter should be changed in order to set the
+	 incoming muon rate to a given required value, typically to 30\,000\,$\mu/$s.\\
+	 See also variable ``INFINITELYLOWMUONRATE''.
+   \item{\bf INFINITELYLOWMUONRATE} \\ 
+         If INFINITELYLOWMUONRATE is specified, each event is treated independently of any other
+         event.  This corresponds to a situation of infinitely low rate of incoming muons, and
+         no pileup can be observed.  The variable ``MUONRATEFACTOR'' becomes irrelevant when
+	 INFINITELYLOWMUONRATE is specified.
+   \item{\bf DATAWINDOWMIN=\emph{value}} \\ 
+         Beginning of the data interval for the positron counters in $\mu$s.
+   \item{\bf DATAWINDOWMAX=\emph{value}} \\ 
+         End of the data interval for the positron counters in $\mu$s.
+   \item{\bf PILEUPWINDOWMIN=\emph{value}} \\ 
+         Beginning of the pileup interval for the M-counter in $\mu$s.
+   \item{\bf PILEUPWINDOWMAX=\emph{value}} \\ 
+         End of the pileup interval for the M-counter in $\mu$s.
+   \item{\bf MUSRMODE=\emph{string}} \\ 
+         Defines the mode of \musr\ experiment -- presently only ``D'', corresponding to
+	 the time differential mode is implemented.
+   \item{\bf REWINDTIMEBINS=\emph{value}} \\
+         A technical parameter specifying when a roll-over of all hits has to be done.
+	 It is specified in TDC bins, and normally there should be no need to change this parameter.
+   \item{\bf DEBUGEVENT \emph{eventID} \emph{debugLevel}}\\
+         Prints out debug information about the event with the ID \emph{``eventID''}.  
+	 The higher the \emph{debugLevel}, the more details are printed.
+	 (Both \emph{eventID} and \emph{debugLevel} are integers).
+   \item{\bf CLONECHANNEL \emph{ID1} \emph{ID2}}\\
+         Clones the hits detected in counter \emph{ID1} into a new counter \emph{ID2}.
+	 A different (even a lower) threshold can be applied to the cloned counter.
+	 This way the same counter can be used as two independent counters -- e.g.\ once as a veto
+	 detector for the M-counter, and simultaneously as a coincidence detector for
+	 a P-counter.  In both cases the energy threshold and time windows are defined independently.
+   \item{\bf musrTH1D \emph{histoName} \emph{histoTitle} \emph{nBins} \emph{min} \emph{max} \emph{variable} 
+        [{\tt rotreference} $\nu_{\rm RRF}$ $\phi_{\rm RRF}$]} \\
+         Defines a histogram (or more precisely an array of histograms, where the number of histograms
+	 in the array is given by the number of conditions, see section~\ref{howToAnalyse}).
+	 The name of the histogram is defined by \emph{histoName} + the number of the condition.
+	 The string variable \emph{histoTitle} specifies the title of the histogram, 
+	 \emph{nBins}, \emph{min} and \emph{max} stand for the number of bins and minimum and maximum
+	 of the $x$-axis of the histogram.  \\
+	 The optional keyword ``{\tt rotreference}'' signals that the given histogram will be filled in
+	 rotating reference frame (RRF) with the frequency of $\nu_{\rm RRF}$ and a phase shift of $\phi_{\rm RRF}$.
+	 \\
+	 The \emph{variable} stands for the variable that will be
+	 filled into the histogram.  The \emph{variable} can be any variable from the output Root tree
+	 of musrSim (see ``Manual of musrSim'') (except for the array variables like 
+	 {\tt det\_*[], save*[], odet\_*[]}). In addition, it can be also one of the following:
+	 \begin{description}
+	   \item[muDecayPosR]         \ldots $\sqrt{ {\rm muDecayPosX}^2 + {\rm muDecayPosY}^2}$.
+	   \item[wght]                \ldots weight of the event.
+	   \item[det\_m0edep]         \ldots energy deposited in the M-counter that gives the muon signal.
+	   \item[det\_posEdep]        \ldots energy deposited in the P-counter that gives the positron signal.
+	   \item[pos\_Momentum]       \ldots magnitude of the momentum of the decay positron (``generated'', not measurable variable).
+	   \item[pos\_Trans\_Momentum] \ldots transverse momentum of the decay positron.
+	   \item[pos\_Radius]         \ldots positron radius calculated from the decay positron momentum and magnetic 
+                                             field at the point of decay.
+	   \item[pos\_Theta]          \ldots polar angle of the decay positron.
+	   \item[pos\_Phi]            \ldots azimuth angle of the decay positron.
+	   \item[det\_time10]         \ldots time difference between the positron and muon counters 
+	                                     (measured by the respective counters).
+	   \item[gen\_time10]         \ldots the time difference between the muon decay and the first muon hit 
+	                                     in the M-counter (i.e.\ {\tt muDecayTime - muM0Time}).
+	   \item[det\_time10\_MINUS\_gen\_time10] \ldots {\tt det\_time10 - gen\_time10} in picoseconds.
+	   \item[det\_time20]          \ldots very similar to {\tt det\_time10}, however taking into
+	                               account ``counter phase shift'' defined by {\tt counterPhaseShifts}
+				       variable.  This gives the user a possibility to sum up backward and
+				       forward histograms into one histogram (this of course make sense
+				       only in the simulation, where there is ``no physics'' happening 
+				       in the sample, just the muon spin rotation).
+	   \item[pileup\_eventID]      \ldots eventID of the $\mu_2$, where $\mu_2$ stands for the muon, 
+	                              which did not give signal in the M-counter, but whose
+				      decay positron gave signal in the positron counter around the time 
+				      when a different muon ($\mu_1$) triggered the M-counter.
+	   \item[pileup\_muDecayDetID] \ldots detector ID, in which $\mu_2$ stopped and decayed. 
+	   \item[pileup\_muDecayPosZ]  \ldots $z$-coordinate of where the $\mu_2$ stopped and decayed.
+	   \item[pileup\_muDecayPosR]  \ldots radius of where the $\mu_2$ stopped and decayed.
+	 \end{description}
+	 Variables are usually set to -1000 if they can not be calculated (e.g.\ {\tt det\_posEdep} = -1000 
+	 if there was no hit in any positron counter).
+   \item{\bf musrTH2D \emph{histoName} \emph{histoTitle} \emph{nBins} \emph{min} \emph{max} \emph{nBins2} \emph{min2} \emph{max2} \emph{variable}} \\
+     Similar to \emph{musrTH1D}, but for a 2-D histogram.
+   \item{\bf humanDecayHistograms \emph{hist\_decay\_detID} \emph{hist\_decay\_detID\_pileup}  \emph{id$_1$} \emph{name$_1$} \ldots \emph{id$_n$} \emph{name$_n$} } \\
+     This is a special kind of histogram, which converts two histograms 
+     (\emph{hist\_decay\_detID} \emph{hist\_decay\_detID\_pileup})
+     into a human-friendly histograms, where detector ID on the $x$-axis is converted into a string label.
+     The \emph{id$_i$} is the detector id, and the \emph{name$_i$} is the corresponding label name.
+     If \emph{name$_i$ = name$_j$}, the corresponding bins of the original histograms will 
+     be summed up together into the same bin.
+     The \emph{hist\_decay\_detID} and \emph{hist\_decay\_detID\_pileup} have to be defined before
+     (by the command {\tt musrTH1D}).
+   \item{\bf condition \emph{conditionID} \emph{conditionName}} \\
+     Definition of a condition, which is then used when filling histograms.  The \emph{conditionID} 
+     specifies the number of the condition, and must be between 0 and 30 (0 and 30 are also possible).  
+     The \emph{conditionName} is one of the following:
+     \begin{description}
+        \item[alwaysTrue]              \ldots  true for every hit in the m-counter (there can be more than one M-counter hit per event).
+	\item[oncePerEvent]            \ldots  true once for every event (the first hit in M-counter, if any, is considered). 
+	\item[muonDecayedInSample\_gen] \ldots  true if muon stopped and decayed in the sample.
+	\item[muonTriggered\_gen]       \ldots  true if muon passed through the M-counter (irrespective of the deposited energy) 
+	                                       -- not a measurable variable.
+	\item[muonTriggered\_det]       \ldots  true if a good muon candidate was found in the M-counter (using coincidences, vetoes, ...).
+	                                       Double hits within the pileup window are excluded.
+	\item[positronHit\_det]         \ldots  true if a good positron candidate was found in the positron counter.  
+	                                       Double hits within the data window are excluded.
+	\item[goodEvent\_det]           \ldots  true if {\tt muonTriggered\_det} and {\tt positronHit\_det}.
+	\item[goodEvent\_gen]           \ldots  true if muon passed through the M-counter, and the muon stopped anywhere 
+	                                       (i.e.\ did not leave the World volume of the simulation).  No requirement
+	                                       on the positron is implied, i.e.\ the positron may or may not be detected.
+					       Not a measurable variable.
+	\item[goodEvent\_det\_AND\_goodEvent\_gen] 
+	\item[pileupEventCandidate]    \ldots  M-counter hit and positron counter hit both come from two different events.
+	\item[pileupEvent]             \ldots  {\tt pileupEventCandidate} and {\tt goodEvent\_det}.
+	\item[goodEvent\_det\_AND\_muonDecayedInSample\_gen] 
+	\item[goodEvent\_F\_det]         \ldots  {\tt goodEvent\_det}, where the positron was detected in the forward detectors
+	                                       defined by the command {\tt counterGrouping}.
+	\item[goodEvent\_B\_det]         \ldots  like {\tt goodEvent\_F\_det} but for backward positron counters.
+	\item[goodEvent\_U\_det]         \ldots  like {\tt goodEvent\_F\_det} but for upper    positron counters.
+	\item[goodEvent\_D\_det]         \ldots  like {\tt goodEvent\_F\_det} but for lower    positron counters.
+	\item[goodEvent\_L\_det]         \ldots  like {\tt goodEvent\_F\_det} but for left     positron counters.
+	\item[goodEvent\_R\_det]         \ldots  like {\tt goodEvent\_F\_det} but for right    positron counters.
+	\item[goodEvent\_F\_det\_AND\_pileupEvent] \ldots {\tt goodEvent\_F\_det} and {\tt pileupEvent}.
+	\item[goodEvent\_B\_det\_AND\_pileupEvent] \ldots {\tt goodEvent\_B\_det} and {\tt pileupEvent}.
+	\item[goodEvent\_U\_det\_AND\_pileupEvent] \ldots {\tt goodEvent\_U\_det} and {\tt pileupEvent}.
+	\item[goodEvent\_D\_det\_AND\_pileupEvent] \ldots {\tt goodEvent\_D\_det} and {\tt pileupEvent}.
+	\item[goodEvent\_L\_det\_AND\_pileupEvent] \ldots {\tt goodEvent\_L\_det} and {\tt pileupEvent}.
+	\item[goodEvent\_R\_det\_AND\_pileupEvent] \ldots {\tt goodEvent\_R\_det} and {\tt pileupEvent}.
+     \end{description}
+     Additional conditions may be implemented on request.
+  \item{\bf draw \emph{histogramName} \emph{conditionID} } \\
+    Plot histogram (for a given condition)  at the end of the analysis. Note that all histograms
+    are saved into the output file irrespective whether they are plotted or not.
+   \item{\bf  counterPhaseShifts \emph{ID$_1$} \emph{$\phi_1$} \emph{ID$_2$} \emph{$\phi_2$} \ldots \emph{ID$_n$} \emph{$\phi_n$} }\\
+     Defines relative phase shifts of signal between different positron counters, which is used
+     for calculation variable {\tt det\_time20}. \emph{ID$_i$} is the ID number of the positron counter,
+     \emph{$\phi_i$} is its phase shift.  This gives the user a possibility to sum up backward and
+     forward histograms into one histogram.
+   \item{\bf  counterGrouping \emph{group} \emph{ID$_1$ ID$_2$ \ldots ID$_n$} } \\
+     This defines a group of detectors, where \emph{group} stands for ``B'' (backward), 
+     ``F'' (forward), ``U'' (up), ``D'' (down), ``L'' (left) and ``R'' (right) detectors.
+     This grouping is used in the definition of some conditions.
+   \item{\bf  setSpecialAnticoincidenceTimeWindow  \emph{detectorID}  \emph{timeMin}  \emph{timeMax} \emph{unit}} \\
+     This command sets a special anti-coincidence time window for a detector \emph{detectorID}.
+     Normally, the anti-coincidence time window is defined by {\tt VCOINCIDENCEW}, and is the same for all anti-coincidence
+     detectors.  However, sometimes it might be interesting to set the anti-coincidence time window
+     differently for a specific detector (e.g.\ one might test an anti-coincidence of a veto detector with 
+     the M-counter for the whole pile-up time window of $\sim$\,10\,$\mu s$. 
+     Unlike in the case of {\tt VCOINCIDENCEW}, here the \emph{units} are not TDC bins, but
+     rather time in ``nanosecond'' or ``microsecond''.
+   \item{\bf  fit  \emph{histogramName}  \emph{function}  \emph{min}  \emph{max} \emph{p$_1$} \ldots \emph{p$_n$}}  \\
+     Fits the histogram by a given function, where \emph{min}, \emph{max} define the range of the fit
+     on the $x$-axis of the histogram, and \emph{p$_1$} \ldots \emph{p$_n$} are (typically, with some exceptions) 
+     the initial values of the function parameters.  The following functions are currently predefined:
+     \begin{description}
+       \item[pol0]    $=p_0$ \ldots  a constant (1 parameter) - typically used to fit background.
+       \item[simpleExpoPLUSconst] $=p_0 \exp(-x/2.19703)+p_1$
+       \item[rotFrameTime20] $= p_2 \cos(p_0 x+p_1)$
+       \item[funct1]  $=p_3 \exp((p_4 - x)/2.19703) \cdot (1+p_2 \cos(p_0 x+p_1))$
+       \item[funct2]  $=p_3 \exp((p_4 - x)/2.19703) \cdot (1+p_2 \cos(p_0 x+p_1)) + p_5$
+ %      \item[funct3]  the same as {\tt funct2}
+       \item[funct4]  $=p_3 \exp((- x)/2.19703) \cdot (1+p_2 \cos(p_0 x+p_1)) + p_4$
+     \end{description}
+
+\end{description}
+%========================================================================================================
+\section{A real-life example: GPD instrument}
+\label{sec:GPD}
+The simulation of the General Purpose Decay-Channel Spectrometer (GPD) 
+instrument~\cite{GPD} installed at PSI has been exemplified 
+in the \musrSim\ manual~\cite{musrSim}.
+Here we analyse the output of this simulation using \musrSimAna.
+The run number of this simulation is 201, therefore the steering
+file names are ``{\tt 201.mac}'' for \musrSim, and  ``{\tt 201.v1190}'' for
+\musrSimAna, respectively, and the output file name of \musrSim\ is saved as
+``{\tt data/musr\_201.root}''.
+The detector system is very simple with only six counters -- M-counter,
+two backward positron counters and three forward positron counters.
+The reader is strongly recommended to see the illustration of the GPD
+geometry in the \musrSim\ manual~\cite{musrSim}.
+
+8\,000\,000 of events were simulated
+(i.e.\ 8\,000\,000 of muons were generated 100\,cm in front of
+the GPD sample). 
+In only 949\,759 events (11.9\% out of the 8 million) there was a signal detected
+in one or more counters.  The remaining muons stopped somewhere (most
+often in collimator, as we will see later), decayed, and the decay positron
+(and any other particles created thereof) missed the counters.
+This is illustrated in more details in Fig.~\ref{det_n},
+%
+\begin{figure}[tbp]\centering
+\epsfig{file=pict/det_n_infititely_low_muon_rate.eps,width=0.8\linewidth,clip=}
+\caption{Number of hits in all counters per event, assuming infinitely low incoming muon
+rate. The same detector may be hit more than once (e.g.\ if both the muon and its decay 
+positron pass through the M-counter).}
+\label{det_n}
+\end{figure}
+%
+where number of detector hit per event, assuming infinitely low incoming muon
+rate, is shown.  This plot was created in Root by executing:\\[1em]
+{\tt 
+root [0] TFile* ff=new TFile("data/musr\_201.root") \\
+root [1] t1->Print() \\
+root [2] t1->Print("det\_n","det\_n>0") \\
+}\\[1em]
+%
+It has to be pointed out, that the ratio of muons passing through the opening
+in collimators to the number of all generated muons strongly depends on the
+beam properties -- beam profile, beam convergence, etc.  Typically, if we have
+too broad muon beam, we simulate
+many ``useless'' events.  However, the other extreme (simulating too narrow
+beam) can lead to underestimating the time-independent background.
+
+It took approximately 12 hours of the CPU (on PC bought in 2010, where 1 out 
+of 4 processor cores was running) to simulate these 8\,000\,000 events.
+Assuming the 30\,000\,$\mu/$s trigger rate, this corresponds to 26 seconds
+of real experimental running.
+
+\subsection{Where the muons stop and decay}
+\label{sect_muons}
+The positions, or more precisely the components of the GPD instrument, where the muons 
+stop and decay, are shown in Fig.~\ref{humanDecayHistograms_1}:
+%
+\begin{figure}[tbp]\centering
+\epsfig{file=pict/Plot201_1.eps,width=0.9\linewidth,%
+%%bbllx=83pt,bblly=330pt,bburx=538pt,bbury=513pt,clip=}
+clip=}
+\caption{This plot indicates, where the muons stopped and decayed. 
+The dashed histogram shows all generated muons. The full-line histograms show
+where stopped the muons, for which either the muon itself or its secondary
+particle ($e^+, \gamma$) triggered the M-counter:  black histogram stands for
+all such muons, corresponding to infinitely low incoming muon rate, while
+the red histogram stands for the incoming muon rate of 30\,000\,$\mu/$s.
+8\,000\,000 of events were simulated.}
+\label{humanDecayHistograms_1}
+\end{figure}
+%
+%Notes to Fig.~\ref{humanDecayHistograms_1}:
+\begin{itemize}
+  \item Figure~\ref{humanDecayHistograms_1} was generated by Root macro file ``Plot201.C''.
+  \item The labels on the $x$-axis are defined in the file {\tt 201.v1190} by the
+	command \\ 
+	{\tt humanDecayHistograms \ldots}
+  \item The dashed-line histogram in  Fig.~\ref{humanDecayHistograms_1} 
+        shows where the muons stopped and decayed if no preselection
+	criteria are applied on the muons, i.e.\ if all generated muons are considered.
+        This is histogram ``{\tt humanDecayHistograms\_1}''.
+  \item The full-line histograms show
+        where stopped the muons, for which either the muon itself or its secondary
+	particle ($e^+, \gamma$) triggered the M-counter:  black histogram stands for
+	all such muons, corresponding to infinitely low incoming muon rate, while
+	the red histogram represents the case for the 30\,000\,$\mu/$s incoming muon rate.
+	An energy deposit of at least 0.4\,MeV in the M-counter is required to fire the trigger.
+	The number of triggered events decreases with the incoming muon rate,
+	because some of the events are rejected due to the 10\,$\mu$s pileup gate.
+
+        The histogram name is in both cases ``{\tt humanDecayHistograms\_4}'',
+	where the black histogram was calculated using the setup file ``{\tt 201a.v1190}''
+	with the keyword {\tt INFINITELYLOWMUONRATE}, while the red histogram
+	was calculated using the setup file ``{\tt 201.v1190}''
+	with {\tt MUONRATEFACTOR=0.0965819}.
+  \item The $\pm 10\,\mu$s pile-up gate at the incoming muon rate of 30\,000$\,\mu/$s 
+        rejects approx.\ 45\% of the triggered events.  This number can be calulated
+	in Root as the ratio of the ``{\tt Integral}'' of the red and black histograms
+	in Fig.~\ref{humanDecayHistograms_1}:\\[1em]
+	{\tt \small
+	  root [0] TFile* file1 = new TFile("data/his\_201\_201a.v1190.root") \\
+	  root [1] humanDecayHistograms\_4->Integral() \\
+	  root [0] TFile* file2 = new TFile("data/his\_201\_201.v1190.root") \\
+	  root [1] humanDecayHistograms\_4->Integral() \\
+	}
+  \item The muon sample fraction (ratio of muons stopped in the sample over all muons that fired
+        the trigger) for the triggered events (full-line histograms) 
+	is 65\%, and it is practically the same
+	for both infinitely low and 30\,000\,$\mu/$s incoming rate.
+	This number can be obtained in Root by dividing the first column of histogram 
+	{\tt humanDecayHistograms\_4} by the sum of all entries in this histogram:\\[1em]
+	{\tt \small
+	  root [0] TFile* file = new TFile("data/his\_201\_201.v1190.root") \\
+	  root [1] (humanDecayHistograms\_4->GetBinContent(1))/(humanDecayHistograms\_4->Integral()) \\
+	}
+  \item The largest fraction of generated muons (dashed-line histogram) stopped in collimators.
+        Only a small fraction of them caused a hit in the M-counter (full-line histograms).
+  \item Despite the high initial muon momentum of $100 \pm 3\,$GeV/c, muons are 
+        significantly scattered in the last 50\,cm region of air.  This can be
+	clearly seen if the magnetic field is off and a point-like muon beam
+	is used (which can be done by modifying the {\tt 201.mac} file)
+	-- only 77\% of the muons stop in the sample cell or in the sample, while the
+	remaining 23\% of the mouns are scattered so much in the air, that they
+	end up in collimators or elsewhere (not shown here).
+  \item ``World'' in the histogram label means that the muon decayed in the beampipe vacuum 
+        or somewhere else in the air (on the fly). 
+  \item ``Escaped'' means that the muon left the simulated instrument (more precisely the 
+        ``world'' volume) prior its decay.
+\end{itemize}
+
+
+Figure~\ref{humanDecayHistograms_9} shows the ``pile-up events''.
+%
+\begin{figure}[htbp]\centering
+\epsfig{file=pict/Plot201_2_new.eps,width=0.9\linewidth,%
+%%bbllx=83pt,bblly=330pt,bburx=538pt,bbury=513pt,clip=}
+clip=}
+\caption{Pile-up events, i.e.\ the events in which one muon ($\mu_1$) fired the
+trigger, while the hit in a positron counter is due to a decay positron from 
+a different muon ($\mu_2$).  Pile-up events look like a good events, and contribute
+to the time-independent background.}
+\label{humanDecayHistograms_9}
+\end{figure}
+%
+These are events, in which one muon ($\mu_1$) is triggered by the m-counter, 
+while a positron from a different muon ($\mu_2$) was detected by 
+a positron counter\footnote{In fact, the trigger may also be triggered by
+the decay positron of $\mu_1$ and/or a positron counter may detect
+directly $\mu_2$, not its decay positron. Such cases are rare, but they 
+are implicitly included in the simulation.}.
+In addition to this requirement, the decay positron of $\mu_1$ must
+escape undetected (e.g.\ it must miss positron counters) and $\mu_2$ must not trigger the m-counter
+-- otherwise the event would be rejected.
+Pile-up events are the source of the time independent background.
+Usually $\mu_1$ is a good-looking muon that stops in the sample or in the sample cell
+(red histogram in Fig.~\ref{humanDecayHistograms_9}), while $\mu_2$ stops and decays at different places,
+mainly in the collimators (green histogram in Fig.~\ref{humanDecayHistograms_9}).
+
+A nice visualisation of where the background-contributing muons $\mu_2$ stop and decay
+is presented in Fig.~\ref{Pileup_muon_decay_map} (histogram ``{\tt hMuDecayMappileup\_9}'').
+%
+\begin{figure}[htbp]\centering
+\epsfig{file=pict/Pileup_muon_decay_map.eps,width=0.7\linewidth,%
+%%bbllx=83pt,bblly=330pt,bburx=538pt,bbury=513pt,clip=}
+clip=}
+\caption{Positions of where the $\mu_2$ stop and decay.}
+\label{Pileup_muon_decay_map}
+\end{figure}
+%
+In this two dimensional histogram, different components of the GPD instrument, 
+like the lead collimator, the copper collimator and the sample cell, can be recognised.
+The lead collimator is located at the $z$-position between -115\,mm and -85\,mm.
+Due to the high initial muon momentum of $\sim 100\,$MeV/c,
+the maximum of muons in Fig.~\ref{Pileup_muon_decay_map} stop quite deep in the
+lead collimator, at around $z=-103$\,mm.  This might be a little bit surprising to the
+\musr\ scientists who are used to work with the surface muons with momentum of 28\,MeV/c.
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\subsection{The $\mu$SR signal}
+%
+Figure~\ref{hdet_time10_10}
+%
+\begin{figure}[htbp]\centering
+\epsfig{file=pict/hdet_time10_10.eps,width=0.495\linewidth,%
+bbllx=13pt,bblly=5pt,bburx=520pt,bbury=351pt,clip=}
+\epsfig{file=pict/hdet_time10_11.eps,width=0.495\linewidth,%
+bbllx=13pt,bblly=5pt,bburx=520pt,bbury=351pt,clip=}
+%%clip=}
+\caption{MuSR signal for the run 201 (TF$=300\,$gauss). The tree forward positron counters 
+are summed up in the left histogram, and the two backward counters in the right histogram.}
+\label{hdet_time10_10}
+\end{figure}
+%
+shows the $\mu$SR spectra for the same run, 
+i.e.\ for the transverse field of 300\,gauss, integrated over the three forward positron
+counters (left histogram called {\tt hdet\_time10\_10}) 
+and over the two backward positron counters (right histogram called {\tt hdet\_time10\_11}).
+Zero on the time axis corresponds to $t_0$, i.e.\ time of the m-counter hit.
+One can see a prompt peak at $t_0$, time independent background at negative times
+and an oscillating signal at positive times.
+The following function has been fitted to the oscillating part of the signal:
+%
+\begin{equation}
+f=p_3 \cdot e^{-t/2.19703} \cdot (1+p_2 \cdot \cos(t \cdot p_0+p_1))+p_4
+\label{eq_simple}
+\end{equation}
+The fits were restricted to the time interval of $(t_0+0.05 \mu\rm{s},t_0+9.95\mu\rm{s})$,
+and the parameter $p_0$ was fixed (e.g. not fitted).
+The fitted amplitude of asymmetry are $p_2 = 0.307 \pm 0.009$ and 
+$p_2 = 0.290 \pm 0.009$ for the forward and backward counters respectively.
+
+Parts of the spectra from Fig.~\ref{hdet_time10_10} are shown 
+in detail in Fig.~\ref{hdet_time10_10_detail}.
+%
+\begin{figure}[htbp]\centering
+\epsfig{file=pict/hdet_time10_10_detail.eps,width=0.495\linewidth,%
+bbllx=13pt,bblly=5pt,bburx=520pt,bbury=351pt,clip=}
+\epsfig{file=pict/hdet_time10_11_pileup.eps,width=0.495\linewidth,%
+bbllx=13pt,bblly=5pt,bburx=520pt,bbury=351pt,clip=}
+%%clip=}
+\caption{MuSR signal for the run 201 (TF$=300\,$gauss) -- details of
+Fig.~\ref{hdet_time10_10}. The left plot shows the signal in the forward counters around $t_0$,
+the right plot shows the (time-independent background) signal at negative times in the
+backward counters.}
+\label{hdet_time10_10_detail}
+\end{figure}
+%
+The left plot in Fig.~\ref{hdet_time10_10_detail} shows the signal 
+in the forward counters around $t_0$, the right plot shows the 
+(time-independent background) signal at negative times in the backward counters.
+
+An important characteristic of a \musr\ instrument is the time-independent 
+background.  It is usually expressed as
+%
+\begin{equation}
+{\rm Bgr} = p_{-} / p_3 ~~~,
+\label{eq_background}
+\end{equation}
+%
+where $p_{-}$ is the fit to the time-independent background, i.e.\ signal at negative times, 
+and $p_3$ is the parameter from eq.(\ref{eq_simple}), which specifies what the
+size of the signal would be at $t_0$ in the absence of oscillations.
+In the case of backward counters ${\rm Bgr}_{\rm backw} = 14.47/262 = 5.5\,\%$,
+in the case of forward counters ${\rm Bgr}_{\rm forw} = 6.88/267.9 = 2.6\,\%$.
+
+Note that the histogram on right hand side of Fig.~\ref{hdet_time10_10_detail}
+is labelled ``{\tt hdet\_time10\_Bgr\_11}'', not ``{\tt hdet\_time10\_11}''.
+In fact, the two histograms are identical, as one can see in the setup file
+{\tt 201.v1190}.  The only difference is in the fitting -- the same data stored in
+both histograms are fitted by different functions in different time ranges.
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\subsection{The $\mu$SR signal from individual counters}
+%
+Figure~\ref{F11} shows the observed signal in the
+forward counter\ No.~11 (FW11).
+%
+\begin{figure}[htbp]\centering
+\epsfig{file=pict/F11_rebinned.eps,width=0.495\linewidth,%
+bbllx=13pt,bblly=5pt,bburx=520pt,bbury=351pt,clip=}
+\epsfig{file=pict/F11_B11_prompt_peak_thicker.eps,width=0.495\linewidth,%
+bbllx=13pt,bblly=5pt,bburx=520pt,bbury=351pt,clip=}
+\caption{\musr\ signal in the forward positron counter\ No.~11 (run 201, TF$=300\,$gauss).
+The left plot shows the (rebinned) signal in the counter,
+the right plot shows the detail of the \emph{prompt peak}, i.e.\ the region 
+around $t_0$ in the same counter (black line), 
+compared with the prompt peak in the backward positron counter\ No.~1 (magenta line).}
+\label{F11}
+\end{figure}
+%
+Originally, the histogram F11 was defined with the bin width of 100\,ps.
+The number of bins was 50995, covering the time interval of approx.\ (-0.2\,$\mu$s, 4.9\,$\mu$s).
+In the left hand side plot, however, the histogram was rebinned 
+(200 bins were summed up into 1 bin).
+The right hand side plot shows the detail of the \emph{prompt peak}, i.e.\ the region 
+around $t_0$, of one forward and one backward positron counters, prior to the rebinning.  
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\subsection{Conclusion of the GPD analysis example}
+%
+The purpose of the example analysis of the GPD simulation was to illustrate
+the potential of \musrSim\ and \musrSimAna\ programs to investigate features
+like time-independent background, sample muon fraction, prompt peak, \ldots
+This information can be used in design and optimisation of \musr\ instruments.
+
+%========================================================================================================
+\begin{thebibliography}{0}
+
+\bibitem{acquisitionProkscha}  T.~Prokscha {\it et al.} ``A novel VME based \musr\ data acquisition system at PSI'',
+Physica {\bf B~404}, (2009) 1007-1009.
+
+\bibitem{TDCsetup} ``TDC Manual -- Setting up the required logic'', 
+http://lmu.web.psi.ch/facilities/electronics/TDC/set\_logic.html
+
+\bibitem{GPD}
+http://lmu.web.psi.ch/facilities/gpd/gpd.html
+
+\bibitem{musrSim}
+K.Sedlak {\it et al.}, ``Manual of musrSim''.
+
+
+\end{thebibliography}
+
+\end{document}
diff --git a/include/musrRootOutput.hh b/include/musrRootOutput.hh
index 4fd8bc0..84e2642 100644
--- a/include/musrRootOutput.hh
+++ b/include/musrRootOutput.hh
@@ -82,6 +82,7 @@ class musrRootOutput  {
     void SetOPSAinfo    (G4int nDetectors, G4int ID, G4int nPhot, G4double timeFirst, G4double timeA, 
 			 G4double timeB, G4double timeC, G4double timeD, G4double timeMean, G4double timeLast, 
 			 G4double timeCFD, G4double amplCFD);
+    void SetCFDSpecialInfo (G4int n, G4double time);
 
