Import Geant4 5.0.0 source tree

This commit is contained in:
Gabriele Cosmo
2016-06-08 16:57:27 +02:00
parent 330b82b769
commit 37fff30d2e
5733 changed files with 263867 additions and 74574 deletions
@@ -0,0 +1,12 @@
all: # :::
grep ":::" GNUmakefile
man: # ::: Make manual.
make clean; latex manCascade; bibtex manCascade; latex manCascade; latex manCascade; dvips manCascade.dvi -o manCascade.ps; gv manCascade.ps
pub: # ::: Make publication.
make clean; latex pubCascade; bibtex pubCascade; latex pubCascade; latex pubCascade; dvips pubCascade.dvi -o pubCascade.ps; gv pubCascade.ps
clean: # ::: clean directory
rm -f \#*.*\# \#*\# \#* .*~ .#* *.*~ *~ *.o; rm -f core tmp.txt *.blg *.bbl *.toc *.log *.aux *.dvi
@@ -0,0 +1,4 @@
Main document is manCascade.tex.
Create documentation with 'gmake' or
full release (ps, html and pdf-versions)
with 'gmake release'.
@@ -0,0 +1,226 @@
%%%%%%%%%% espcrc2.sty %%%%%%%%%%
% C(amera) R(eady) C(opy) document-style option. (two-column format).
% Version 2.6: 24 November 1994
% To be used with LaTeX version 2.09 (14 January 1992 or later), or LaTeX2e.
%
%
% Copyright (C) 1992 by Elsevier Science Publishers. All rights reserved.
%
% IMPORTANT NOTICE:
%
% You are not allowed to change this file. You may however copy this file
% to a file with a different name and then change the copy.
%
% You are NOT ALLOWED to distribute this file alone. You are NOT ALLOWED
% to take money for the distribution or use of this file (or a changed
% version) except for a nominal charge for copying etc.
%
% You are allowed to distribute this file under the condition that it is
% distributed together with espcrc2.tex.
%
% If you receive only this file from someone, complain!
%
%
%
% Usage: \documentstyle[twoside,espcrc2]{article}
%
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\def\filedate{24 November 1993}
\typeout{Document-style option `espcrc2' \fileversion \space\space
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% SIDE MARGINS:
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\evensidemargin 4mm % Left margin on even-numbered pages.
% VERTICAL SPACING:
\topmargin 16mm % Nominal distance from top of page to top
% of box containing running head.
\headheight 13mm % No running headline, and no
\headsep 21pt % space between running headline and text.
\footskip 30pt % Baseline-baseline distance between
% running footline and last line of text.
% DIMENSION OF TEXT:
\textheight 202mm % Height of text part of page
\textwidth 160mm % Width of text part of page, i.e of line
\columnsep 10mm % Horizontal space between columns
\columnseprule 0pt % No vertical rule between columns
% PARAGRAPHING
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% SECTIONAL UNITS:
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\def\subsection{\@startsection{subsection}{2}{\z@}
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\def\subsubsection{\@startsection{subsubsection}{3}{\z@}
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\def\subparagraph{\@startsection{subparagraph}{4}{\parindent}
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% at top or bottom of page.
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% text.
% FOOTNOTE
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% EQUATION
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% TITLE
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% \let\thanks\@gobble
\def\thefootnote{\fnsymbol{footnote}}%
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\let\maketitle\relax \let\@maketitle\relax
\gdef\@thanks{}\let\thanks\relax
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\def\@maketitle{% % Actual formatting of \maketitle
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\vskip 8mm % 930715: 8mm white space above title
\raggedright % Front-matter text is ragged right
\hyphenpenalty\@M % and is not hyphenated.
{\Large \@title \par} % Title set in larger font.
\vskip\@bls % One line of vertical space after title.
{\normalsize % each author set in the normal
\@author \par} % typeface size
\vskip\@bls % One line of vertical space after author(s).
\@address % all addresses
\egroup
\twocolumn[% % Front-matter text is over 2 columns.
\unvbox\fm@box % Unwrap contents of front-matter box
\vskip\@bls % add 1 line of vertical space,
\unvbox\abstract@box % unwrap contents of abstract boxes,
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\newcounter{address}
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\def\@makeadmark#1{\hbox{$^{\rm #1}$}}
\def\address#1{\addressmark\begingroup
\xdef\@tempa{\theaddress}\let\\=\relax
\def\protect{\noexpand\protect\noexpand}\xdef\@address{\@address
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\def\@address{}
\def\addressmark{\stepcounter{address}%
\xdef\@tempb{\theaddress}\@makeadmark{\@tempb}}
\def\addresstext#1#2{\leavevmode \begingroup
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% ABSTRACT:
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\def\abstract{%
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\ignorespaces}
\def\endabstract{\par \egroup}
% BIBLIOGRAPHY
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\def\newblock{\hskip 0.11em plus 0.33em minus -0.07em}
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% Collapse citation numbers to ranges.
\newcount\@tempcntc
\def\@citex[#1]#2{\if@filesw\immediate\write\@auxout{\string\citation{#2}}\fi
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{\@ifundefined
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{\setbox\z@\hbox{\global\@tempcntc0\csname b@\@citeb\endcsname\relax}%
\ifnum\@tempcntc=\z@ \@citeo\@tempcntb\m@ne
\@citea\def\@citea{,\penalty\@m}
\hbox{\csname b@\@citeb\endcsname}%
\else
\advance\@tempcntb\@ne
\ifnum\@tempcntb=\@tempcntc
\else\advance\@tempcntb\m@ne\@citeo
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\def\@citeo{\ifnum\@tempcnta>\@tempcntb\else\@citea
\def\@citea{,\penalty\@m}%
\ifnum\@tempcnta=\@tempcntb\the\@tempcnta\else
{\advance\@tempcnta\@ne\ifnum\@tempcnta=\@tempcntb \else
\def\@citea{--}\fi
\advance\@tempcnta\m@ne\the\@tempcnta\@citea\the\@tempcntb}\fi\fi}
% PAGE STYLES
\def\ps@crcplain{\let\@mkboth\@gobbletwo
\def\@oddhead{\reset@font{\sl\rightmark}\hfil \rm\thepage}%
\def\@evenhead{\reset@font\rm \thepage\hfil\sl\leftmark}%
\let\@oddfoot\@empty
\let\@evenfoot\@oddfoot}
% INITIALIZATION
% \twocolumn % Formatting is in 2 columns, with
\sloppy % paragraphs that can be loosely set,
\emergencystretch=1pc % (with 1 pc extra for emergencies),
\flushbottom % and pages of equal length
\ps@crcplain % modified 'plain' page style
@@ -0,0 +1,852 @@
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\title{HETC/INUCL++ manual - System for Modelling Hadronic Intranuclear Processes}
\author{Aatos Heikkinen, Nikita Stepanov
\address{ Helsinki Institute of Physics,
P.O.Box 9,\\
FIN-00014 University of Helsinki, Finland }
}
\begin{document}
\begin{abstract}
HETC/INUCL is a simulation package and a model of intermediate energy nuclear
reactions.