     void SetSaveDetectorInfo (G4int ID, G4int particleID, G4double ke, G4double x, G4double y, G4double z, G4double time, 
 			      G4double px, G4double py, G4double pz, G4double polx, G4double poly, G4double polz) ;
@@ -225,6 +226,7 @@ class musrRootOutput  {
     static G4bool store_odet_timeLast;
     static G4bool store_odet_timeCFD;
     static G4bool store_odet_amplCFD;
+    static G4bool store_odet_timeCFDarray;
 
     static G4int oldEventNumberInG4EqEMFieldWithSpinFunction;
 
@@ -333,6 +335,71 @@ class musrRootOutput  {
     G4double odet_timeLast[odet_nMax];
     G4double odet_timeCFD[odet_nMax];
     G4double odet_amplCFD[odet_nMax];
+    G4double odet_timeCFD100[odet_nMax];
+    G4double odet_timeCFD101[odet_nMax];
+    G4double odet_timeCFD102[odet_nMax];
+    G4double odet_timeCFD103[odet_nMax];
+    G4double odet_timeCFD104[odet_nMax];
+    G4double odet_timeCFD105[odet_nMax];
+    G4double odet_timeCFD106[odet_nMax];
+    G4double odet_timeCFD107[odet_nMax];
+    G4double odet_timeCFD108[odet_nMax];
+    G4double odet_timeCFD109[odet_nMax];
+    G4double odet_timeCFD110[odet_nMax];
+    G4double odet_timeCFD111[odet_nMax];
+    G4double odet_timeCFD112[odet_nMax];
+    G4double odet_timeCFD200[odet_nMax];
+    G4double odet_timeCFD201[odet_nMax];
+    G4double odet_timeCFD202[odet_nMax];
+    G4double odet_timeCFD203[odet_nMax];
+    G4double odet_timeCFD204[odet_nMax];
+    G4double odet_timeCFD205[odet_nMax];
+    G4double odet_timeCFD206[odet_nMax];
+    G4double odet_timeCFD207[odet_nMax];
+    G4double odet_timeCFD208[odet_nMax];
+    G4double odet_timeCFD209[odet_nMax];
+    G4double odet_timeCFD210[odet_nMax];
+    G4double odet_timeCFD211[odet_nMax];
+    G4double odet_timeCFD212[odet_nMax];
+    G4double odet_timeCFD300[odet_nMax];
+    G4double odet_timeCFD301[odet_nMax];
+    G4double odet_timeCFD302[odet_nMax];
+    G4double odet_timeCFD303[odet_nMax];
+    G4double odet_timeCFD304[odet_nMax];
+    G4double odet_timeCFD305[odet_nMax];
+    G4double odet_timeCFD306[odet_nMax];
+    G4double odet_timeCFD307[odet_nMax];
+    G4double odet_timeCFD308[odet_nMax];
+    G4double odet_timeCFD309[odet_nMax];
+    G4double odet_timeCFD310[odet_nMax];
+    G4double odet_timeCFD311[odet_nMax];
+    G4double odet_timeCFD312[odet_nMax];
+    G4double odet_timeCFD400[odet_nMax];
+    G4double odet_timeCFD401[odet_nMax];
+    G4double odet_timeCFD402[odet_nMax];
+    G4double odet_timeCFD403[odet_nMax];
+    G4double odet_timeCFD404[odet_nMax];
+    G4double odet_timeCFD405[odet_nMax];
+    G4double odet_timeCFD406[odet_nMax];
+    G4double odet_timeCFD407[odet_nMax];
+    G4double odet_timeCFD408[odet_nMax];
+    G4double odet_timeCFD409[odet_nMax];
+    G4double odet_timeCFD410[odet_nMax];
+    G4double odet_timeCFD411[odet_nMax];
+    G4double odet_timeCFD412[odet_nMax];
+    G4double odet_timeCFD500[odet_nMax];
+    G4double odet_timeCFD501[odet_nMax];
+    G4double odet_timeCFD502[odet_nMax];
+    G4double odet_timeCFD503[odet_nMax];
+    G4double odet_timeCFD504[odet_nMax];
+    G4double odet_timeCFD505[odet_nMax];
+    G4double odet_timeCFD506[odet_nMax];
+    G4double odet_timeCFD507[odet_nMax];
+    G4double odet_timeCFD508[odet_nMax];
+    G4double odet_timeCFD509[odet_nMax];
+    G4double odet_timeCFD510[odet_nMax];
+    G4double odet_timeCFD511[odet_nMax];
+    G4double odet_timeCFD512[odet_nMax];
 
   public:
     static const Int_t save_nMax=1000;
diff --git a/include/musrScintSD.hh b/include/musrScintSD.hh
index 05dbbef..2cd4069 100644
--- a/include/musrScintSD.hh
+++ b/include/musrScintSD.hh
@@ -35,13 +35,22 @@ class signalInfo {
   public:
     signalInfo(G4int id, G4int nP, G4double tFirst, 
   	       G4double tA, G4double tB, G4double tC, G4double tD, G4double tE, G4double tLast,
-               G4double tCFD, G4double aCFD) {
-               detID=id; nPhot=nP; timeFirst=tFirst;
-               timeA=tA; timeB=tB; timeC=tC; timeD=tD; timeE=tE; timeLast=tLast;
-               timeCFD=tCFD; amplCFD=aCFD;}
+               G4double tCFD, G4double aCFD, G4double tCFDarray[1000]) 
+               {
+                 detID=id; nPhot=nP; timeFirst=tFirst;
+                 timeA=tA; timeB=tB; timeC=tC; timeD=tD; timeE=tE; timeLast=tLast;
+                 timeCFD=tCFD; amplCFD=aCFD; 
+                 if (musrRootOutput::store_odet_timeCFDarray) {for(int i=0;i<1000;i++) {timeCFDarray[i]=tCFDarray[i];}}
+               }
     ~signalInfo() {}
     void transferDataToRoot(musrRootOutput* myRootOut, G4int nn) {
                myRootOut->SetOPSAinfo(nn,detID,nPhot,timeFirst,timeA,timeB,timeC,timeD,timeE,timeLast,timeCFD,amplCFD);
+	       for (Int_t kk=0; kk<13; kk++) {
+		 for (Int_t ll=0; ll<5; ll++) {
+		   int index = (ll+1)*100+kk;
+		   myRootOut -> SetCFDSpecialInfo(index,timeCFDarray[index]);
+		 }
+	       }
     }
 
   private:
@@ -59,6 +68,7 @@ class signalInfo {
     G4double timeLast;
     G4double timeCFD;
     G4double amplCFD;
+    G4double timeCFDarray[1000];
 };
 
 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
@@ -95,6 +105,7 @@ class musrScintSD : public G4VSensitiveDetector
     void ProcessOpticalPhoton(G4Step*);
     void EndOfEvent_OptiacalPhotons();
     void ReadInPulseShapeArray(const char* filename);
+    void FindCFDtime(G4double& OPSA_CFD_time, G4double& OPSA_CFD_ampl, G4double timeOfFirstPhoton);
     G4int FindAPDcellID(G4Step* aStep);
     void SetAPDcellSizes(G4int nx, G4int ny, G4int nz, G4double half_ax, G4double half_ay, G4double half_az) {
       APDcellsEffectRequested = true;
diff --git a/musrSimAna/201.v1190 b/musrSimAna/201.v1190
new file mode 100644
index 0000000..88352da
--- /dev/null
+++ b/musrSimAna/201.v1190
@@ -0,0 +1,160 @@
+# TDC V1190 Set up file generated by Deltat : 16-Apr-2008 10:30:27
+# bins are always in TDC channel units (195.3125 ps/channel)
+
+INSTRUMENT=GPS
+
+DESCRIPTION=No Veto -- 1port
+TYPE=TDCV1190
+RESOLUTION=100
+
+MDELAY=0
+PDELAY=2000
+#REWINDTIMEBINS=10000000
+
+MCOINCIDENCEW=50
+PCOINCIDENCEW=50
+VCOINCIDENCEW=100
+
+# 30000 mu/s
+MUONRATEFACTOR=0.0965819
+#INFINITELYLOWMUONRATE
+
+DATAWINDOWMIN=-2.
+DATAWINDOWMAX=10.0
+PILEUPWINDOWMIN=-10.0
+PILEUPWINDOWMAX=10.0
+
+102; "M up";         M; 0.4;  2005; ;
+  1; "B1";           P; 0.4;  2005; ; B1; 1485; 1515; 50995;
+  2; "B2";           P; 0.4;  2005; ; B2; 1485; 1515; 50995;
+ 11; "F1";           P; 0.4;  2005; ; F11; 1485; 1515; 50995;
+ 12; "F2";           P; 0.4;  2005; ; F12; 1485; 1515; 50995;
+ 13; "F3";           P; 0.4;  2005; ; F13; 1485; 1515; 50995;
+! 21; "Coinc B1"      K; 0.4;  2005;
+! 22; "Coinc B2"      K; 0.4;  2005;
+!401; "Act Veto"      V; 0.1;  2005;
+! 3; "F right";      K; 0.4;  1263;
+! 4; "B left";       P; 0.2;  1311;  5 -10 -11 -12 -13;  Back;   1485; 1515; 50995;
+! 5; "B right";      K; 0.2;  1262;
+! 6;  Up;            P; 0.2;  1306;  -10 -11 -12 -13;    Up;     1490; 1520; 51000;
+! 7;  Down;          P; 0.2;  1264;  -10 -11 -12 -13;    Down;   1525; 1555; 51035;
+! 8; "R int";        P; 0.2;  1309;  -10 -11 -12 -13;    R_int;  1480; 1510; 50990;
+! 9; "R ext";        P; 0.3;  1267;  -10 -11 -12 -13;    R_ext;  1520; 1550; 51020; 8; Rite
+!10; "Bveto up";     V; 0.3;  2085;
+!11; "Bveto down";   V; 0.3;  2089;
+!12; "Bveto left";   V; 0.3;  2080;
+!13; "Bveto right";  V; 0.3;  2079;
+!14; "F center";     P; 0.2;  2073;  -10 -11 -12 -13;    F_cntr;  720;  750; 50230; 2; Forw
+!15;  Clock;         C;
+!16;  Rejected;      R;
+!17;  Ch17;          N;
+!18;  Ch18;          N;
+!19;  Ch19;          N;
+!20;  Ch20;          N;
+!21;  Ch21;          N;
+!22;  Ch22;          N;
+!23;  Ch23;          N;
+!24;  Ch24;          N;
+!25;  Ch25;          N;
+!26;  Ch26;          N;
+!27;  Ch27;          N;
+!28;  Ch28;          N;
+!29;  Ch29;          N;
+!30;  Ch30;          N;
+!31;  Ch31;          N;
+
+#DEBUGEVENT   704 10
+#DEBUGEVENT  1427 10
+#DEBUGEVENT  3222 10
+#DEBUGEVENT  5223 10
+#DEBUGEVENT  8351 10
+#DEBUGEVENT  8581 10
+#DEBUGEVENT  9041 10
+#DEBUGEVENT  9645 10
+
+
+
+counterPhaseShifts 1  0  2 0  11 180  12 180  13 180
+counterGrouping B 1 2
+counterGrouping F 11 12 13
+
+musrTH2D hMuDecayMap "Muon decay map;z [mm]; r[mm]" 100 -80. 20. 40 0. 20. muDecayPosZ muDecayPosR
+musrTH2D hMuDecayMap_a "Muon decay map;z (mm); x (mm)" 400 -300. 100. 400 -200. 200. muDecayPosZ muDecayPosX
+musrTH2D hMuDecayMappileup "Pileup muon decay map;z (mm); r (mm)" 400 -300. 100. 200 0. 200. pileup_muDecayPosZ pileup_muDecayPosR
+musrTH2D hMuDecayMappileup_a "Pileup muon decay map;z (mm); x (mm)" 400 -300. 100. 400 -200. 200. pileup_muDecayPosZ pileup_muDecayPosX
+musrTH1D hMuDecayPosZ "Penetration of muons into the sample;z (mm);N" 100 -5.0 5. muDecayPosZ
+musrTH1D hMuDecayPosZpileup "Decay of the muons contributing to pileup bgr.;z[mm];N" 400 -300 100 pileup_muDecayPosZ
+musrTH1D hMuDecayPosX "X of decayed muons;x[mm];N" 100 -5.0 5. muDecayPosX
+musrTH1D hdet_m0edep  "Energy deposited in the trigger;E[MeV];N" 100 0. 2 det_m0edep
+musrTH1D hdet_posEdep  "Energy deposited in the positron Counters;E[MeV];N" 100 0. 2 det_posEdep
+#musrTH1D hdet_time0  "detected muSR spectra;time[#mus];N" 220 -11. 11. det_time0
+#musrTH1D hdet_time1  "detected muSR spectra;time[#mus];N" 220 -11. 11. det_time1
+#musrTH1D hdet_time10  "detected muSR spectra;time[#mus];N" 220 -11. 11. det_time10
+musrTH1D hgen_time10  "generated muSR spectra;time[#mus];N" 220 -11. 11. gen_time10
+musrTH1D hdet_time10_MINUS_gen_time10   "detected - generated ;time_{det}-time_{gen} [ps];N" 100 -500. 500. det_time10_MINUS_gen_time10
+#musrTH1D hMuDecayDetID "Detector ID where the muons decay;Detector ID; N" 4000 -2000. 2000. muDecayDetID
+musrTH1D hdet_time10      "detected muSR spectra (phase shifted);time[#mus];N" 700 -2.0 12.0 det_time10
+musrTH1D hdet_time10_Bgr  "detected muSR spectra (phase shifted);time[#mus];N" 700 -2.0 12.0 det_time10
+musrTH1D hdet_time20      "detected muSR spectra (phase shifted);time[#mus];N" 700 -2.0 12.0 det_time20
+musrTH1D hdet_time20_Bgr  "detected muSR spectra (phase shifted);time[#mus];N" 700 -2.0 12.0 det_time20
+musrTH1D hMuDecayDetID "Detector ID where the muons decay;Detector ID; N" 2002 -1001. 1001. muDecayDetID
+musrTH1D hMuDecayDetIDpileup "Detector ID where the pileup muons decay;Detector ID; N" 2002 -1001. 1001. pileup_muDecayDetID
+humanDecayHistograms hMuDecayDetID hMuDecayDetIDpileup 201 Sample 211 SampleCell 300 Holder 301 Holder 302 Holder 303 Holder 304 Holder 305 Holder 306 Holder 307 Holder 308 Holder 309 Holder 310 Holder 313 Holder 314 Holder 315 Holder 316 Holder 251 Col_Cu 255 Col_1 257 Col_1 261 Col_2 263 Col_2 265 Al_Plate 102 M0 103 M0Holder 1 BC 2 BC 11 FC 12 FC 13 FC -1 World 291 Magnet 292 Magnet 293 Al_Uprof 230 Elsewhere 231 Elsewhere 232 Elsewhere 233 Elsewhere  256 Elsewhere 262 Elsewhere 267 Elsewhere -1000 Escaped
+
+condition 0 alwaysTrue
+condition 1 oncePerEvent
+condition 2 muonDecayedInSample_gen
+condition 3 muonTriggered_gen
+condition 4 muonTriggered_det
+condition 5 positronHit_det
+condition 6 goodEvent_det
+condition 7 goodEvent_gen
+condition 8 goodEvent_det_AND_goodEvent_gen
+condition 9 pileupEvent
+condition 10 goodEvent_F_det
+condition 11 goodEvent_B_det
+condition 12 goodEvent_F_det_AND_pileupEvent
+condition 13 goodEvent_B_det_AND_pileupEvent
+
+fit hdet_time20_Bgr pol0 WW  -1.9 -0.1 0 
+fit hdet_time20 funct4 "" 0.2 9.8 0 0 0.3 100 0
+fit hdet_time10 funct4 "" 0.05 9.95 0 0 0.3 100 0
+fit hdet_time10_Bgr pol0 WW -1.95 -0.05 0 
+
+#draw hMuDecayPosZ 0
+draw hMuDecayPosZ 1
+#draw hMuDecayPosZ 2
+#draw hMuDecayPosZ 3
+#draw hMuDecayPosZ 4
+###draw hMuDecayMap 0
+###draw hMuDecayMap 1
+draw hdet_m0edep 0
+draw hdet_m0edep 1
+draw hdet_m0edep 2
+draw hdet_m0edep 3
+draw hdet_m0edep 4
+draw hdet_m0edep 5
+draw hdet_m0edep 6
+draw hdet_time10 6
+#draw hdet_time20 10
+#draw hdet_time20 11
+#draw hdet_time20_Bgr 10
+#draw hdet_time20_Bgr 11
+draw hgen_time10 7
+draw hdet_time10_MINUS_gen_time10 8
+draw hdet_posEdep 5
+draw hMuDecayDetID 1
+draw hdet_m0edep 9
+draw hdet_time10 9
+draw hMuDecayDetIDpileup 1
+draw hMuDecayDetIDpileup 6
+draw hMuDecayDetIDpileup 9
+draw humanDecayHistograms 1
+draw humanDecayHistograms 6
+draw humanDecayHistograms 9
+draw humanDecayPileupHistograms 1
+draw humanDecayPileupHistograms 6
+draw humanDecayPileupHistograms 9
+draw hdet_time20 4
+draw hdet_time20 6
+$
diff --git a/musrSimAna/201a.v1190 b/musrSimAna/201a.v1190
new file mode 100644
index 0000000..8e40760
--- /dev/null
+++ b/musrSimAna/201a.v1190
@@ -0,0 +1,158 @@
+# TDC V1190 Set up file generated by Deltat : 16-Apr-2008 10:30:27
+# bins are always in TDC channel units (195.3125 ps/channel)
+
+INSTRUMENT=GPS
+
+DESCRIPTION=No Veto -- 1port
+TYPE=TDCV1190
+RESOLUTION=100
+
+MDELAY=0
+PDELAY=2000
+#REWINDTIMEBINS=10000000
+
+MCOINCIDENCEW=50
+PCOINCIDENCEW=50
+VCOINCIDENCEW=100
+
+# 30000 mu/s
+#MUONRATEFACTOR=0.0965819
+INFINITELYLOWMUONRATE
+
+DATAWINDOWMIN=-2.
+DATAWINDOWMAX=10.0
+PILEUPWINDOWMIN=-10.0
+PILEUPWINDOWMAX=10.0
+
+102; "M up";         M; 0.4;  2005; ;
+  1; "B1";           P; 0.4;  2005; ; B1; 1485; 1515; 50995;
+  2; "B2";           P; 0.4;  2005; ; B2; 1485; 1515; 50995;
+ 11; "F1";           P; 0.4;  2005; ; F11; 1485; 1515; 50995;
+ 12; "F2";           P; 0.4;  2005; ; F12; 1485; 1515; 50995;
+ 13; "F3";           P; 0.4;  2005; ; F13; 1485; 1515; 50995;
+! 21; "Coinc B1"      K; 0.4;  2005;
+! 22; "Coinc B2"      K; 0.4;  2005;
+!401; "Act Veto"      V; 0.1;  2005;
+! 3; "F right";      K; 0.4;  1263;
+! 4; "B left";       P; 0.2;  1311;  5 -10 -11 -12 -13;  Back;   1485; 1515; 50995;
+! 5; "B right";      K; 0.2;  1262;
+! 6;  Up;            P; 0.2;  1306;  -10 -11 -12 -13;    Up;     1490; 1520; 51000;
+! 7;  Down;          P; 0.2;  1264;  -10 -11 -12 -13;    Down;   1525; 1555; 51035;
+! 8; "R int";        P; 0.2;  1309;  -10 -11 -12 -13;    R_int;  1480; 1510; 50990;
+! 9; "R ext";        P; 0.3;  1267;  -10 -11 -12 -13;    R_ext;  1520; 1550; 51020; 8; Rite
+!10; "Bveto up";     V; 0.3;  2085;
+!11; "Bveto down";   V; 0.3;  2089;
+!12; "Bveto left";   V; 0.3;  2080;
+!13; "Bveto right";  V; 0.3;  2079;
+!14; "F center";     P; 0.2;  2073;  -10 -11 -12 -13;    F_cntr;  720;  750; 50230; 2; Forw
+!15;  Clock;         C;
+!16;  Rejected;      R;
+!17;  Ch17;          N;
+!18;  Ch18;          N;
+!19;  Ch19;          N;
+!20;  Ch20;          N;
+!21;  Ch21;          N;
+!22;  Ch22;          N;
+!23;  Ch23;          N;
+!24;  Ch24;          N;
+!25;  Ch25;          N;
+!26;  Ch26;          N;
+!27;  Ch27;          N;
+!28;  Ch28;          N;
+!29;  Ch29;          N;
+!30;  Ch30;          N;
+!31;  Ch31;          N;
+
+#DEBUGEVENT   704 10
+#DEBUGEVENT  1427 10
+#DEBUGEVENT  3222 10
+#DEBUGEVENT  5223 10
+#DEBUGEVENT  8351 10
+#DEBUGEVENT  8581 10
+#DEBUGEVENT  9041 10
+#DEBUGEVENT  9645 10
+
+
+
+counterPhaseShifts 1  0  2 0  11 180  12 180  13 180
+counterGrouping B 1 2
+counterGrouping F 11 12 13
+
+musrTH2D hMuDecayMap "Muon decay map;z [mm]; r[mm]" 100 -80. 20. 40 0. 20. muDecayPosZ muDecayPosR
+musrTH2D hMuDecayMappileup "Pileup muon decay map;z [mm]; r[mm]" 400 -300. 100. 200 0. 200. pileup_muDecayPosZ pileup_muDecayPosR
+musrTH1D hMuDecayPosZ "Penetration of muons into the sample;z[mm];N" 100 -5.0 5. muDecayPosZ
+musrTH1D hMuDecayPosZpileup "Decay of the muons contributing to pileup bgr.;z[mm];N" 400 -300 100 pileup_muDecayPosZ
+musrTH1D hMuDecayPosX "X of decayed muons;x[mm];N" 100 -5.0 5. muDecayPosX
+musrTH1D hdet_m0edep  "Energy deposited in the trigger;E[MeV];N" 100 0. 2 det_m0edep
+musrTH1D hdet_posEdep  "Energy deposited in the positron Counters;E[MeV];N" 100 0. 2 det_posEdep
+#musrTH1D hdet_time0  "detected muSR spectra;time[#mus];N" 220 -11. 11. det_time0
+#musrTH1D hdet_time1  "detected muSR spectra;time[#mus];N" 220 -11. 11. det_time1
+#musrTH1D hdet_time10  "detected muSR spectra;time[#mus];N" 220 -11. 11. det_time10
+musrTH1D hgen_time10  "generated muSR spectra;time[#mus];N" 220 -11. 11. gen_time10
+musrTH1D hdet_time10_MINUS_gen_time10   "detected - generated ;time_{det}-time_{gen} [ps];N" 100 -500. 500. det_time10_MINUS_gen_time10
+#musrTH1D hMuDecayDetID "Detector ID where the muons decay;Detector ID; N" 4000 -2000. 2000. muDecayDetID
+musrTH1D hdet_time10      "detected muSR spectra (phase shifted);time[#mus];N" 700 -2.0 12.0 det_time10
+musrTH1D hdet_time10_Bgr  "detected muSR spectra (phase shifted);time[#mus];N" 700 -2.0 12.0 det_time10
+musrTH1D hdet_time20      "detected muSR spectra (phase shifted);time[#mus];N" 700 -2.0 12.0 det_time20
+musrTH1D hdet_time20_Bgr  "detected muSR spectra (phase shifted);time[#mus];N" 700 -2.0 12.0 det_time20
+musrTH1D hMuDecayDetID "Detector ID where the muons decay;Detector ID; N" 2002 -1001. 1001. muDecayDetID
+musrTH1D hMuDecayDetIDpileup "Detector ID where the pileup muons decay;Detector ID; N" 2002 -1001. 1001. pileup_muDecayDetID
+humanDecayHistograms hMuDecayDetID hMuDecayDetIDpileup 201 Sample 211 SampleCell 300 Holder 301 Holder 302 Holder 303 Holder 304 Holder 305 Holder 306 Holder 307 Holder 308 Holder 309 Holder 310 Holder 313 Holder 314 Holder 315 Holder 316 Holder 251 Col_Cu 255 Col_1 257 Col_1 261 Col_2 263 Col_2 265 Al_Plate 102 M0 103 M0Holder 1 BC 2 BC 11 FC 12 FC 13 FC -1 World 291 Magnet 292 Magnet 293 Al_Uprof 230 Elsewhere 231 Elsewhere 232 Elsewhere 233 Elsewhere  256 Elsewhere 262 Elsewhere 267 Elsewhere -1000 Escaped
+
+condition 0 alwaysTrue
+condition 1 oncePerEvent
+condition 2 muonDecayedInSample_gen
+condition 3 muonTriggered_gen
+condition 4 muonTriggered_det
+condition 5 positronHit_det
+condition 6 goodEvent_det
+condition 7 goodEvent_gen
+condition 8 goodEvent_det_AND_goodEvent_gen
+condition 9 pileupEvent
+condition 10 goodEvent_F_det
+condition 11 goodEvent_B_det
+condition 12 goodEvent_F_det_AND_pileupEvent
+condition 13 goodEvent_B_det_AND_pileupEvent
+
+fit hdet_time20_Bgr pol0 WW  -1.9 -0.1 0 
+fit hdet_time20 funct4 "" 0.2 9.8 0 0 0.3 100 0
+fit hdet_time10 funct4 "" 0.05 9.95 0 0 0.3 100 0
+fit hdet_time10_Bgr pol0 WW -1.95 -0.05 0 
+
+#draw hMuDecayPosZ 0
+draw hMuDecayPosZ 1
+#draw hMuDecayPosZ 2
+#draw hMuDecayPosZ 3
+#draw hMuDecayPosZ 4
+###draw hMuDecayMap 0
+###draw hMuDecayMap 1
+draw hdet_m0edep 0
+draw hdet_m0edep 1
+draw hdet_m0edep 2
+draw hdet_m0edep 3
+draw hdet_m0edep 4
+draw hdet_m0edep 5
+draw hdet_m0edep 6
+draw hdet_time10 6
+#draw hdet_time20 10
+#draw hdet_time20 11
+#draw hdet_time20_Bgr 10
+#draw hdet_time20_Bgr 11
+draw hgen_time10 7
+draw hdet_time10_MINUS_gen_time10 8
+draw hdet_posEdep 5
+draw hMuDecayDetID 1
+draw hdet_m0edep 9
+draw hdet_time10 9
+draw hMuDecayDetIDpileup 1
+draw hMuDecayDetIDpileup 6
+draw hMuDecayDetIDpileup 9
+draw humanDecayHistograms 1
+draw humanDecayHistograms 6
+draw humanDecayHistograms 9
+draw humanDecayPileupHistograms 1
+draw humanDecayPileupHistograms 6
+draw humanDecayPileupHistograms 9
+draw hdet_time20 4
+draw hdet_time20 6
+$
diff --git a/musrSimAna/musrAnalysis.cxx b/musrSimAna/musrAnalysis.cxx
index aec0808..758e6ae 100644
--- a/musrSimAna/musrAnalysis.cxx
+++ b/musrSimAna/musrAnalysis.cxx
@@ -503,8 +503,9 @@ void musrAnalysis::ReadInInputParameters(char* charV1190FileName) {
 	}
       }
       else if  (strcmp(tmpString0,"fit")==0) {
-	char histoName[100]; char functionName[100]; float xMin; float xMax; float p0, p1, p2, p3, p4, p5, p6;
-	sscanf(&line[0],"%*s %s %s %g %g %g %g %g %g %g",histoName,functionName,&xMin,&xMax,&p0,&p1,&p2,&p3,&p4,&p5,&p6);
+	char histoName[100]; char functionName[100]; char functOption[100]; float xMin; float xMax; float p0, p1, p2, p3, p4, p5, p6;
+	sscanf(&line[0],"%*s %s %s %s %g %g %g %g %g %g %g",histoName,functionName,functOption,&xMin,&xMax,&p0,&p1,&p2,&p3,&p4,&p5,&p6);
+	if (strcmp(functOption,"\"\"")==0) strcpy(functOption,"");
 
 	TF1 *funct;
 	
@@ -576,7 +577,7 @@ void musrAnalysis::ReadInInputParameters(char* charV1190FileName) {
 	  exit(1);
 	}
 
-	tmpHistograms->AssignFunction(funct, xMin, xMax);
+	tmpHistograms->AssignFunction(funct, functOption, xMin, xMax);
       }
       
       else { 
@@ -957,6 +958,8 @@ void musrAnalysis::FillHistograms(Int_t iiiEntry) {
     //    Long64_t dataBinMax = (mCounterHitExistsForThisEventID) ? timeBin0+dataWindowBinMax : timeBinOfThePreviouslyProcessedHit+100000000;
     pileup_eventID             = -1001;
     pileup_muDecayDetID_double = -1001;
+    pileup_muDecayPosX         = -1000000000;
+    pileup_muDecayPosY         = -1000000000;
     pileup_muDecayPosZ         = -1000000000;
     pileup_muDecayPosR         = -1000000000;
     if (mCounterHitExistsForThisEventID) {
@@ -970,6 +973,8 @@ void musrAnalysis::FillHistograms(Int_t iiiEntry) {
 	fChain->GetEntry(posEntry);
 	pileup_eventID             = eventID;
 	pileup_muDecayDetID_double = muDecayDetID;
+	pileup_muDecayPosX         = muDecayPosX;
+	pileup_muDecayPosY         = muDecayPosY;
 	pileup_muDecayPosZ         = muDecayPosZ;
 	pileup_muDecayPosR         = sqrt(muDecayPosX*muDecayPosX+muDecayPosY*muDecayPosY);
 	//	if (pileup_muDecayDetID_double==-1000) {
diff --git a/musrSimAna/musrAnalysis.hh b/musrSimAna/musrAnalysis.hh
index ef76ecd..746dc1a 100644
--- a/musrSimAna/musrAnalysis.hh
+++ b/musrSimAna/musrAnalysis.hh
@@ -208,6 +208,8 @@ public :
    Double_t        det_time20;
    Double_t        pileup_eventID;
    Double_t        pileup_muDecayDetID_double;
+   Double_t        pileup_muDecayPosX;
+   Double_t        pileup_muDecayPosY;
    Double_t        pileup_muDecayPosZ;
    Double_t        pileup_muDecayPosR;
 
@@ -443,6 +445,8 @@ musrAnalysis::musrAnalysis(TTree *tree)
   variableMap["det_time10_MINUS_gen_time10"]=&det_time10_MINUS_gen_time10;
   variableMap["pileup_eventID"]=&pileup_eventID;
   variableMap["pileup_muDecayDetID"]=&pileup_muDecayDetID_double;
+  variableMap["pileup_muDecayPosX"]=&pileup_muDecayPosX;
+  variableMap["pileup_muDecayPosY"]=&pileup_muDecayPosY;
   variableMap["pileup_muDecayPosZ"]=&pileup_muDecayPosZ;
   variableMap["pileup_muDecayPosR"]=&pileup_muDecayPosR;
   variableMap["det_time20"]=&det_time20;
diff --git a/musrSimAna/musrTH.cxx b/musrSimAna/musrTH.cxx
index 01f95ac..e956918 100644
--- a/musrSimAna/musrTH.cxx
+++ b/musrSimAna/musrTH.cxx
@@ -16,6 +16,7 @@ musrTH::musrTH(char* dimension, char* histoName, char* histoTitle, Int_t nrOfBin
   bool_rotating_reference_frame=false;
   rot_ref_frequency=0;
   rot_ref_phase=0;
+  strcpy(funct_option,"");
   //  std::cout<<"hojhoj    variableName1="<<variableName1<<"   variableToBeFilled_X="<<variableToBeFilled_X<<std::endl;
 
   char nameHist[500];
@@ -189,10 +190,12 @@ void musrTH::FillHumanDecayArray(musrTH* decayMapHistos, humanDecayMapType myMap
   }
 }
 //==============================================================================================
-void  musrTH::AssignFunction(TF1* function, Double_t xMin, Double_t xMax) {
+void  musrTH::AssignFunction(TF1* function, char* functOption, Double_t xMin, Double_t xMax) {
   funct = function;
+  strcpy(funct_option,functOption);
   funct_xMin = xMin;
   funct_xMax = xMax;
+  std::cout<<"musrTH::AssignFunction: "<<funct->GetName()<<", option="<<funct_option<<", xMin="<<xMin<<", xMax="<<xMax<<std::endl;
 
 }
 //==============================================================================================
@@ -218,13 +221,16 @@ void  musrTH::FitHistogramsIfRequired(Double_t omega) {
     }
   }
 