INUCL consists of cascade, fission models, pre-equilibrium, and evaporation
This manual describes the models used in INUCL++.
This documet works as an manual, status report and working document for INUCL project. In accordance with this, we represent results acieved with INUCL. Comparison with measurement is made.
We also descripe staus of Geant4 installation on INUCL software \cite{titarenko99a}.
\end{abstract}
\maketitle
% uncomment main sections when needed
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% declarations for front matter
%\title{HETC/INUCL++ manual - System for Modelling Hadronic Intranuclear Processes}
%\author{Aatos Heikkinen, Nikita Stepanov
%\address{ Helsinki Institute of Physics,
%P.O.Box 9,\\
%FIN-00014 University of Helsinki, Finland }
% }
%\begin{document}
%\begin{abstract}
%HETC/INUCL is a simulation package and a model of intermediate energy nuclear
%reactions.
%INUCL consists of cascade, fission models, pre-equilibrium, and evaporation
%This manual describes the models used in INUCL++.
%This documet works as an manual, status report and working document for INUCL project. In accordance with this, we represent results acieved with INUCL. Comparison with measurement is made.
%We also descripe staus of Geant4 installation on INUCL software \cite{titarenko99a}.
%\end{abstract}
%\maketitle
\section{VOCABULARY}
\begin{itemize}
\item {\it NR} Nuclear reaction
\item {\it quasi-elastic reaction} NR where nucleon can be knocked out of its nuclear.
\item {\it T-nucleus} Target nucleus
\end{itemize}
\section{INTRODUCTION TO INTERMEDIATE-ENERGY NUCLEAR PHYSICS}
Fig :::. Schematic nucleon structure.
The central nucleon is shown as collection of three constituent quarks interacting via the color force.
Closer views show a more complex picture.
At higher energies ($~200~MeV$) energy is high enough to momentarily exite a nucleon into the exited dalta-resonant state ($\Delta$-resonance).
\subsection{Classification of Cross-Sections of NRS}
Let us denote an incident particle and a nucleus under investigation by the symbols $a$ and $A$, respectively.
Following final states following from $a + A$ are possible \cite{iljinov94}:
\begin{itemize}
\item $a + A$ : elastic scattering
\item $a^{*} + A$ : scattering with an exitation of the $a$ particle
\item $a + A^{*}$ : scattering with an exitation of the nucleus
\item $a^{*} + A^{*}$ : scattering in which both the particle and the nucleus are exited
\item $a^{'} + A^{'}$ : reaction involving the production of a new particle and a new nucleus
\item $a^{'} + a^{''} + A^{'}$ : reaction involving the production of two new particles and a new nucleus
\end{itemize}
\subsection{Quantum Formulation of Collision Problem}
\subsubsection{Reaction Channels}
Consider a collision of two complex particles. ::: \cite{iljinov94}
\subsubsection{Transition Probabilities and S-Matrix}
In accordance with general priciples of quantum theory, the probability
::: \cite{iljinov94}
\subsubsection{S-Matrix and Cross-SectionsScattering Amplitude}
::: \cite{iljinov94}
\subsection{Nuclear Structure Phase Diagram}
THe atomic nucleus with its $A$ nucleons is governed by a large number of degrees of freedom.
\subsection{Nuclear density}
Nuclear charge densities are usually well described using present-day effective two-body forces; it is also clear that saturation of the charge dencity indeed occurs.
The central density barely varies when the nucleon number changes.
\subsection{Nuclear radius}
\subsection{Mass formula}
A parametrization of the nuclear binding energy in the groud state,
was first discussed by Bethe, Bacher and Weizs\"{a}cker.
Parametrization conatains volume, surface, Coulomb and symmetry correction terms (we neglegt here typical shell model correction terms) and reads
$$B(E, A) = a_{\nu} A - a_{s} A^{2/3} - a_{c} Z(Z-1)A^{-1/3} -$$
\begin{equation}
a_{A}\frac{(A-2Z)^2}{A}
\end{equation}
Nuclear charge radius turns out to be a rather well-defined quantity.
\subsection{Symmetry consepts in Nuclear Physics}
The nuclear two-body force obeys quite a large number of basic invariances.
Forexample invariance under interchange of the spatial coordinates, translation invariance, Galilean invariance, space reflection symmetry, time reversal invariance, rotation invariance in coordinate space and rotation invariance in charge space (isospin).
The symmetry consept (1932) of isospin symmetry,
describing the charge independence of the nuclear forces by means of the isospin consept with the SU(2) group as the underlying mathematical group was suggested by Heisenberg.
This (simplest of all dynamical symmetries) expresses the invariance of the Hamiltonian under the exchange of all proton and neutron coordinates \cite{heyde98}.
\subsection{Quantum effects}
On the level of the nucleons themselves, invariance of the total nuclear wave functions under the exchange of identical nucleons affects the possible models realized.
The Pauli principle implies antisymmetry for the total fermionic wave function and this has very definite consequences for the types of collective motion that can be set up inside the nucleus.
\subsection{INC-Model}
Widely used semiclassical miscroscopic description of a collision between a particle and a nucleus,
was proposed by Serber \cite{serber47} and Goldberger \cite{goldberger48}.
\section{INTRODUCTION TO INUCL}
\subsection{BACKGROUND}
Originally the INUCL code was published in 1983 \cite{stepanov}.
This code, written with Fortran has been used in [:::] \cite{:::}.
Comprison of results between INCUL and LAHET, CEM95, HETC, CASCADE,
YIELDX, and ALICE code are presented in Refs. \cite{titarenko99a}.