+  Double_t ppp[100];
   std::cout<<"    Initial parameter setting: ";
-  for (Int_t i=0; i<(funct->GetNumberFreeParameters()); i++) std::cout<<funct->GetParameter(i)<<", ";
+  Int_t n_ppp = funct->GetNumberFreeParameters();
+  for (Int_t i=0; i<n_ppp; i++) {ppp[i]=funct->GetParameter(i); std::cout<<ppp[i]<<", ";}
   std::cout<<std::endl;
       
   for (Int_t i=0; i<musrAnalysis::nrConditions; i++) {
     //    std::cout<<"fitted histogram pointer="<<histArray1D[i]<<std::endl;
-    histArray1D[i]->Fit(funct,"WW","",funct_xMin,funct_xMax);
+    for (Int_t j=0; j<n_ppp; j++) {funct->SetParameter(j,ppp[j]);}
+    histArray1D[i]->Fit(funct,funct_option,"",funct_xMin,funct_xMax);
     //    histArray1D[i]->Fit(funct,"LL","",funct_xMin,funct_xMax);
   }
   //  if (strcmp(funct->GetName(),"simpleExpoPLUSconst")==0) {
diff --git a/musrSimAna/musrTH.hh b/musrSimAna/musrTH.hh
index 7f6b9c0..87fef96 100644
--- a/musrSimAna/musrTH.hh
+++ b/musrSimAna/musrTH.hh
@@ -37,7 +37,7 @@ public:
   Int_t GetNbinsX1D();
   Int_t GetNbinsX2D();
   Int_t GetNbinsY2D();
-  void  AssignFunction(TF1* function, Double_t xMin, Double_t xMax);
+  void  AssignFunction(TF1* function, char* functOption, Double_t xMin, Double_t xMax);
   void  FitHistogramsIfRequired(Double_t omega);
   void  SetRotatingReferenceFrame(Double_t frequency, Double_t phase) {bool_rotating_reference_frame=true; 
                                                                        rot_ref_frequency=frequency; rot_ref_phase=phase;}
@@ -52,6 +52,7 @@ private:
   std::list<int> drawList;
   TF1*   funct;
   Double_t funct_xMin, funct_xMax;
+  char   funct_option[100];
   Bool_t bool_rotating_reference_frame;
   Double_t rot_ref_frequency, rot_ref_phase;
   //  Double_t N0_FromLastFit;
diff --git a/run/101.mac b/run/101.mac
index c5104ca..1aa1e58 100644
--- a/run/101.mac
+++ b/run/101.mac
@@ -18,67 +18,32 @@
 #
 #============================================================
 /musr/command visattributes log_World invisible
-/musr/command visattributes log_source red
+#/musr/command visattributes log_source red
 /musr/command visattributes G4_PLASTIC_SC_VINYLTOLUENE lightblue
 ###################################################################################
 #########################  P H Y S I C S      P R O C E S S E S  ##################
 ###################################################################################
-# --- Low Energy (default) ---
-/musr/command process addDiscreteProcess gamma G4LowEnergyPhotoElectric
-/musr/command process addDiscreteProcess gamma G4LowEnergyCompton
-/musr/command process addDiscreteProcess gamma G4LowEnergyGammaConversion
-/musr/command process addDiscreteProcess gamma G4LowEnergyRayleigh
-/musr/command process addProcess         e-    G4MultipleScattering -1 1 1
-#/musr/command process addDiscreteProcess e-    G4CoulombScattering
-/musr/command process addProcess         e-    G4LowEnergyIonisation -1 2 2
-/musr/command process addProcess         e-    G4LowEnergyBremsstrahlung -1 -1 3
-/musr/command process addProcess         e+    G4MultipleScattering -1 1 1
-#/musr/command process addDiscreteProcess e+    G4CoulombScattering
-/musr/command process addProcess         e+    G4eIonisation    -1 2 2
-/musr/command process addProcess         e+    G4eBremsstrahlung   -1 3 3
-/musr/command process addProcess         e+    G4eplusAnnihilation 0 -1 4
+# Geant 4.9.4
+/musr/command process addDiscreteProcess gamma G4PhotoElectricEffect
+/musr/command process addDiscreteProcess gamma G4ComptonScattering
+/musr/command process addDiscreteProcess gamma G4GammaConversion
+/musr/command process addDiscreteProcess gamma G4RayleighScattering
+/musr/command process addProcess         e-    G4eMultipleScattering    -1  1  1
+/musr/command process addProcess         e-    G4eIonisation            -1  2  2
+/musr/command process addProcess         e-    G4eBremsstrahlung        -1  3  3
+/musr/command process addProcess         e+    G4eMultipleScattering    -1  1  1
+/musr/command process addProcess         e+    G4eIonisation            -1  2  2
+/musr/command process addProcess         e+    G4eBremsstrahlung        -1  3  3
+/musr/command process addProcess         e+    G4eplusAnnihilation       0 -1  4
+#/musr/command process addProcess         mu-   G4MuMultipleScattering   -1  1  1
+#/musr/command process addProcess         mu-   G4MuIonisation           -1  2  2
+#/musr/command process addProcess         mu-   G4MuBremsstrahlung       -1  3  3
+#/musr/command process addProcess         mu-   G4MuPairProduction       -1  4  4
+#/musr/command process addProcess         mu+   G4MuMultipleScattering   -1  1  1
+#/musr/command process addProcess         mu+   G4MuIonisation           -1  2  2
+#/musr/command process addProcess         mu+   G4MuBremsstrahlung       -1  3  3
+#/musr/command process addProcess         mu+   G4MuPairProduction       -1  4  4
 #
-# --- High Energy ---
-#/musr/command process addDiscreteProcess gamma G4PhotoElectricEffect
-#/musr/command process addDiscreteProcess gamma G4ComptonScattering
-#/musr/command process addDiscreteProcess gamma G4GammaConversion
-#/musr/command process addProcess         e-    G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess e-    G4CoulombScattering
-#/musr/command process addProcess         e-    G4eIonisation       -1 2 2
-#/musr/command process addProcess         e-    G4eBremsstrahlung   -1 3 3
-#/musr/command process addProcess         e+    G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess e+    G4CoulombScattering
-#/musr/command process addProcess         e+    G4eIonisation    -1 2 2
-#/musr/command process addProcess         e+    G4eBremsstrahlung   -1 3 3
-#/musr/command process addProcess         e+    G4eplusAnnihilation 0 -1 4
-#
-# --- Penelope ---
-#/musr/command process addDiscreteProcess gamma G4PenelopePhotoElectric
-#/musr/command process addDiscreteProcess gamma G4PenelopeCompton
-#/musr/command process addDiscreteProcess gamma G4PenelopeGammaConversion
-#/musr/command process addDiscreteProcess gamma G4PenelopeRayleigh
-#/musr/command process addProcess         e-    G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess e-    G4CoulombScattering
-#/musr/command process addProcess         e-    G4PenelopeIonisation   -1 2 2
-#/musr/command process addProcess         e-    G4PenelopeBremsstrahlung -1 -1 3
-#/musr/command process addProcess         e+    G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess e+    G4CoulombScattering
-#/musr/command process addProcess         e+    G4PenelopeIonisation,     -1  2 2
-#/musr/command process addProcess         e+    G4PenelopeBremsstrahlung, -1 -1 3
-#/musr/command process addProcess         e+    G4PenelopeAnnihilation,    0 -1 4
-#
-# --- Muons ---
-#/musr/command process addProcess          mu+   G4MultipleScattering -1 1 1
-##/musr/command process addProcess          mu+   MultipleAndCoulombScattering -1 1 1 goulombRegion
-##/musr/command process addDiscreteProcess  mu+   G4CoulombScattering
-#/musr/command process addProcess          mu+   G4MuIonisation       -1 2 2
-#/musr/command process addProcess          mu+   G4MuBremsstrahlung   -1 3 3
-#/musr/command process addProcess          mu+   G4MuPairProduction   -1 4 4
-#/musr/command process addProcess          mu-   G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess  mu-   G4CoulombScattering
-#/musr/command process addProcess          mu-   G4MuIonisation       -1 2 2
-#/musr/command process addProcess          mu-   G4MuBremsstrahlung   -1 3 3
-#/musr/command process addProcess          mu-   G4MuPairProduction   -1 4 4
 ###################################################################################
 ##################  S O M E   O T H E R    P A R A M E T E R S   ##################
 ###################################################################################
@@ -165,6 +130,19 @@
 /musr/command rootOutput det_VvvProcID off
 /musr/command rootOutput det_VvvTrackID off
 /musr/command rootOutput det_VvvParticleID off
+/musr/command rootOutput odet_ID           off
+/musr/command rootOutput nOptPhot          off
+/musr/command rootOutput odet_nPhot        off
+/musr/command rootOutput odet_timeFirst    off
+/musr/command rootOutput odet_timeA        off
+/musr/command rootOutput odet_timeB        off
+/musr/command rootOutput odet_timeC        off
+/musr/command rootOutput odet_timeD        off
+/musr/command rootOutput odet_timeE        off
+/musr/command rootOutput odet_timeMean     off
+/musr/command rootOutput odet_timeLast     off
+/musr/command rootOutput odet_timeCFD      off
+/musr/command rootOutput odet_amplCFD      off
 ### Root variables that are not written out by default, but can be switched on:
 #/musr/command rootOutput fieldIntegralBx on
 #/musr/command rootOutput fieldIntegralBy on
@@ -177,7 +155,7 @@
 ###################################################################################
 #/vis/disable
 #/control/execute visFromToni.mac
-/control/execute visDawn102.mac
+/control/execute visDawn101.mac
 #/control/execute visVRML.mac
 ###################################################################################
 ######################### P A R T I C L E   G U N #################################
@@ -200,4 +178,5 @@
 #/gps/ang/maxtheta 2 deg
 #/gps/ang/maxphi 2 deg
 ########################  B E A M    O N  #######################################
-/run/beamOn 10
+#/run/beamOn 1000
+/run/beamOn 5
\ No newline at end of file
diff --git a/run/102.mac b/run/102.mac
index e87030d..e817cdf 100644
--- a/run/102.mac
+++ b/run/102.mac
@@ -23,62 +23,27 @@
 ###################################################################################
 #########################  P H Y S I C S      P R O C E S S E S  ##################
 ###################################################################################
-# --- Low Energy (default) ---
-/musr/command process addDiscreteProcess gamma G4LowEnergyPhotoElectric
-/musr/command process addDiscreteProcess gamma G4LowEnergyCompton
-/musr/command process addDiscreteProcess gamma G4LowEnergyGammaConversion
-/musr/command process addDiscreteProcess gamma G4LowEnergyRayleigh
-/musr/command process addProcess         e-    G4MultipleScattering -1 1 1
-#/musr/command process addDiscreteProcess e-    G4CoulombScattering
-/musr/command process addProcess         e-    G4LowEnergyIonisation -1 2 2
-/musr/command process addProcess         e-    G4LowEnergyBremsstrahlung -1 -1 3
-/musr/command process addProcess         e+    G4MultipleScattering -1 1 1
-#/musr/command process addDiscreteProcess e+    G4CoulombScattering
-/musr/command process addProcess         e+    G4eIonisation    -1 2 2
-/musr/command process addProcess         e+    G4eBremsstrahlung   -1 3 3
-/musr/command process addProcess         e+    G4eplusAnnihilation 0 -1 4
+# Geant 4.9.4
+/musr/command process addDiscreteProcess gamma G4PhotoElectricEffect
+/musr/command process addDiscreteProcess gamma G4ComptonScattering
+/musr/command process addDiscreteProcess gamma G4GammaConversion
+/musr/command process addDiscreteProcess gamma G4RayleighScattering
+/musr/command process addProcess         e-    G4eMultipleScattering    -1  1  1
+/musr/command process addProcess         e-    G4eIonisation            -1  2  2
+/musr/command process addProcess         e-    G4eBremsstrahlung        -1  3  3
+/musr/command process addProcess         e+    G4eMultipleScattering    -1  1  1
+/musr/command process addProcess         e+    G4eIonisation            -1  2  2
+/musr/command process addProcess         e+    G4eBremsstrahlung        -1  3  3
+/musr/command process addProcess         e+    G4eplusAnnihilation       0 -1  4
+#/musr/command process addProcess         mu-   G4MuMultipleScattering   -1  1  1
+#/musr/command process addProcess         mu-   G4MuIonisation           -1  2  2
+#/musr/command process addProcess         mu-   G4MuBremsstrahlung       -1  3  3
+#/musr/command process addProcess         mu-   G4MuPairProduction       -1  4  4
+#/musr/command process addProcess         mu+   G4MuMultipleScattering   -1  1  1
+#/musr/command process addProcess         mu+   G4MuIonisation           -1  2  2
+#/musr/command process addProcess         mu+   G4MuBremsstrahlung       -1  3  3
+#/musr/command process addProcess         mu+   G4MuPairProduction       -1  4  4
 #
-# --- High Energy ---
-#/musr/command process addDiscreteProcess gamma G4PhotoElectricEffect
-#/musr/command process addDiscreteProcess gamma G4ComptonScattering
-#/musr/command process addDiscreteProcess gamma G4GammaConversion
-#/musr/command process addProcess         e-    G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess e-    G4CoulombScattering
-#/musr/command process addProcess         e-    G4eIonisation       -1 2 2
-#/musr/command process addProcess         e-    G4eBremsstrahlung   -1 3 3
-#/musr/command process addProcess         e+    G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess e+    G4CoulombScattering
-#/musr/command process addProcess         e+    G4eIonisation    -1 2 2
-#/musr/command process addProcess         e+    G4eBremsstrahlung   -1 3 3
-#/musr/command process addProcess         e+    G4eplusAnnihilation 0 -1 4
-#
-# --- Penelope ---
-#/musr/command process addDiscreteProcess gamma G4PenelopePhotoElectric
-#/musr/command process addDiscreteProcess gamma G4PenelopeCompton
-#/musr/command process addDiscreteProcess gamma G4PenelopeGammaConversion
-#/musr/command process addDiscreteProcess gamma G4PenelopeRayleigh
-#/musr/command process addProcess         e-    G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess e-    G4CoulombScattering
-#/musr/command process addProcess         e-    G4PenelopeIonisation   -1 2 2
-#/musr/command process addProcess         e-    G4PenelopeBremsstrahlung -1 -1 3
-#/musr/command process addProcess         e+    G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess e+    G4CoulombScattering
-#/musr/command process addProcess         e+    G4PenelopeIonisation,     -1  2 2
-#/musr/command process addProcess         e+    G4PenelopeBremsstrahlung, -1 -1 3
-#/musr/command process addProcess         e+    G4PenelopeAnnihilation,    0 -1 4
-#
-# --- Muons ---
-#/musr/command process addProcess          mu+   G4MultipleScattering -1 1 1
-##/musr/command process addProcess          mu+   MultipleAndCoulombScattering -1 1 1 goulombRegion
-##/musr/command process addDiscreteProcess  mu+   G4CoulombScattering
-#/musr/command process addProcess          mu+   G4MuIonisation       -1 2 2
-#/musr/command process addProcess          mu+   G4MuBremsstrahlung   -1 3 3
-#/musr/command process addProcess          mu+   G4MuPairProduction   -1 4 4
-#/musr/command process addProcess          mu-   G4MultipleScattering -1 1 1
-##/musr/command process addDiscreteProcess  mu-   G4CoulombScattering
-#/musr/command process addProcess          mu-   G4MuIonisation       -1 2 2
-#/musr/command process addProcess          mu-   G4MuBremsstrahlung   -1 3 3
-#/musr/command process addProcess          mu-   G4MuPairProduction   -1 4 4
 ###################################################################################
 ##################  S O M E   O T H E R    P A R A M E T E R S   ##################
 ###################################################################################
@@ -165,6 +130,19 @@
 /musr/command rootOutput det_VvvProcID off
 /musr/command rootOutput det_VvvTrackID off
 /musr/command rootOutput det_VvvParticleID off
+/musr/command rootOutput odet_ID           off
+/musr/command rootOutput nOptPhot          off
+/musr/command rootOutput odet_nPhot        off
+/musr/command rootOutput odet_timeFirst    off
+/musr/command rootOutput odet_timeA        off
+/musr/command rootOutput odet_timeB        off
+/musr/command rootOutput odet_timeC        off
+/musr/command rootOutput odet_timeD        off
+/musr/command rootOutput odet_timeE        off
+/musr/command rootOutput odet_timeMean     off
+/musr/command rootOutput odet_timeLast     off
+/musr/command rootOutput odet_timeCFD      off
+/musr/command rootOutput odet_amplCFD      off
 ### Root variables that are not written out by default, but can be switched on:
 #/musr/command rootOutput fieldIntegralBx on
 #/musr/command rootOutput fieldIntegralBy on
@@ -177,7 +155,7 @@
 ###################################################################################
 #/vis/disable
 #/control/execute visFromToni.mac
-/control/execute visDawn1.mac
+/control/execute visDawn102.mac
 #/control/execute visVRML.mac
 ###################################################################################
 ######################### P A R T I C L E   G U N #################################
diff --git a/run/110.mac b/run/110.mac
new file mode 100644
index 0000000..c6ea60b
--- /dev/null
+++ b/run/110.mac
@@ -0,0 +1,241 @@
+#-----------------------------------------------------------------------
+# Macro file for the simulation of electron/positrons from the Sr decay
+# passing through the scintiallator detectors (blocks).
+# Unless specified otherwises, the default units are mm, ns, MeV, MeV/c.
+# Lines starting with star "#" are comments.
+###################################################################################
+#############################  G E O M E T R Y  ###################################
+#
+# WORLD
+/musr/command construct box World     10 10 100 G4_AIR                0 0 0 no_logical_volume  norot dead -1
+#
+# Sr SOURCE
+/musr/command construct sphere source   0  0.02  0 360 0 180  G4_Sr                   0 0 0 log_World       norot dead 301
+#
+# SCINTILLATOR BLOCKS
+/musr/command construct box scintFarAwayC1  1.5  1.5  1  G4_PLASTIC_SC_VINYLTOLUENE 0 0 5   log_World   norot musr/ScintSD 10
+/musr/command construct box scintFarAwayC2  1.5  1.5  1  G4_PLASTIC_SC_VINYLTOLUENE 0 0 14  log_World   norot musr/ScintSD 11
+#
+# APDs
+/musr/command construct box APD1      0.1  1.5 1.5      G4_Cu                       1.6 0  5 log_World     norot   dead 20
+/musr/command construct box APD2      0.1  1.5 1.5      G4_Cu                       1.6 0 14 log_World     norot   dead 21
+#
+# Plastic holders
+/musr/command construct box Holder1   0.75 4   4        G4_GLASS_PLATE              2.5 0  5 log_World     norot   dead 30
+/musr/command construct box Holder2   0.75 4   4        G4_GLASS_PLATE              2.5 0 14 log_World     norot   dead 31
+#============================================================
+/musr/command visattributes log_World invisible
+/musr/command visattributes log_source red
+/musr/command visattributes G4_PLASTIC_SC_VINYLTOLUENE lightblue
+/musr/command visattributes log_APD1 red
+###################################################################################
+########################## O P T I C A L    P H O T O N S #########################
+#         PhotonEnergy[nEntries] = 
+#	{ 2.695*eV,   2.75489*eV, 2.8175*eV,  2.88302*eV,                 // 460, 450, 440, 430 nm
+#	  2.95167*eV, 3.02366*eV, 3.09925*eV, 3.17872*eV, 3.26237*eV,     // 420, 410, 400, 390, 380 nm
+#	  3.30587*eV, 3.35054*eV, 3.44361*eV, 3.542*eV,   3.64618*eV };   // 375, 370, 360, 350, 340 nm
+#/musr/command materialPropertiesTable optScintMPT ABSLENGTH    2   2.695e-6 3.64618e-6  80 80
+/musr/command materialPropertiesTable optScintMPT RINDEX        2   2.695e-6 3.64618e-6  1.58 1.58
+/musr/command materialPropertiesTable optScintMPT FASTCOMPONENT 14  2.695e-6 2.75489e-6 2.8175e-6 2.88302e-6 2.95167e-6 3.02366e-6 3.09925e-6 3.17872e-6 3.26237e-6 3.30587e-6 3.35054e-6 3.44361e-6 3.542e-6 3.64618e-6  0.01 0.07 0.15 0.26 0.375 0.52 0.65 0.80 0.95 1 0.88 0.44 0.08 0.01
+#/musr/command materialPropertiesTable optScintMPT SLOWCOMPONENT 14   2.695e-6 2.75489e-6 2.8175e-6 2.88302e-6 2.95167e-6 3.02366e-6 3.09925e-6 3.17872e-6 3.26237e-6 3.30587e-6 3.35054e-6 3.44361e-6 3.542e-6 3.64618e-6  0.01 0.07 0.15 0.26 0.375 0.52 0.65 0.80 0.95 1 0.88 0.44 0.08 0.01
+/musr/command materialPropertiesTable optScintMPT SCINTILLATIONYIELD 0 9167.
+/musr/command materialPropertiesTable optScintMPT RESOLUTIONSCALE    0 1.0
+/musr/command materialPropertiesTable optScintMPT FASTTIMECONSTANT   0 1.32
+/musr/command materialPropertiesTable optScintMPT FASTSCINTILLATIONRISETIME 0 0.063
+#/musr/command materialPropertiesTable optScintMPT SLOWTIMECONSTANT   0 1.6
+/musr/command materialPropertiesTable optScintMPT YIELDRATIO         0 1.0
+/musr/command setMaterialPropertiesTable optScintMPT G4_PLASTIC_SC_VINYLTOLUENE
+#
+#  AIR
+/musr/command materialPropertiesTable    optAIR_MPT ABSLENGTH         2   2.0e-6 4.5e-6 0.001 0.001
+/musr/command materialPropertiesTable    optAIR_MPT RINDEX            2   2.0e-6 4.5e-6 1.0003 1.0003
+/musr/command setMaterialPropertiesTable optAIR_MPT G4_AIR
+#
+#  OPTICAL BOUNDARY:  SCINTILLATOR -> AIR
+#/musr/command materialPropertiesTable airWrap1 REFLECTIVITY     2  2.0e-6 4.5e-6  1.0 1.0
+#/musr/command materialPropertiesTable airWrap1 EFFICIENCY       2  2.0e-6 4.5e-6  0. 0.
+#/musr/command materialPropertiesTable airWrap1 
+#/musr/command opticalSurface airBoundary1 phys_scintFarAwayC1 phys_World dielectric_dielectric polished unified airWrap1
+/musr/command opticalSurface airBoundary1 phys_scintFarAwayC1 phys_World dielectric_dielectric polishedteflonair LUT
+
+#  OPTICAL BOUNDARY:  SCINTILLATOR -> AIR
+#/musr/command materialPropertiesTable airWrap2 REFLECTIVITY     2  2.0e-6 4.5e-6  1.0 1.0
+#/musr/command materialPropertiesTable airWrap2 EFFICIENCY       2  2.0e-6 4.5e-6  0. 0.
+/musr/command opticalSurface airBoundary2 phys_scintFarAwayC2 phys_World dielectric_dielectric polishedteflonair LUT
+#
+#  OPTICAL BOUNDARY:  SCINTILLATOR -> APD 1
+/musr/command materialPropertiesTable apdWrapping1 REFLECTIVITY     2  2.0e-6 4.5e-6  0.0 0.0
+/musr/command materialPropertiesTable apdWrapping1 EFFICIENCY       2  2.0e-6 4.5e-6  0.25 0.25
+/musr/command opticalSurface APDsurface phys_scintFarAwayC1 phys_APD1 dielectric_metal polished LUT apdWrapping1
+#
+#  OPTICAL BOUNDARY:  SCINTILLATOR -> APD 2
+/musr/command materialPropertiesTable apdWrapping2 REFLECTIVITY     2  2.0e-6 4.5e-6  0.0 0.0
+/musr/command materialPropertiesTable apdWrapping2 EFFICIENCY       2  2.0e-6 4.5e-6  0.25 0.25
+/musr/command opticalSurface APDsurface phys_scintFarAwayC2 phys_APD2 dielectric_metal polished LUT apdWrapping2
+#
+#
+/musr/command OPSA signalSeparationTime 1000
+#/musr/command OPSA eventsForOPSAhistos -2 0
+/musr/command OPSA OPSAhist 1000 0. 10.
+/musr/command OPSA pulseShapeArray APDpulseShapeFile_2011_1e_Z.txt
+/musr/command OPSA CFD -0.2 0.4 -1.8
+/musr/command OPSA APDcells 1 60 60 0.1 1.5 1.5
+/musr/command OPSA photonFractions 0.01 0.05 0.5 0.2
+/musr/command OPSA SetAPDcellsTimeVariationSigma 0.1
+###################################################################################
+#########################  P H Y S I C S      P R O C E S S E S  ##################
+###################################################################################
+# Geant 4.9.4
+/musr/command process addDiscreteProcess gamma G4PhotoElectricEffect
+/musr/command process addDiscreteProcess gamma G4ComptonScattering
+/musr/command process addDiscreteProcess gamma G4GammaConversion
+/musr/command process addDiscreteProcess gamma G4RayleighScattering
+/musr/command process addDiscreteProcess opticalphoton G4OpAbsorption
+/musr/command process addDiscreteProcess opticalphoton G4OpRayleigh
+/musr/command process addDiscreteProcess opticalphoton G4OpBoundaryProcess
+#/musr/command process addDiscreteProcess opticalphoton G4OpWLS
+/musr/command process addProcess         e-    G4eMultipleScattering    -1  1  1
+/musr/command process addProcess         e-    G4eIonisation            -1  2  2
+/musr/command process addProcess         e-    G4eBremsstrahlung        -1  3  3
+/musr/command process addProcess         e-    G4Scintillation           4 -1  4
+/musr/command process addProcess         e+    G4eMultipleScattering    -1  1  1
+/musr/command process addProcess         e+    G4eIonisation            -1  2  2
+/musr/command process addProcess         e+    G4eBremsstrahlung        -1  3  3
+/musr/command process addProcess         e+    G4eplusAnnihilation       0 -1  4
+/musr/command process addProcess         e+    G4Scintillation           5 -1  5
+#/musr/command process addProcess         mu-   G4MuMultipleScattering   -1  1  1
+#/musr/command process addProcess         mu-   G4MuIonisation           -1  2  2
+#/musr/command process addProcess         mu-   G4MuBremsstrahlung       -1  3  3
+#/musr/command process addProcess         mu-   G4MuPairProduction       -1  4  4
+#/musr/command process addProcess         mu-   G4Scintillation           5 -1  5
+#/musr/command process addProcess         mu+   G4MuMultipleScattering   -1  1  1
+#/musr/command process addProcess         mu+   G4MuIonisation           -1  2  2
+#/musr/command process addProcess         mu+   G4MuBremsstrahlung       -1  3  3
+#/musr/command process addProcess         mu+   G4MuPairProduction       -1  4  4
+#/musr/command process addProcess         mu+   G4Scintillation           5 -1  5
+#
+#
+###/home/install/geant4.9.3/source/processes/electromagnetic/utils/src/G4EnergyLossMessenger.cc
+######## /process/msc/StepLimit Minimal | UseDistanceToBoundary | UseSafety 
+#/process/msc/StepLimit UseSafety
+###/process/msc/LateralDisplacement
+#/process/msc/RangeFactor 0.04
+#/process/msc/GeomFactor 2.5
+###/process/msc/FactorForAngleLimit
+#/process/msc/Skin 3.0
+###/process/msc/ThetaLimit 0.2 rad
+###################################################################################
+##################  S O M E   O T H E R    P A R A M E T E R S   ##################
+###################################################################################
+#/musr/command rootOutputDirectoryName /home/sedlak/simData
+# Store all events into the ROOT tree or just the interesting ones ? (true is default)
+#/musr/command storeOnlyEventsWithHits false
+#/musr/command storeOnlyEventsWithHitInDetID 11
+# Set the minimum time separation between two subsequent signals in the same detector (in ns)
+/musr/command signalSeparationTime 50
+#
+/musr/command maximumRunTimeAllowed 400000
+/musr/run/howOftenToPrintEvent 1
+/musr/run/randomOption 2
+# Use optical photons:
+/musr/command G4OpticalPhotons true
+#/tracking/verbose 5
+#/process/verbose 5
+###################################################################################
+#########################   R O O T     O U T P U T  ##############################
+###################################################################################
+#/musr/command rootOutput runID off
+#/musr/command rootOutput eventID off
+/musr/command rootOutput weight off
+/musr/command rootOutput BFieldAtDecay off
+/musr/command rootOutput muIniPosX off
+/musr/command rootOutput muIniPosY off
+/musr/command rootOutput muIniPosZ off
+/musr/command rootOutput muIniMomX off
+/musr/command rootOutput muIniMomY off
+/musr/command rootOutput muIniMomZ off
+/musr/command rootOutput muIniPolX off
+/musr/command rootOutput muIniPolY off
+/musr/command rootOutput muIniPolZ off
+/musr/command rootOutput muIniTime off
+/musr/command rootOutput muDecayDetID off
+/musr/command rootOutput muDecayPosX off
+/musr/command rootOutput muDecayPosY off
+/musr/command rootOutput muDecayPosZ off
+/musr/command rootOutput muDecayTime off
+/musr/command rootOutput muDecayPolX off
+/musr/command rootOutput muDecayPolY off
+/musr/command rootOutput muDecayPolZ off
+/musr/command rootOutput muTargetTime off
+/musr/command rootOutput muTargetPolX off
+/musr/command rootOutput muTargetPolY off
+/musr/command rootOutput muTargetPolZ off
+/musr/command rootOutput muM0Time off
+/musr/command rootOutput muM0PolX off
+/musr/command rootOutput muM0PolY off
+/musr/command rootOutput muM0PolZ off
+/musr/command rootOutput muM1Time off
+/musr/command rootOutput muM1PolX off
+/musr/command rootOutput muM1PolY off
+/musr/command rootOutput muM1PolZ off
+/musr/command rootOutput muM2Time off
+/musr/command rootOutput muM2PolX off
+/musr/command rootOutput muM2PolY off
+/musr/command rootOutput muM2PolZ off
+#/musr/command rootOutput posIniMomX off
+#/musr/command rootOutput posIniMomY off
+#/musr/command rootOutput posIniMomZ off
+/musr/command rootOutput fieldNomVal off
+#/musr/command rootOutput det_ID off
+#/musr/command rootOutput det_edep off
+/musr/command rootOutput det_edep_el off
+/musr/command rootOutput det_edep_pos off
+/musr/command rootOutput det_edep_gam off
+/musr/command rootOutput det_edep_mup off
+#/musr/command rootOutput det_nsteps off
+#/musr/command rootOutput det_length off
+#/musr/command rootOutput det_start off
+#/musr/command rootOutput det_end off
+#/musr/command rootOutput det_x off
+#/musr/command rootOutput det_y off
+#/musr/command rootOutput det_z off
+#/musr/command rootOutput det_kine off
+/musr/command rootOutput det_VrtxKine off
+/musr/command rootOutput det_VrtxX off
+/musr/command rootOutput det_VrtxY off
+/musr/command rootOutput det_VrtxZ off
+/musr/command rootOutput det_VrtxVolID off
+/musr/command rootOutput det_VrtxProcID off
+/musr/command rootOutput det_VrtxTrackID off
+/musr/command rootOutput det_VrtxParticleID off
+/musr/command rootOutput det_VvvKine off
+/musr/command rootOutput det_VvvX off
+/musr/command rootOutput det_VvvY off
+/musr/command rootOutput det_VvvZ off
+/musr/command rootOutput det_VvvVolID off
+/musr/command rootOutput det_VvvProcID off
+/musr/command rootOutput det_VvvTrackID off
+/musr/command rootOutput det_VvvParticleID off
+### Root variables that are not written out by default, but can be switched on:
+#/musr/command rootOutput fieldIntegralBx on
+#/musr/command rootOutput fieldIntegralBy on
+#/musr/command rootOutput fieldIntegralBz on
+#/musr/command rootOutput fieldIntegralBz1 on
+#/musr/command rootOutput fieldIntegralBz2 on
+#/musr/command rootOutput fieldIntegralBz3 on
+###################################################################################
+#########################  V I S U A L I S A T I O N ##############################
+###################################################################################
+/vis/disable
+#/control/execute visFromToni.mac
+#/control/execute visDawn1.mac
+#/control/execute visVRML201.mac
+###################################################################################
+######################### P A R T I C L E   G U N #################################
+###################################################################################
+/gun/primaryparticle e-
+/gun/vertex 0 0 0 mm
+/gun/momentum 2.15 MeV
+########################  B E A M    O N  #######################################
+/run/beamOn 20
+#/run/beamOn 5000000
diff --git a/run/APDpulseShapeFile_2011_1e_Z.txt b/run/APDpulseShapeFile_2011_1e_Z.txt
new file mode 100644
index 0000000..eba35ff
--- /dev/null
+++ b/run/APDpulseShapeFile_2011_1e_Z.txt
@@ -0,0 +1,10006 @@
+% This is the file that contains responce function (pulse shape)
+% of a single cell (single photon) detected by G-APD
+% (Hamamatsu MPPC S10362-33-050) measured by Alexey Stoykov for
+% 84 single electron events and averaged later on.
+% Measurement was done on 14.3.2011
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diff --git a/run/visDawn101.mac b/run/visDawn101.mac
index a314f71..b735c59 100644
--- a/run/visDawn101.mac
+++ b/run/visDawn101.mac
@@ -23,7 +23,7 @@
 