Year 2000 a aroject to implement INUCL into Geant4 hadronic physic
module using C++ wal launched.
New now works also as standalone c++ software called INUCL++.
\subsection{SUMMARY OF INUCL MODEL FEATURES}
\begin{itemize}
\item Originally INUCL was designed as a particle - nucleus interaction simulation block for the particle - target interaction simulation program PHOENIX. It produces an exclusive approach to simulating events with reasonable performance.
\item INUCL is based on N. Stepanov Ph.D. thesis, ITEP, Moscow, 1990.
Also, contribution Vladimir D. Kazaritsky.
\item Now we have standalone F77 based INUCL code and INUCL++ written in C++.
INUCL++ is now written using Geant4 coding style and integration to hadronic models in in progress. Problem: speed is five times slower.
\end{itemize}
\subsubsection{INUCL models}
\begin{itemize}
\item Intranuclear cascade
\item Precompound decay (exiton master equation)
\item Evaporation (Weisskopf - Ewing)
\item Fission (phenomenological model, incorporating some features of the fission statistical model)
\end{itemize}
\subsubsection{Particles treated}
\begin{itemize}
\item Range of targets allowed arbitrary.
\item Range of projectiles allowed p, n, pi and nuclei.
\item From a few Mev to 10 GeV for n, p, pi and up to about 100 MeV / nucleon for nuclei.
\end{itemize}
\subsubsection{Cross sections}
\begin{itemize}
\item Total inelastic cross section has to be taken from outside to normalize all data.
\item Total reaction cross-sections [mbarn] were calculated by J.R. Letaw's formulae
%$45 A^0.7 (1+0.016 sin(5.3-2.63 log10(A)))^(1-0.62 exp(-E / 200) sin(10.9 E^(-0.28)))$
\item Ref.: S. Pearlstein, The Astrophysical Journal, 346: 1049-1060, 1989 November 15
\item Fermi energy calculated in a local density approximation.
\end{itemize}
Nuclear density distribution are derived from the Re(Vopt( r)) distribution. In cascade part, nucleus is divided into a finite number of zones with constant density.
%nuclear radius parameterization: By the definition R(A) is derived from eq. Den(R(A)) = 0.01*Den max
\subsubsection{Nucleon nucleon cross-sections}
\begin{itemize}
\item Parametrizations based on the experimental data (ED) are used.
\item They are energy and isospin dependent.
\item The parameterizations described in ([1] Barashenkov V.S., Toneev V.D. High Energy interactions of particles and nuclei with nuclei. Moscow, 1972
%(in Russian, but there is an English translation)) are used.
\item Pauli exclusion in the INC: Simulated particle-particle interaction is accepted only for secondary nucleons which have $E_n > E_f$.
\item Nuclear density effects are recalculated after each step
\item Cascade is stopped when all the particles, which can escape the nucleus, do it. Then conformity with the energy - conservation law is checked and the given event is accepted, if $E_{exitation} > E_{cut} \approx $a few $MeV$.
\item For nucleons binding energies are calculated using mass formula. For pions Vopt is taken to be constant (about 7 MeV).
\end{itemize}
%What criteria for p-h excitation? is the next phase precompound or compound'? Only pions. The next phase is precompound. Initial conditions are defined during the cascad phase: p -number of "particles", i.e. nucleons, which can not escape the nucleus and have too small interaction probability; h - number of "holes" = number of nuclear nucleons involved in the cascade; energy - momentum of the exiton system derived from the conservation law.
\subsubsection{Precompound phase}
%, describe the PE model used, parameters, i.e., partial state densities, transition rates?
\begin{itemize}
\item Main parameters are taken from (Ribansky I. et al, Nucl.Phys.,1973, A205, p.545 (level densities); Kolbach.C., Z.Phys.,1978, A287, p.319 (matrix elements)).
%(Only N -> N, N -> N + 2, N -> N -2, N -> N - 1 channels are treated.)
\item The angular distribution is isotropic in the frame of rest of the exiton system.
\end{itemize}
%Describe parameters used: level densities, inverse cross-sections or transmission coefficient, choice of optical model parameters if relevant (or reference to source), range of excitations allowed, inclusive or exclusive results? Weisskopf-Ewing evaporation in competition with fission. Emissions of n,p,d,t,He3,He4,gamma is allowed. Level densities derived from exp.data are used. Angular momentum and spin dependence are not included. Other parameters are the same as in ([1], see 5a.) Fermi breakup is allowed onlyin some extreme cases, i.e. for light nuclei and E(exitation) > 3.*Eb. Only the total nuleus decay into neutrons and protons is treated.
\begin{verbatim}
particles p, n, pi, D, T, He3, He4,\gamma
(INUCLN with neutrino 31.3.98)
pion aborption
interaction crosssections
(all data for (N, N) and (pi, N) interactions (dn/dsigma, d3sigma/d3p,
partial multiplicity for npi<=5 error 10-20\%)
pre-equilibrium exiton model
\end{verbatim}
\section{INUCL MANUAL PAGES}
\subsection{Reaction initial state simulation}
\subsubsection{Projectiles and enery range of model}
The GEANT4 INCUL model is cpable to predict final states :::
The allowed allowed bombarding kinetic enery is recommended to be more than
$20~MeV$ in the laboratory frame.
The upper limit of initial kinetic energy is approximately $10~GeV$.
\subsubsection{Nucleus initialization}
\begin{itemize}
\item {\bf Nucleon radii}:
\item {\bf The initial momenta of the nucleons}:
\item {\bf Nucleon binding energy}:
\end{itemize}
\subsection{Random choice of the impact parameter}
The impact parameter $b$ is randomly selected according to
\subsection{Hadron propagation}
\subsection{Selection of particle collisions and particle decays}
\subsection{Hadron interation cross sections}
\subsection{Hadron collision simulation}
\subsubsection{Two-body hadron scattering}
\subsubsection{Angular distribution of two-body hadron scatterings}
\subsubsection{$\pi$-absorption simulation}
\subsection{Resonance decay simulation}
\subsection{Phenomenological potentials}
\subsubsection{The nucleon potential}
\subsection{Pauli blocking simulation}
\subsection{Residual nucleus parameters in the hadron-nucleus collision}
\subsection{Calculation of a residual nucleus exitation energy}
\subsection{Staus of this document}
8.6.02 created by A. Heikkinen
\section{INTRANUCLEAR CASCADE MODEL}
\subsection{NUCLEON DENCITY IN THE ATOM}
Halo nucleus such as $^{11}Li$ are not modelled.
\subsection{IMPULSE DISTRIBUTION}
\subsection{DISTRIBUTION OF POTENTIAL ENERGY}
\subsection{QUANTUM EFFECTS}
Pauli exclusion principle
\subsection{DESCRIPTION OF INC}
\section{FISSION}
\section{PRE-EQUILIBRIUM}
\section{EVAPORATION}
Exited nuclei cools further trough the emission of gamma radiation.
If simulation is detailed,
the emitted gamma rays contain information about the cooling route
and region the nucleus is passing trough.
\section{FROM INUCL TO INUCL++}
\subsection{DESIGN AND ANALYSIS}
We desided to make separate INUCL++ implementations one as an stand
alone with spesific cross-section data and particle definition, and
another iplementation that re-uses Geant4 classes.
So, requirements for the INUCL++ came mainly from Geant4.
Coding style and organization should follow those used in Geant4.
Interace-classes to Geant4 hadronic models define the separation of
cascade, fission, pre-equilibrium, and evaporation. Thus INUCL++
implementation in Geant4 consists of four separate modules.
\subsection{IMPLEMENTATION}
\subsection{TESTING}
Extensive testing :::
Speed comparison :::
\section{INUCL++ AS A STANDALONE PROGRAM}
\section{INUCL++ IN GEANT4}
\section{RESULTS}
We have rewritten INUCL into C++ and tested the performance.
Here we combine INUCL models and HETC INC.
We give here summary of results. Each configuration consists of N=1000 events simulated with same energy etc. parameters.
\subsection{Particle multiplicities}
Multiplities for collisions between $p$ projectile ( $0.5~GeV< E <5.0~GeV$) and aluminium $Al$, iron $Fe$ and lead $Pb$ tragets (at rest) are listed in Figs. \ref{pAlMultiplicity} - \ref{pPbPionMultiplicity}.
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pAlMultiplicity.eps} }
\caption{Particle multiplicities for $(p, ^{27}Al$).}
\label{pAlMultiplicity}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pFeMultiplicity.eps} }
\caption{Particle multiplicities for $(p, ^{56}Fe$).}
\label{pFeMultiplicity}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbMultiplicity.eps} }
\caption{Particle multiplicities for $(p, ^{82}Pb$).}
\label{pPbMultiplicity}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbPionMultiplicity.eps} }
\caption{Pion multiplicities.}
\label{pPbPionMultiplicity}
\end{center}
\end{figure}
\subsection{Particle energies}
Figs. \ref{pPbProtonEnergy} - \ref{p500MeVPbProtonEnergy} give an summary of cascade products energy-levels.
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbProtonEnergy.eps} }
\caption{Average proton energies.}
\label{pPbProtonEnergy}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbNeutronEnergy.eps} }
\caption{Average neutron energies.}
\label{pPbNeutronEnergy}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC pPbNucleonExitation.eps} }
\caption{Average nucleon exitation energy.}
\label{pPbNucleonExitation}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC p50MeVPbProtonEnergy.eps} }
\caption{Proton energy spectrum, when projectile particle (p) had an energy of $0.05~GeV$.}
\label{p50MeVPbProtonEnergy}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC p500MeVPbProtonEnergy.eps} }
\caption{Proton energy spectrum, when projectile particle (p) had an energy of $0.5~GeV$.}
\label{p500MeVPbProtonEnergy}
\end{center}
\end{figure}
\bibliographystyle{unsrt} % Options plain, unsrt, alpha, abbrv
%\bibstyle{plain}
%\begin{thebibliography}{99}
\bibliography{\AATOS texts/references/references.bib}
%\end{thebibliography}
\begin{appendix}
\section{PROJECT plan}
\begin{itemize}
\item we will continue testing INUCL++ against previous verison.
\item we reorganize the code is sutch mannet that integratin to Geant4
is smooth
\item before year 2002 will provide INUCL++ as a stanalone program,
or as an hadronic cascaded modules
(INC, pre-equilibrium, evaporation, fission) in Geant4.
\end{itemize}
\section{UML DIAGRAMS}
Preliminary suggestion for Inucl class interface to Geant4 cascade, pre-equilibrium
and evaporation modules.
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{\PIC cascadeUml.eps} }
\caption{General class structure for Inucl INC model.}
\label{massPb}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{preEquilibriumUml.eps} }
\caption{General class structure for Inucl pre-equilibrium model.}
\label{massPb}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{evaporationUml.eps} }
\caption{General class structure for Inucl evaporation/fission model.}
\label{massPb}
\end{center}
\end{figure}
\section{DOWNLOADING INUCL++}
INUCL++ is downloadable from INUCL homepage at
http://cern.ch/aatos.heikkinen/inucl
\scriptsize
\begin{verbatim}
\end{verbatim}
\normalsize
\section{OVERVIEW OF GEANT4 INUCL ACTIVITIES 2001-2002 }
\subsection{General}
Inside LHC Programme Software and Physics project Geant4 activities are under catecory {\it Simulation and event recosntruction}.
In 2001 HIP joined as participating institute the worl wide Geant4 collaboration with the major responsibility for development and maintenance of the nuclear evaporation and intra-nuclear cascade processes.
Two major codes HETC and INUCL are to be implemented and developed for Geant4 hadronic processes.
The conversion of the hadronic evaporation processes of HETC code to Geant4 was completed in 2001 and good progress was made in the Object-Oriented implementation of the intra-nuclear cascade processes.
For another important nuclear Maonte Carlo code, INUCL, an object oriented model was prepared, containing models for intra-nuclear cascade, pre-equilibrium state, fission and evaporation.
Year 2002 started with implementation of INUCL++ as a standalone software.
A preliminary version of architecture using INUCL++ intra-nuclear model. It also integrates HETC cascades and utilites Geant4 hadronic models frameworks.
\subsection{ABOUT GEANT4}
Geant4 represents one of the largest and most ambitious projects of geographically-distributed software development and large-scale object-oriented systems.
\subsection{COLLABORATION TSB AND CB WORK}
In 2001 HIP joined as participating institute the worl wide Geant4 collaboration with the major responsibility for development and maintenance of the nuclear evaporation and intra-nuclear cascade processes.