 # Configure the viewer (optional)
 #/vis/viewer/set/viewpointThetaPhi 235 -45
-/vis/viewer/set/viewpointThetaPhi  80 190
+/vis/viewer/set/viewpointThetaPhi  80 30
 #/vis/viewer/set/lightsThetaPhi    120  60 
 #/vis/viewer/set/hiddenEdge        true
 /vis/viewer/set/style             surface
diff --git a/run/visDawn102.mac b/run/visDawn102.mac
new file mode 100644
index 0000000..b735c59
--- /dev/null
+++ b/run/visDawn102.mac
@@ -0,0 +1,70 @@
+# This is a macro file for visualizing G4 events.
+# It can either be included in another macro or called with /control/exec vis.mac
+
+# Create an OpenGL driver (i.e. a scene handler and viewer)
+# Some useful choices: VRML2FILE, OGLSX, OGLIX, DAWNFILE, etc.
+#/vis/open VRML2FILE
+#*/vis/open OGLIX 600x600-0+0
+/vis/open DAWNFILE
+
+# To calculate volumes and masses uncomment the next two lines
+#*/vis/open ATree 
+#*/vis/ASCIITree/verbose 4
+
+
+# Create a new empty scene and attach it to handler
+/vis/scene/create
+
+# Add world volume, trajectories and hits to the scene
+/vis/scene/add/volume
+/vis/scene/add/trajectories
+/vis/scene/add/hits
+/vis/sceneHandler/attach
+
+# Configure the viewer (optional)
+#/vis/viewer/set/viewpointThetaPhi 235 -45
+/vis/viewer/set/viewpointThetaPhi  80 30
+#/vis/viewer/set/lightsThetaPhi    120  60 
+#/vis/viewer/set/hiddenEdge        true
+/vis/viewer/set/style             surface
+/vis/viewer/zoom 0.8
+# Style: s - surface, w - wireframe
+# Note: "surface style" and "hiddenEdge true" remove transparency!
+# Other viewpoints (25 55) (235 -45) (125 35)
+
+
+# Store trajectory information for visualisation (set to 0 if too many tracks cause core dump)
+/tracking/storeTrajectory 1
+
+#At the end of each event (default behaviour)
+#/vis/scene/endOfEventAction refresh
+#At the end of run of X events - Data from X events will be superimposed
+#cks 
+#/vis/scene/endOfEventAction accumulate
+#At the end of Y runs - Data from Y runs will be superimposed
+#/vis/scene/endOfRunAction accumulate
+
+# Coloured trajectories for an easier particle identification:
+# PDG IDs and colours: e- 11 red, e+ -11 blue, nu_e 12 yellow, 
+#         mu+ -13 magenta, anti_nu_mu -14 green, gamma 22 grey
+# 
+#/vis/modeling/trajectories/create/drawByCharge
+#/vis/modeling/trajectories/drawByCharge-0/set 1 cyan
+
+/vis/modeling/trajectories/create/drawByParticleID
+#*/vis/modeling/trajectories/drawByParticleID-0/set gamma grey
+#/vis/modeling/trajectories/drawByParticleID-0/setRGBA gamma 1 1 1 0
+/vis/modeling/trajectories/drawByParticleID-0/setRGBA mu+   1 0 0   1
+/vis/modeling/trajectories/drawByParticleID-0/setRGBA e+    0 0 1   1
+/vis/modeling/trajectories/drawByParticleID-0/setRGBA gamma 0 1 0   1
+/vis/modeling/trajectories/drawByParticleID-0/setRGBA e-    1 0 1   1
+/vis/modeling/trajectories/drawByParticleID-0/setRGBA nu_e       1 1 1 0 1
+/vis/modeling/trajectories/drawByParticleID-0/setRGBA anti_nu_mu 1 1 1 0.5
+#/vis/modeling/trajectories/drawByParticleID-0/set nu_e white
+#/vis/modeling/trajectories/drawByParticleID-0/set anti_nu_mu white
+
+# Verbosity of hits
+#/hits/verbose 2
+
+# Output just the detector geometry
+/vis/viewer/flush
diff --git a/run/vis_201.mac b/run/vis_201.mac
index eaeefb1..a03f104 100644
--- a/run/vis_201.mac
+++ b/run/vis_201.mac
@@ -61,7 +61,7 @@
 #/musr/command construct box KoincB2   20   90   2.5 G4_PLASTIC_SC_VINYLTOLUENE     -33  0  -60   log_World matrix3   musr/ScintSD 22
 # --- M0 ---
 /musr/command construct box M0         5    5   1.0 G4_PLASTIC_SC_VINYLTOLUENE       0  0  -46   log_World matrix4   musr/ScintSD 102
-/musr/command construct GPDmHolder GPDmHolder  5 25 1.0 G4_PLASTIC_SC_VINYLTOLUENE   0 -25 -46   log_World   norot   dead         103
+#/musr/command construct GPDmHolder GPDmHolder  5 25 1.0 G4_PLASTIC_SC_VINYLTOLUENE   0 -25 -46   log_World   norot   dead         103
 # --- Magnet ---
 #/musr/command construct tubs Magnet1  180  375 78 0 360 G4_Cu                         133 0 0   log_World matrix5   dead         291
 #/musr/command construct tubs Magnet2  180  375 78 0 360 G4_Cu                        -133 0 0   log_World matrix5   dead         292
@@ -81,10 +81,12 @@
 #/musr/command visattributes log_GPDsampleHolderE red
 #/musr/command visattributes log_GPDsampleHolderF red
 #/musr/command visattributes log_GPDsampleHolderG red
-/musr/command visattributes log_GPDcollimator magenta
-/musr/command visattributes log_Firstcollimator magenta
-/musr/command visattributes log_SecondCollimator magenta
-/musr/command visattributes log_GPDmHolder magenta
+/musr/command visattributes log_GPDcollimator green
+/musr/command visattributes log_Firstcollimator green
+/musr/command visattributes log_Firstcollimatorhole green
+/musr/command visattributes log_SecondCollimator green
+/musr/command visattributes log_SecondCollHole green
+#/musr/command visattributes log_GPDmHolder magenta
 #/musr/command visattributes log_target blue
 /musr/command visattributes log_M0 red
 #/musr/command visattributes G4_Pb blue
diff --git a/src/musrDetectorConstruction.cc b/src/musrDetectorConstruction.cc
index 381b795..567970b 100644
--- a/src/musrDetectorConstruction.cc
+++ b/src/musrDetectorConstruction.cc
@@ -1187,6 +1187,8 @@ G4VPhysicalVolume* musrDetectorConstruction::Construct()  {
 	  if (strcmp(tmpString2,"odet_timeD")==0)    {musrRootOutput::store_odet_timeD = false;}
 	  if (strcmp(tmpString2,"odet_timeMean")==0) {musrRootOutput::store_odet_timeMean = false;}
 	  if (strcmp(tmpString2,"odet_timeLast")==0) {musrRootOutput::store_odet_timeLast = false;}
+	  if (strcmp(tmpString2,"odet_timeCFD")==0)  {musrRootOutput::store_odet_timeCFD = false;}
+	  if (strcmp(tmpString2,"odet_amplCFD")==0)  {musrRootOutput::store_odet_amplCFD = false;}
 	}
 	else if(strcmp(storeIt,"on")==0) {
 	  if (strcmp(tmpString2,"fieldIntegralBx")==0){musrRootOutput::store_fieldIntegralBx = true;}
@@ -1195,6 +1197,7 @@ G4VPhysicalVolume* musrDetectorConstruction::Construct()  {
 	  if (strcmp(tmpString2,"fieldIntegralBz1")==0){musrRootOutput::store_fieldIntegralBz1 = true;}
 	  if (strcmp(tmpString2,"fieldIntegralBz2")==0){musrRootOutput::store_fieldIntegralBz2 = true;}
 	  if (strcmp(tmpString2,"fieldIntegralBz3")==0){musrRootOutput::store_fieldIntegralBz3 = true;}
+	  if (strcmp(tmpString2,"odet_timeCFDarray")==0){musrRootOutput::store_odet_timeCFDarray = true;}
 