Our contribution in TSB and CB will be focused in near future to initiatives and coordination of hadronic cascade framework inside Geant4 hadronic framework.
\subsection{INCUL}
\subsubsection{INTORODUCTION TO INUCL}
INUCL++ is an object oriented implementation of Monte Carlo transport code INUCL for computing the properties of high-energy hadronic cascades in matter.
The functionality of INUCL++ is divided into intranuclear cascade, pre-equilibrium, fission, and evaporation parts.
The stand-alone version INUCL++ is comparable to codes such as HETC and LAHET \cite{titarenko99}.
\subsubsection{INUCL++}
We have made independent version INUCL++ using OO methods.
Architecture of INUCL++ intra-nuclear model plays an important role in our Geant4 work, since we use it also for HETC cascades modelling and as an platform to form a general framework for cascading model.
\subsection{PLANS FOR YEAR 2002}
\begin{itemize}
\item INUCL cascade model introduced to Geant4
\item We also aim to have significant progress on pre-equilibrium, fission models.
\end{itemize}
\begin{figure}
\begin{center}
\leavevmode
\mbox{\epsfxsize=8cm \epsffile{massPb.eps2} }
\caption{::: Pb from 1 GeV .}
\label{massPb}
\end{center}
\end{figure}
\subsection{HIP Geant4 activities 2001-2002}
General:
\begin{itemize}
\item In 2001 HIP joined as participating institute the world wide Geant4 collaboration
\item Responsibility for development and maintenance of the nuclear evaporation and intra-nuclear cascade processes.
\item Two major codes HETC and INUCL are to be implemented and developed for Geant4 hadronic processes.
\end{itemize}
Research activities:
\begin{itemize}
\item Participation to Geant4 TSB and CB meetings
\item The conversion of the hadronic evaporation processes of HETC code to Geant4 was completed in 2001
\item Good progress was made in the Object-Oriented implementation of the intra-nuclear cascade processes
\item An object oriented model of INUCL was prepared, containing models for intra-nuclear cascade, pre-equilibrium state, fission and evaporation
\item Implementation of INUCL++ as a standalone software was finalized
\item Prototype for cascading framework was prepared using experience gained from INUCL OO design
\end{itemize}
Future plans:
\begin{itemize}
\item INUCL cascade model introduced to Geant4
\item Fully integration of HETC intra nuclear cascade -model and Geant4.
\item Significant progress on HETC and INUCL pre-equilibrium and fission models.
\item Introduction of general cascade framework to Geant4 hadronic models
\end{itemize}
\section{SAMPLE RUN RESULT}
\scriptsize
\begin{verbatim}
Number of events 100000
average multiplicity 21.5523
average proton number 3.53569
average neutron number 14.5048
average nucleon Ekin 0.0321547
average proton Ekin 0.0848587
average neutron Ekin 0.0193075
average pion number 0.3036
average pion Ekin 0.132491
average pi+ 0.1165
average pi- 0.058
average pi0 0.1291
average A 126.891
average Z 53.1615
average Exitation Energy 0.0258312
average num of fragments 1.69988
fission prob. 0.0117 c.sec 20.592
=====================================================
********** Izotop analysis ******************
++++++++++++++++++++++++++++++++++++++++++++++++++++++++
**** izotop Z **** 0
A 1 exp.cs 33520 err 12.4
sim. cs 30536.4 err 23.1827
ratio 0.910989 err 0.000769346
simulated production rate 17.3502
A 0 exp.cs 217.4 err 1.22
sim. cs 256.749 err 2.12574
ratio 1.181 err 0.0118124
simulated production rate 0.14588
not found in simulations 0
not found in exper: 0
simulated production rate 17.3502
simulated production rate 0.14588
matched 2 CHSQ 58.3536
raw chsq 13620.6
average ratio 1.04599 err 0.00629088
lhood 1.14436
exper. cs 33737.4 err 13.62
inucl. cs 30793.1 err 25.3085
++++++++++++++++++++++++++++++++++++++++++++++++++++++++
++++++++++++++++++++++++++++++++++++++++++++++++++++++++
**** izotop Z **** 1
A 1 exp.cs 7645 err 6.08
sim. cs 6801.24 err 10.9408
ratio 0.889632 err 0.00159645
simulated production rate 3.86434
A 0 exp.cs 109.4 err 0.96
sim. cs 226.195 err 1.99525
ratio 2.0676 err 0.0257258
simulated production rate 0.12852
not found exper.: A 2 exp.cs 658.7 err 4.2
not found exper.: A 3 exp.cs 338.6 err 3.1
not found in simulations 2
not found in exper: 0
simulated production rate 3.86434
simulated production rate 0.12852
matched 2 CHSQ 40.3162
raw chsq 6501.58
average ratio 1.47862 err 0.0136611
lhood 1.68244
exper. cs 8751.7 err 14.34
inucl. cs 7027.43 err 12.9361
\end{verbatim}
\normalsize
\section{WORKING DOCUMENT}
\subsection{15.7.2002}
\subsection{11.7.2002}
Now platform is ready. G4 and subcodes are organized and compiles. It is time to do actual interface.
Plan for today work 13-15 and 17-20. Build solid understanding of interface. And build it using tests.
\begin{itemize}
\item to do: ApplyYout self seciton CascadeInterfaceen, koncretic conversion between system nucleust and particles, study more interfacing, write towards working interface
\item KineticTrack is starting point for us.
\item Study G4VIntraNuclearTransport (base class G4HadronicInteraction, G4KineticTrack, G4VParticleChange, G4ReactionProductVector) class. And kinetic model. G4TheoFSGenerator steers the collaboration between hadronic generator and intra-nuclear transport
\item Methods in CascadeInteface : {\tt G4VParticleChange* ApplyYourself(const G4Track\& aTrack, G4Nucleus\& theNucleus);
G4ReactionProductVector* Propagate(G4KineticTrackVector* theSecondaries, G4V3DNucleus* theNucleus);} G4ReactionProductVector ok also for G4VParticleChange
\item For use of ApplyYourself see G4PreCompoundModel
\item
\end{itemize}
\subsection{10.7.2002}
\begin{itemize}
\item {\bf}: localised files (inucl cascade code at {\tt html/inucl/inucl++/demo},
hetc code at {\tt html/geant4/geant4/source/processes/ hadronic/models/cascade/cascade},
documentation {\tt html/inucl/doc}).