 	  if ((musrRootOutput::store_fieldIntegralBx)||(musrRootOutput::store_fieldIntegralBy)||
 	      (musrRootOutput::store_fieldIntegralBz)||(musrRootOutput::store_fieldIntegralBz1)||
diff --git a/src/musrRootOutput.cc b/src/musrRootOutput.cc
index 02da927..b6e4c20 100644
--- a/src/musrRootOutput.cc
+++ b/src/musrRootOutput.cc
@@ -160,7 +160,7 @@ G4bool musrRootOutput::store_odet_timeMean = true;
 G4bool musrRootOutput::store_odet_timeLast = true;
 G4bool musrRootOutput::store_odet_timeCFD = true;
 G4bool musrRootOutput::store_odet_amplCFD = true;
-
+G4bool musrRootOutput::store_odet_timeCFDarray = false;
 
 G4int musrRootOutput::oldEventNumberInG4EqEMFieldWithSpinFunction=-1;
 
@@ -301,7 +301,73 @@ void musrRootOutput::BeginOfRunAction() {
   if (store_odet_timeLast)    {rootTree->Branch("odet_timeLast",&odet_timeLast,"odet_timeLast[odet_n]/D");}
   if (store_odet_timeCFD)     {rootTree->Branch("odet_timeCFD",&odet_timeCFD,"odet_timeCFD[odet_n]/D");}
   if (store_odet_amplCFD)     {rootTree->Branch("odet_amplCFD",&odet_amplCFD,"odet_amplCFD[odet_n]/D");}
-
+  if (store_odet_timeCFDarray)     {
+    rootTree->Branch("odet_timeCFD100",&odet_timeCFD100,"odet_timeCFD100[odet_n]/D");
+    rootTree->Branch("odet_timeCFD101",&odet_timeCFD101,"odet_timeCFD101[odet_n]/D");
+    rootTree->Branch("odet_timeCFD102",&odet_timeCFD102,"odet_timeCFD102[odet_n]/D");
+    rootTree->Branch("odet_timeCFD103",&odet_timeCFD103,"odet_timeCFD103[odet_n]/D");
+    rootTree->Branch("odet_timeCFD104",&odet_timeCFD104,"odet_timeCFD104[odet_n]/D");
+    rootTree->Branch("odet_timeCFD105",&odet_timeCFD105,"odet_timeCFD105[odet_n]/D");
+    rootTree->Branch("odet_timeCFD106",&odet_timeCFD106,"odet_timeCFD106[odet_n]/D");
+    rootTree->Branch("odet_timeCFD107",&odet_timeCFD107,"odet_timeCFD107[odet_n]/D");
+    rootTree->Branch("odet_timeCFD108",&odet_timeCFD108,"odet_timeCFD108[odet_n]/D");
+    rootTree->Branch("odet_timeCFD109",&odet_timeCFD109,"odet_timeCFD109[odet_n]/D");
+    rootTree->Branch("odet_timeCFD110",&odet_timeCFD110,"odet_timeCFD110[odet_n]/D");
+    rootTree->Branch("odet_timeCFD111",&odet_timeCFD111,"odet_timeCFD111[odet_n]/D");
+    rootTree->Branch("odet_timeCFD112",&odet_timeCFD112,"odet_timeCFD112[odet_n]/D");
+    rootTree->Branch("odet_timeCFD200",&odet_timeCFD200,"odet_timeCFD200[odet_n]/D");
+    rootTree->Branch("odet_timeCFD201",&odet_timeCFD201,"odet_timeCFD201[odet_n]/D");
+    rootTree->Branch("odet_timeCFD202",&odet_timeCFD202,"odet_timeCFD202[odet_n]/D");
+    rootTree->Branch("odet_timeCFD203",&odet_timeCFD203,"odet_timeCFD203[odet_n]/D");
+    rootTree->Branch("odet_timeCFD204",&odet_timeCFD204,"odet_timeCFD204[odet_n]/D");
+    rootTree->Branch("odet_timeCFD205",&odet_timeCFD205,"odet_timeCFD205[odet_n]/D");
+    rootTree->Branch("odet_timeCFD206",&odet_timeCFD206,"odet_timeCFD206[odet_n]/D");
+    rootTree->Branch("odet_timeCFD207",&odet_timeCFD207,"odet_timeCFD207[odet_n]/D");
+    rootTree->Branch("odet_timeCFD208",&odet_timeCFD208,"odet_timeCFD208[odet_n]/D");
+    rootTree->Branch("odet_timeCFD209",&odet_timeCFD209,"odet_timeCFD209[odet_n]/D");
+    rootTree->Branch("odet_timeCFD210",&odet_timeCFD210,"odet_timeCFD210[odet_n]/D");
+    rootTree->Branch("odet_timeCFD211",&odet_timeCFD211,"odet_timeCFD211[odet_n]/D");
+    rootTree->Branch("odet_timeCFD212",&odet_timeCFD212,"odet_timeCFD212[odet_n]/D");
+    rootTree->Branch("odet_timeCFD300",&odet_timeCFD300,"odet_timeCFD300[odet_n]/D");
+    rootTree->Branch("odet_timeCFD301",&odet_timeCFD301,"odet_timeCFD301[odet_n]/D");
+    rootTree->Branch("odet_timeCFD302",&odet_timeCFD302,"odet_timeCFD302[odet_n]/D");
+    rootTree->Branch("odet_timeCFD303",&odet_timeCFD303,"odet_timeCFD303[odet_n]/D");
+    rootTree->Branch("odet_timeCFD304",&odet_timeCFD304,"odet_timeCFD304[odet_n]/D");
+    rootTree->Branch("odet_timeCFD305",&odet_timeCFD305,"odet_timeCFD305[odet_n]/D");
+    rootTree->Branch("odet_timeCFD306",&odet_timeCFD306,"odet_timeCFD306[odet_n]/D");
+    rootTree->Branch("odet_timeCFD307",&odet_timeCFD307,"odet_timeCFD307[odet_n]/D");
+    rootTree->Branch("odet_timeCFD308",&odet_timeCFD308,"odet_timeCFD308[odet_n]/D");
+    rootTree->Branch("odet_timeCFD309",&odet_timeCFD309,"odet_timeCFD309[odet_n]/D");
+    rootTree->Branch("odet_timeCFD310",&odet_timeCFD310,"odet_timeCFD310[odet_n]/D");
+    rootTree->Branch("odet_timeCFD311",&odet_timeCFD311,"odet_timeCFD311[odet_n]/D");
+    rootTree->Branch("odet_timeCFD312",&odet_timeCFD312,"odet_timeCFD312[odet_n]/D");
+    rootTree->Branch("odet_timeCFD400",&odet_timeCFD400,"odet_timeCFD400[odet_n]/D");
+    rootTree->Branch("odet_timeCFD401",&odet_timeCFD401,"odet_timeCFD401[odet_n]/D");
+    rootTree->Branch("odet_timeCFD402",&odet_timeCFD402,"odet_timeCFD402[odet_n]/D");
+    rootTree->Branch("odet_timeCFD403",&odet_timeCFD403,"odet_timeCFD403[odet_n]/D");
+    rootTree->Branch("odet_timeCFD404",&odet_timeCFD404,"odet_timeCFD404[odet_n]/D");
+    rootTree->Branch("odet_timeCFD405",&odet_timeCFD405,"odet_timeCFD405[odet_n]/D");
+    rootTree->Branch("odet_timeCFD406",&odet_timeCFD406,"odet_timeCFD406[odet_n]/D");
+    rootTree->Branch("odet_timeCFD407",&odet_timeCFD407,"odet_timeCFD407[odet_n]/D");
+    rootTree->Branch("odet_timeCFD408",&odet_timeCFD408,"odet_timeCFD408[odet_n]/D");
+    rootTree->Branch("odet_timeCFD409",&odet_timeCFD409,"odet_timeCFD409[odet_n]/D");
+    rootTree->Branch("odet_timeCFD410",&odet_timeCFD410,"odet_timeCFD410[odet_n]/D");
+    rootTree->Branch("odet_timeCFD411",&odet_timeCFD411,"odet_timeCFD411[odet_n]/D");
+    rootTree->Branch("odet_timeCFD412",&odet_timeCFD412,"odet_timeCFD412[odet_n]/D");
+    rootTree->Branch("odet_timeCFD500",&odet_timeCFD500,"odet_timeCFD500[odet_n]/D");
+    rootTree->Branch("odet_timeCFD501",&odet_timeCFD501,"odet_timeCFD501[odet_n]/D");
+    rootTree->Branch("odet_timeCFD502",&odet_timeCFD502,"odet_timeCFD502[odet_n]/D");
+    rootTree->Branch("odet_timeCFD503",&odet_timeCFD503,"odet_timeCFD503[odet_n]/D");
+    rootTree->Branch("odet_timeCFD504",&odet_timeCFD504,"odet_timeCFD504[odet_n]/D");
+    rootTree->Branch("odet_timeCFD505",&odet_timeCFD505,"odet_timeCFD505[odet_n]/D");
+    rootTree->Branch("odet_timeCFD506",&odet_timeCFD506,"odet_timeCFD506[odet_n]/D");
+    rootTree->Branch("odet_timeCFD507",&odet_timeCFD507,"odet_timeCFD507[odet_n]/D");
+    rootTree->Branch("odet_timeCFD508",&odet_timeCFD508,"odet_timeCFD508[odet_n]/D");
+    rootTree->Branch("odet_timeCFD509",&odet_timeCFD509,"odet_timeCFD509[odet_n]/D");
+    rootTree->Branch("odet_timeCFD510",&odet_timeCFD510,"odet_timeCFD510[odet_n]/D");
+    rootTree->Branch("odet_timeCFD511",&odet_timeCFD511,"odet_timeCFD511[odet_n]/D");
+    rootTree->Branch("odet_timeCFD512",&odet_timeCFD512,"odet_timeCFD512[odet_n]/D");
+  }
 