There is also another g4 version at {\tt html/geant4/geant4.3.1 })
\item studied g4 hadronic cascade interface.
\item {\bf all code and documentation in one place} {\tt html/geant4/geant4/source/processes/ hadronic/models/cascade/cascade}
\item general plan: {\bf thursday} put cascade code to g4 installation (+), make compile (+), study interface structure (+), make small testing (+),
{\bf friday} create real interface,
{\bf sunday} create inteface, and test basics (modify test13 hadronic testing)
{\bf monday morning at 8} co g4 at cern, pack {\tt hadronic/models/cascade}, replace cascade files, add new ones, and commit. Mail hpw. Start holiday at 10 am.
\item cascading basic structure: {\tt G4Collider (base),
G4ElementaryParticlCollider,
G4IntraNucleiCollider (:G4Collider, has G4ElementaryParticlCollider, ),
G4NucleiModel (initializes cascade,zones, boundary trasitions, fermi energy, density, potential),
G4InucleNuclei/G4HETCNuclei (A, Z, kinetic energy, mass formula, exiton configuration) }
\item change G4vector to vector:
\item {\tt G4InuclCollider} does the lining of different models inside collision with method command {\tt collide(bull, targ)}
\item {\tt G4IntraNucleiCascader} does the actual cascading. I starts by setting elementary particel cascader {\tt G4IntraNucleiCascader* incascader-> setElementaryParticleCollider( G4ElementaryParticleCollider*)}
\item The actual cascading is then done: {\tt theIntraNucleiCascader-> collide(\&nbullet, \&ntarget);}
\item finally, laboratory frame change, and some other organizational things happen
\item g4 inc base class is defined in models/generator/ management/include/ G4VIntraNuclearTransportModel.hh
\item INC model is set by G4TheoFSGenerator (: public G4HadronicInteraction) by method: {\tt void SetTransport( G4VIntraNuclearTransportModel *const value);}
\end{itemize}
\subsection{10.6.2002}
\begin{itemize}
\item {\bf compilation}: made compilation faster (now takes 45 seconds) by tunig compiler setting and include-statements
\item {\bf sample run}: result from original C++ test are saved to this document as sample run.
\item {\bf compilation}: fixed writing errors, so code now compiles
\item {\bf manual pages}: tempalte for manual pages copied to this document from GEANT4 ninematic model manual
\end{itemize}
\subsection{7.6.2002}
\begin{itemize}
\item {\bf document template}: Added new style and collected material to this documet. Rethinking chapter organization.
\item {\bf picture rezise}: {\tt convert x.ps x.eps2}
\item {\bf new references}: Some text added fron new sources
\end{itemize}
\end{appendix}
%\end{document}
% end of file
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{0 LineSpace PageHeight { /i exch def 0 i MyMatrix itransform moveto PageWidth i MyMatrix idtransform lineto } for stroke } def
/HS_VERT
{0 LineSpace PageWidth { /i exch def i 0 MyMatrix itransform moveto i PageHeight MyMatrix idtransform lineto } for stroke } def
/HS_CROSS
{ HS_HORIZ HS_VERT } def
/HS_FDIAG
{0 PageHeight sub LineSpace 3.5 mul PageWidth
{ /i exch def i 0 MyMatrix itransform moveto i PageHeight add PageHeight
MyMatrix idtransform lineto } for stroke } def
/HS_BDIAG
{0 LineSpace 3.5 mul PageWidth PageHeight add
{ /i exch def i 0 MyMatrix itransform moveto i PageHeight sub
PageHeight MyMatrix idtransform lineto } for stroke } def
/HS_DIAGCROSS
{ HS_FDIAG HS_BDIAG } def
/StrokeWithPen
{/join exch def /Penwidth PenArray lpWidth get def
Penwidth setlinewidth
Penwidth 1 le
{ 0 setlinecap }
{ Penwidth 5 gt { 1 setlinecap } { 2 setlinecap } ifelse } ifelse
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{ Penwidth 8 gt { 1 setlinejoin } { 2 setlinejoin } ifelse } ifelse } if
join LineJoin -1 ne and {SetLineJoin setlinejoin} if
join MiterLimit -1 ne and {MiterLimit miterlimit} if
PenArray lpRed get 255 div PenArray lpGreen get 255 div PenArray lpBlue get 255 div setrgbcolor
/PenStyle PenArray lpStyle get def
PenStyle 5 lt { PenDashArray PenStyle get 0 setdash stroke }
{ PenStyle 6 eq { [] 0 setdash stroke } {newpath} ifelse } ifelse
join {0 setlinejoin 10 setmiterlimit} if } def
/FillWithBkColor
{ gsave BkColorArray bkRed get 255 div
BkColorArray bkGreen get 255 div BkColorArray bkBlue get
255 div setrgbcolor fill grestore } def
/FillWithBrush
{/BrushStyle BrushArray lbStyle get def
BrushStyle 2 eq dup BrushStyle 0 eq or
{ BrushArray lbRed get 255 div BrushArray lbGreen get 255 div BrushArray lbBlue get 255 div setrgbcolor
{ gsave BkMode 2 eq {FillWithBkColor} if clip
PenArray lpWidth get PenWidthMemo dup 0 ne {div} {pop} ifelse setlinewidth
HatchStyleArray BrushArray lbHatchStyle get get exec
grestore }
{ fill } ifelse }
{BrushStyle 3 eq {BrushArray 5 get p SHR
gsave clip /Tmp save def pfill Tmp restore grestore} {pop}ifelse
} ifelse } def
/Fill&Stroke
{ gsave FillWithBrush grestore StrokeWithPen } def
/patfont 10 dict def patfont begin
/FontType 3 def
/FontMatrix [1 0 0 -1 0 0] def
/FontBBox [0 0 16 16]
def/Encoding StandardEncoding def
/BuildChar{pop pop 16 0 0 0 16 16
setcachedevice 16 16 false [1 0 0 1 .25 .25]{pat}imagemask}bind def
end
/p{/pat 32 string def
{}forall 0 1 7{dup 2 mul pat exch 3 index put dup
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/AU{1 add cvi 15 or}bind def
/AD{1 sub cvi -16 and}bind def
/SHR{pathbbox
AU/Y1 exch def AU/X1 exch def AD/Y0 exch def AD/X0 exch def}bind def
/M /moveto load def
/pfill{/PatFont patfont
definefont setfont/ch(AAAA)def X0 64 X1{Y1 -16 Y0{1 index exch M ch
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/LineTo
{ /y exch def /x exch def
moveto x y lineto currentpoint false StrokeWithPen } def
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/RectanglePath
{
3 index 3 index moveto 3 index 1 index lineto
1 index 1 index lineto 1 index 3 index lineto
3 index 3 index lineto pop pop pop pop closepath} def
/RectanglePathBackwards
{
3 index 3 index moveto 1 index 3 index lineto
1 index 1 index lineto 3 index 1 index lineto
3 index 3 index lineto pop pop pop pop closepath} def
%%EndResource
%%BeginResource: EllipticPath
/EllipticPath
{matrix currentmatrix dup 3 index 6 index sub 2 div
3 index 6 index sub 2 div
7 index 2 index add
7 index 2 index add
matrix translate 3 1 roll matrix scale
exch matrix concatmatrix exch matrix concatmatrix setmatrix
1 0 moveto 0 0 1 360 0 arcn closepath
setmatrix
pop pop pop pop
}def
/EllipticPathBackwards
{matrix currentmatrix dup 3 index 6 index sub 2 div
3 index 6 index sub 2 div
7 index 2 index add
7 index 2 index add
matrix translate 3 1 roll matrix scale
exch matrix concatmatrix exch matrix concatmatrix setmatrix
1 0 moveto 0 0 1 0 360 arc closepath
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pop pop pop pop
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{/y2 exch def /x2 exch def /y1 exch def /x1 exch def
newpath
x1 y1 moveto x2 y1 lineto x2 y2 lineto x1 y2 lineto
closepath
false StrokeWithPen } def
/FillRectangle
{/y2 exch def /x2 exch def /y1 exch def /x1 exch def
/MyMatrix matrix def
newpath
x1 y1 moveto x2 y1 lineto x2 y2 lineto x1 y2 lineto
closepath
FillWithBrush} def
/FrameRectangle
{/y2 exch def /x2 exch def /y1 exch def /x1 exch def
/MyMatrix matrix def
/x1 x1 0.5 sub def /x2 x2 0.5 add def /y2 y2 0.5 sub def /y1 y1 0.5 add def newpath
x1 y1 moveto x2 y1 lineto x2 y2 lineto x1 y2 lineto x1 y1 lineto
/x1 x1 1 add def /x2 x2 1 sub def /y2 y2 1 add def /y1 y1 1 sub def
x1 y1 moveto x1 y2 lineto x2 y2 lineto x2 y1 lineto x1 y1 lineto
closepath
FillWithBrush} def
%%EndResource
%%BeginResource: Polygon
/Polygon
{/MyMatrix matrix def
newpath PolylineArray PolylineMode 1 sub get exec closepath
true Fill&Stroke } def
/FillPolygon
{/MyMatrix matrix def
newpath PolylineArray PolylineMode 1 sub get exec closepath
FillWithBrush } def
%%EndResource
%%BeginResource: Polyline
/PolylineArray [ {DrawPolyline} {Bezier} ] def
/Polyline
{PolylineArray PolylineMode 1 sub get exec pop pop currentpoint true StrokeWithPen } def
/Bezier
{/nbPoint exch def /nbCurves nbPoint 1 sub 3 idiv def /nbLeft nbPoint 1 sub nbCurves 3 mul sub def
moveto 1 1 nbCurves { pop 4 2 roll 6 -2 roll curveto } for
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} def
/DrawPolyline
{/nbPoint exch def moveto
1 1 nbPoint 1 sub { pop lineto } for
} def
%%EndResource
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/Ellipse
{gsave
/Dy exch def /Dx exch def /Cy exch def /Cx exch def
Cx Cy translate Dx Dy scale
/MyMatrix Dx Dy matrix scale Cx Cy matrix translate matrix concatmatrix def
newpath 0 0 1 0 360 arc closepath
1 Dx div 1 Dy div scale 0 Cx sub 0 Cy sub translate
false Fill&Stroke
grestore } def
/FillEllipse
{gsave
/Dy exch def /Dx exch def /Cy exch def /Cx exch def
Cx Cy translate Dx Dy scale
/MyMatrix Dx Dy matrix scale Cx Cy matrix translate matrix concatmatrix def
newpath 0 0 1 0 360 arc closepath
FillWithBrush
grestore } def
%%EndResource
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/Arc
{ gsave
/ang1 exch def /ang2 exch def /Dy exch def /Dx exch def /Cy exch def /Cx exch def
Cx Cy translate Dx Dy
scale 1 -1 scale
newpath
ClockWise {0 0 1 ang2 ang1 narc} {0 0 1 ang2 ang1 arc} ifelse
1 -1 scale 1 Dx div 1 Dy div scale 0 Cx sub 0 Cy sub translate
false StrokeWithPen
grestore } def
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/Pie
{gsave
/ang1 exch def /ang2 exch def /Dy exch def /Dx exch def /Cy exch def /Cx exch def
Cx Cy translate Dx Dy scale
1 -1 scale
/MyMatrix Dx Dy matrix scale Cx Cy matrix translate matrix concatmatrix def
newpath 0 0 moveto ClockWise {0 0 1 ang2 ang1 narc} {0 0 1 ang2 ang1 arc} ifelse closepath
1 -1 scale 1 Dx div 1 Dy div scale 0 Cx sub 0 Cy sub translate
true Fill&Stroke
grestore } def
%%EndResource
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/Chord
{gsave
/ang1 exch def /ang2 exch def /Dy exch def /Dx exch def /Cy exch def /Cx exch def
Cx Cy translate Dx Dy scale
1 -1 scale
/MyMatrix Dx Dy matrix scale Cx Cy matrix translate matrix concatmatrix def
newpath ClockWise {0 0 1 ang2 ang1 narc} {0 0 1 ang2 ang1 arc} ifelse closepath
1 -1 scale 1 Dx div 1 Dy div scale 0 Cx sub 0 Cy sub translate
true Fill&Stroke
grestore } def
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/min {1 index 1 index le { pop} {exch pop} ifelse } def
/RoundRectangle
{/r2 exch def /r1 exch def /y2 exch def /x2 exch def /y1 exch def /x1 exch def