   //  htest1 = new TH1F("htest1","The debugging histogram 1",50,-4.,4.);
   //  htest2 = new TH1F("htest2","The debugging histogram 2",50,0.,3.142);
@@ -562,7 +628,74 @@ void musrRootOutput::SetOPSAinfo    (G4int nDetectors, G4int ID, G4int nPhot, G4
     odet_amplCFD[nDetectors]=amplCFD;
   }
 }
-
+//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
+void musrRootOutput::SetCFDSpecialInfo (G4int n, G4double time) {
+  if      (n==100) {odet_timeCFD100[odet_n-1] = time/microsecond;} // G4cout<<"OKKKKK odet_n-1="<<odet_n-1<<G4endl;}
+  else if (n==101) {odet_timeCFD101[odet_n-1] = time/microsecond;}
+  else if (n==102) {odet_timeCFD102[odet_n-1] = time/microsecond;}
+  else if (n==103) {odet_timeCFD103[odet_n-1] = time/microsecond;}
+  else if (n==104) {odet_timeCFD104[odet_n-1] = time/microsecond;}
+  else if (n==105) {odet_timeCFD105[odet_n-1] = time/microsecond;}
+  else if (n==106) {odet_timeCFD106[odet_n-1] = time/microsecond;}
+  else if (n==107) {odet_timeCFD107[odet_n-1] = time/microsecond;}
+  else if (n==108) {odet_timeCFD108[odet_n-1] = time/microsecond;}
+  else if (n==109) {odet_timeCFD109[odet_n-1] = time/microsecond;}
+  else if (n==110) {odet_timeCFD110[odet_n-1] = time/microsecond;}
+  else if (n==111) {odet_timeCFD111[odet_n-1] = time/microsecond;}
+  else if (n==112) {odet_timeCFD112[odet_n-1] = time/microsecond;}
+  else if (n==200) {odet_timeCFD200[odet_n-1] = time/microsecond;}
+  else if (n==201) {odet_timeCFD201[odet_n-1] = time/microsecond;}
+  else if (n==202) {odet_timeCFD202[odet_n-1] = time/microsecond;}
+  else if (n==203) {odet_timeCFD203[odet_n-1] = time/microsecond;}
+  else if (n==204) {odet_timeCFD204[odet_n-1] = time/microsecond;}
+  else if (n==205) {odet_timeCFD205[odet_n-1] = time/microsecond;}
+  else if (n==206) {odet_timeCFD206[odet_n-1] = time/microsecond;}
+  else if (n==207) {odet_timeCFD207[odet_n-1] = time/microsecond;}
+  else if (n==208) {odet_timeCFD208[odet_n-1] = time/microsecond;}
+  else if (n==209) {odet_timeCFD209[odet_n-1] = time/microsecond;}
+  else if (n==210) {odet_timeCFD210[odet_n-1] = time/microsecond;}
+  else if (n==211) {odet_timeCFD211[odet_n-1] = time/microsecond;}
+  else if (n==212) {odet_timeCFD212[odet_n-1] = time/microsecond;}
+  else if (n==300) {odet_timeCFD300[odet_n-1] = time/microsecond;}
+  else if (n==301) {odet_timeCFD301[odet_n-1] = time/microsecond;}
+  else if (n==302) {odet_timeCFD302[odet_n-1] = time/microsecond;}
+  else if (n==303) {odet_timeCFD303[odet_n-1] = time/microsecond;}
+  else if (n==304) {odet_timeCFD304[odet_n-1] = time/microsecond;}
+  else if (n==305) {odet_timeCFD305[odet_n-1] = time/microsecond;}
+  else if (n==306) {odet_timeCFD306[odet_n-1] = time/microsecond;}
+  else if (n==307) {odet_timeCFD307[odet_n-1] = time/microsecond;}
+  else if (n==308) {odet_timeCFD308[odet_n-1] = time/microsecond;}
+  else if (n==309) {odet_timeCFD309[odet_n-1] = time/microsecond;}
+  else if (n==310) {odet_timeCFD310[odet_n-1] = time/microsecond;}
+  else if (n==311) {odet_timeCFD311[odet_n-1] = time/microsecond;}
+  else if (n==312) {odet_timeCFD312[odet_n-1] = time/microsecond;}
+  else if (n==400) {odet_timeCFD400[odet_n-1] = time/microsecond;}
+  else if (n==401) {odet_timeCFD401[odet_n-1] = time/microsecond;}
+  else if (n==402) {odet_timeCFD402[odet_n-1] = time/microsecond;}
+  else if (n==403) {odet_timeCFD403[odet_n-1] = time/microsecond;}
+  else if (n==404) {odet_timeCFD404[odet_n-1] = time/microsecond;}
+  else if (n==405) {odet_timeCFD405[odet_n-1] = time/microsecond;}
+  else if (n==406) {odet_timeCFD406[odet_n-1] = time/microsecond;}
+  else if (n==407) {odet_timeCFD407[odet_n-1] = time/microsecond;}
+  else if (n==408) {odet_timeCFD408[odet_n-1] = time/microsecond;}
+  else if (n==409) {odet_timeCFD409[odet_n-1] = time/microsecond;}
+  else if (n==410) {odet_timeCFD410[odet_n-1] = time/microsecond;}
+  else if (n==411) {odet_timeCFD411[odet_n-1] = time/microsecond;}
+  else if (n==412) {odet_timeCFD412[odet_n-1] = time/microsecond;}
+  else if (n==500) {odet_timeCFD500[odet_n-1] = time/microsecond;}
+  else if (n==501) {odet_timeCFD501[odet_n-1] = time/microsecond;}
+  else if (n==502) {odet_timeCFD502[odet_n-1] = time/microsecond;}
+  else if (n==503) {odet_timeCFD503[odet_n-1] = time/microsecond;}
+  else if (n==504) {odet_timeCFD504[odet_n-1] = time/microsecond;}
+  else if (n==505) {odet_timeCFD505[odet_n-1] = time/microsecond;}
+  else if (n==506) {odet_timeCFD506[odet_n-1] = time/microsecond;}
+  else if (n==507) {odet_timeCFD507[odet_n-1] = time/microsecond;}
+  else if (n==508) {odet_timeCFD508[odet_n-1] = time/microsecond;}
+  else if (n==509) {odet_timeCFD509[odet_n-1] = time/microsecond;}
+  else if (n==510) {odet_timeCFD510[odet_n-1] = time/microsecond;}
+  else if (n==511) {odet_timeCFD511[odet_n-1] = time/microsecond;}
+  else if (n==512) {odet_timeCFD512[odet_n-1] = time/microsecond;}
+}
 
 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 void musrRootOutput::setRootOutputDirectoryName(char dirName[1000]) {
diff --git a/src/musrScintSD.cc b/src/musrScintSD.cc
index 8f691b7..264b486 100644
--- a/src/musrScintSD.cc
+++ b/src/musrScintSD.cc
@@ -688,6 +688,7 @@ void musrScintSD::EndOfEvent_OptiacalPhotons() {
 	  OPSA_timeMean = OPSAhisto->GetMean() + OPSA_timeFirst;
 
 	  // if required, convert the histogram with photon times to histogram of electronic pulse shape
+	  G4double timeCFDarray[1000];
 	  if (bool_pulseShapeExists) {
 	    //	    for (Int_t iBin=1; iBin<=OPSAhistoNbin; iBin++) { // loop over all bins of photon histogram
 	    //	      Double_t photonCount = OPSAhisto ->GetBinContent(iBin);
@@ -703,50 +704,45 @@ void musrScintSD::EndOfEvent_OptiacalPhotons() {
 	    //	    }
 	    if (boolStoreThisOPSAhist) OPSAshape -> Write();
 	    
-	    // Now fill the histogram with the CFD signal
-	    for (Int_t iBin=1; iBin<=OPSAhistoNbin; iBin++) { // loop over all bins of electronic signal histogram
-	      Double_t signalValue = OPSAshape->GetBinContent(iBin);
-	      Double_t xValue      = (iBin-0.5)*OPSAhistoBinWidth;
-	      OPSA_CFD->Fill(xValue,signalValue*OPSA_CFD_a1);
-	      Double_t xValueShifted = xValue + OPSA_CFD_delay;
-	      if (xValueShifted>OPSAhistoMax) continue;   //return if out of range;
-	      OPSA_CFD->Fill(xValueShifted,signalValue);
-	    } 
-	    if (boolStoreThisOPSAhist) OPSA_CFD -> Write();
-	    
-	    // Find the timeCFD from CFD signal
-	    Double_t oldYvalue;
-	    Double_t yValue=-1000;
-	    //	    G4bool   OPSA_CFD_time_found = false;
-	    OPSA_CFD_ampl = OPSA_CFD->GetMaximum();
-	    int binmax = OPSA_CFD->GetMaximumBin();
-	    int binmim = OPSA_CFD->GetMinimumBin();
-	    for (Int_t iBin=binmim; iBin<=binmax; iBin++) { // loop over bins between min and max of CFD histogram
-	      //	      Double_t xValue = (iBin-0.5)*OPSAhistoBinWidth;
-	      Double_t xValue = OPSA_CFD->GetXaxis()->GetBinCenter(iBin);
-	      oldYvalue       = yValue;
-	      yValue          = OPSA_CFD->GetBinContent(iBin);
-	      //	      if (yValue>OPSA_CFD_ampl) OPSA_CFD_ampl=yValue; // find the CFD signal amplitude;
-	      //	      if (xValue < 0.6*OPSA_CFD_delay) continue; // it is believed the CFD signal can not cross y=0 much before the delay time
-	      //	      if ((yValue >= 0)&&(!OPSA_CFD_time_found)) {  // signal just crossed the y=0 axis for the first time ==> record CFD time
-	      if (yValue >= 0) {       // signal just crossed the y=0 axis
-		//		OPSA_CFD_time_found = true;
-		OPSA_CFD_time = xValue - yValue/(yValue-oldYvalue)*OPSAhistoBinWidth;   //linear interpolation
-		OPSA_CFD_time += OPSA_timeFirst - OPSA_CFD_delay + OPSA_CFD_timeShiftOffset;       // correct for 
-		//		G4cout<<"OPSA_CFD_time = "<<OPSA_CFD_time<<G4endl;
-		break;
+
+	    //  If requested, store CFD times for various CFD delays and amplitudes of the reverted signal
+	    if (musrRootOutput::store_odet_timeCFDarray) {
+	      G4double OPSA_CFD_a1_saveThis    = OPSA_CFD_a1;
+	      G4double OPSA_CFD_delay_saveThis = OPSA_CFD_delay;
+	      const int nDelay = 13;
+	      G4double delay[nDelay]={0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 1.0, 1.5, 2.0, 2.5, 3.0, 4.0};
+	      const int nAmpl1 = 5;
+	      G4double ampl1[nAmpl1] = {-0.05, -0.1, -0.2, -0.3, -0.4};
+	      for (Int_t kk=0; kk<nDelay; kk++) {
+		for (Int_t ll=0; ll<nAmpl1; ll++) {
+		  OPSA_CFD_a1    = ampl1[ll];
+		  OPSA_CFD_delay = delay[kk];
+		  FindCFDtime(OPSA_CFD_time, OPSA_CFD_ampl, OPSA_timeFirst);
+		  int index = (ll+1)*100+kk;
+		  if (index<1000) timeCFDarray[(ll+1)*100+kk] = OPSA_CFD_time;
+		  else {G4cout<<"FATALNI ERROR in musrScintSD by calculating (ll+1)*100+kk"<<G4endl;}
+		  //		G4cout<<"   delay= "<<OPSA_CFD_delay<<"  ampl1= "<<OPSA_CFD_a1
+		  //		      <<"  OPSA_CFD_time= "<<OPSA_CFD_time<<"   OPSA_CFD_ampl= "<<OPSA_CFD_ampl<<G4endl;
+		}
 	      }
+	      OPSA_CFD_a1    = OPSA_CFD_a1_saveThis;
+	      OPSA_CFD_delay = OPSA_CFD_delay_saveThis;
 	    }
 
+	    // Now fill the histogram with the CFD signal
+	    FindCFDtime(OPSA_CFD_time, OPSA_CFD_ampl, OPSA_timeFirst);
+	    //	    G4cout<<"OPSA_CFD_time = "<<OPSA_CFD_time<<"   OPSA_CFD_ampl = "<<OPSA_CFD_ampl<<G4endl;
+	    if (boolStoreThisOPSAhist) OPSA_CFD -> Write();
+
 	    // Find the timeC and timeD from the shape histogram
-	    yValue=-1000;
+	    Double_t yValue=-1000;
 	    G4bool   OPSA_C_time_found = false;
 	    G4bool   OPSA_D_time_found = false;
 	    Double_t D_threshold = OPSA_D_threshold * (OPSAshape->GetMaximum());  // covert relative "OPSA_D_threshold" into 
 	                                                                          // the absolute threshold using signal amplitude
 	    for (Int_t iBin=1; iBin<=OPSAhistoNbin; iBin++) { // loop over all bins of CFD histogram
 	      Double_t xValue = (iBin-0.5)*OPSAhistoBinWidth;
-	      oldYvalue       = yValue;
+	      Double_t oldYvalue = yValue;
 	      yValue          = OPSAshape->GetBinContent(iBin);
 	      if ( (yValue>=OPSA_C_threshold) && (!OPSA_C_time_found) ) {  // signal just moved above the threshold
 		OPSA_C_time_found = true;
@@ -777,7 +773,7 @@ void musrScintSD::EndOfEvent_OptiacalPhotons() {
 	  }
 
 	  signalInfo* mySignalInfo = new signalInfo(OPSA_detID,OPSA_nPhot,OPSA_timeFirst,OPSA_timeA,OPSA_timeB,OPSA_timeC,
-						    OPSA_timeD,OPSA_timeMean,OPSA_timeLast,OPSA_CFD_time,OPSA_CFD_ampl);
+						    OPSA_timeD,OPSA_timeMean,OPSA_timeLast,OPSA_CFD_time,OPSA_CFD_ampl,timeCFDarray);
 	  OPSA_signal_Map.insert(std::pair<G4int,signalInfo*>(OPSA_nPhot,mySignalInfo) );
 	}
 	OPSA_nPhot       = 0;
@@ -890,4 +886,35 @@ G4int musrScintSD::FindAPDcellID(G4Step* aStep) {
 		"musrScintSD::FindAPDcellID: APD cell out of range (iz). Wrong dimensions of APD in \"/musr/command OPSA APDcells\" command?",false);
   return in;
 }
+
+//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
+
+void musrScintSD::FindCFDtime(G4double& OPSA_CFD_time, G4double& OPSA_CFD_ampl, G4double timeOfFirstPhoton) {
+  OPSA_CFD->Reset("M");
+  for (Int_t iBin=1; iBin<=OPSAhistoNbin; iBin++) { // loop over all bins of electronic signal histogram
+    Double_t signalValue = OPSAshape->GetBinContent(iBin);
+    Double_t xValue      = (iBin-0.5)*OPSAhistoBinWidth;
+    OPSA_CFD->Fill(xValue,signalValue*OPSA_CFD_a1);
+    Double_t xValueShifted = xValue + OPSA_CFD_delay;
+    if (xValueShifted>OPSAhistoMax) continue;   //return if out of range;
+    OPSA_CFD->Fill(xValueShifted,signalValue);
+  } 
+	    
+  // Find the timeCFD from CFD signal
+  Double_t oldYvalue;
+  Double_t yValue=-1000;
+  OPSA_CFD_ampl = OPSA_CFD->GetMaximum();
+  int binmax = OPSA_CFD->GetMaximumBin();
+  int binmim = OPSA_CFD->GetMinimumBin();
+  for (Int_t iBin=binmim; iBin<=binmax; iBin++) { // loop over bins between min and max of CFD histogram
+    Double_t xValue = OPSA_CFD->GetXaxis()->GetBinCenter(iBin);
+    oldYvalue       = yValue;
+    yValue          = OPSA_CFD->GetBinContent(iBin);
+    if (yValue >= 0) {       // signal just crossed the y=0 axis
+      OPSA_CFD_time = xValue - yValue/(yValue-oldYvalue)*OPSAhistoBinWidth;   //linear interpolation
+      OPSA_CFD_time += timeOfFirstPhoton - OPSA_CFD_delay + OPSA_CFD_timeShiftOffset;       // correct for 
+      break;
+    }
+  }
+}
 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......