y2 2 div r2 min cvi /r2 exch def
x2 2 div r1 min cvi /r1 exch def
/width x2 r1 idiv def /height y2 r2 idiv def
gsave
x1 y1 translate r1 r2 scale
1 -1 scale
/MyMatrix r1 r2 matrix scale x1 y1 matrix translate matrix concatmatrix def
newpath
1 1 1 180 270 arc
width 1 sub 0 lineto width 1 sub 1 1 270 0 arc
width height 1 sub lineto width 1 sub height 1 sub 1 0 90 arc
1 height lineto 1 height 1 sub 1 90 180 arc
closepath
PenArray TmpPenArray copy pop
PenArray lpWidth PenArray lpWidth get r1 abs r2 abs add 2 div div put
false Fill&Stroke
TmpPenArray PenArray copy pop
grestore } def
%%EndResource
%%BeginResource: TextOut
/TextOut
{TextColorArray 0 get 255 div TextColorArray 1 get 255 div TextColorArray 2 get 255 div setrgbcolor
gsave translate rotate
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%%EndResource
%%BeginResource: MwSetFont
/EncodingDict 256 dict def
EncodingDict begin
0 [/.notdef /.notdef /.notdef /.notdef
/.notdef /.notdef /.notdef /.notdef
/.notdef /.notdef /.notdef /.notdef
/.notdef /.notdef /.notdef /.notdef
/.notdef /.notdef /.notdef /.notdef
/.notdef /.notdef /.notdef /.notdef
/.notdef /.notdef /.notdef /.notdef
/.notdef /.notdef /.notdef /.notdef
/space /exclam /quotedbl /numbersign
/dollar /percent /ampersand /quotesingle
/parenleft /parenright /asterisk /plus
/comma /hyphen /period /slash /zero /one
/two /three /four /five /six /seven
/eight /nine /colon /semicolon /less
/equal /greater /question /at /A /B /C
/D /E /F /G /H /I /J /K /L /M /N /O /P
/Q /R /S /T /U /V /W /X /Y /Z
/bracketleft /backslash /bracketright
/asciicircum /underscore /grave /a
/b /c /d /e /f /g /h /i /j /k /l /m /n
/o /p /q /r /s /t /u /v /w /x /y /z
/braceleft /bar /braceright /asciitilde
/.notdef /.notdef /.notdef /quotesinglbase
/florin /quotedblbase /ellipsis /dagger
/daggerdbl /circumflex /perthousand /Scaron
/guilsinglleft /OE /.notdef /.notdef
/.notdef /.notdef /quoteleft /quoteright
/quotedblleft /quotedblright /bullet /endash
/emdash /tilde /trademark /scaron
/guilsinglright /oe /.notdef /.notdef
/Ydieresis /.notdef /exclamdown /cent
/sterling /currency /yen /brokenbar
/section /dieresis /copyright
/ordfeminine /guillemotleft /logicalnot
/hyphen /registered /macron /degree
/plusminus /twosuperior /threesuperior
/acute /mu /paragraph /periodcentered
/cedilla /onesuperior /ordmasculine
/guillemotright /onequarter /onehalf
/threequarters /questiondown /Agrave
/Aacute /Acircumflex /Atilde /Adieresis
/Aring /AE /Ccedilla /Egrave /Eacute
/Ecircumflex /Edieresis /Igrave /Iacute
/Icircumflex /Idieresis /Eth /Ntilde
/Ograve /Oacute /Ocircumflex /Otilde
/Odieresis /multiply /Oslash /Ugrave
/Uacute /Ucircumflex /Udieresis /Yacute
/Thorn /germandbls /agrave /aacute
/acircumflex /atilde /adieresis /aring
/ae /ccedilla /egrave /eacute
/ecircumflex /edieresis /igrave /iacute
/icircumflex /idieresis /eth /ntilde
/ograve /oacute /ocircumflex /otilde
/odieresis /divide /oslash /ugrave
/uacute /ucircumflex /udieresis /yacute
/thorn /ydieresis] def
end
/fntdict 100 dict def
/MwScaleAndSetFont
{
2 index findfont dup length dict begin
{1 index /FID ne {def} {pop pop} ifelse} forall
dup EncodingDict exch known
{EncodingDict exch get /Encoding exch def} {pop} ifelse
currentdict end /font0 exch definefont
exch scalefont setfont pop
} def
/MwSetFont
{
% look in cache of scaled fonts
1 index /askedsize exch def
2 index /askedname exch def
fntdict askedname known
{ % font name found in cache - what about the size
/fntszdict fntdict askedname get def
fntszdict askedsize known
{
% font size found in cache
fntszdict askedsize get setfont pop pop pop
}
{
MwScaleAndSetFont
fntszdict askedsize currentfont put
}
ifelse
}
{ % not found in cache
MwScaleAndSetFont
/fntszdict 200 dict def
fntszdict askedsize currentfont put
fntdict askedname fntszdict put
}
ifelse
} def
%%EndResource
%%BeginResource: DisplayBB
/DisplayBB {gsave initgraphics 72 300 div 72 300 div scale 0 3300 translate
1 -1 scale 1 setlinewidth 1 0 0 setrgbcolor
/y2 exch def /x2 exch def /y1 exch def /x1 exch def
newpath x1 y1 moveto x2 y1 lineto x2 y2 lineto x1 y2 lineto closepath
stroke grestore } def
%%EndResource
%%EndProlog
%%BeginSetup
[{
%%BeginFeature: *InputSlot AUTO
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%%EndFeature
} stopped cleartomark
[{
%%BeginFeature: *PageRegion LETTER
LETTER
%%EndFeature
} stopped cleartomark
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%%Page:
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/ClockWise false def /LineJoin -1 def /MiterLimit -1 def /PolylineMode 1 def /LineCap 0 def
[0 0 0 0 0] UpdatePen
[0 255 255 255 0 <>] UpdateBrush
[0 0 0] UpdateTextColor
[255 255 255] UpdateBkColor
2 UpdateBkMode
0 0
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% in this file are expressed in pixels, but interpreted by
% Postscript as points (1/72 inch)!
% -->so scale accordingly!
72 300 div 72 300 div scale
% So that (0, 0) is at top-left corner of paper sheet (takes postscript scaling into account too)
0 3300 translate
1 -1 scale
/Courier 38 0 MwSetFont
gstate /Mwgstate exch def
%%EndPageSetup:
Mwgstate setgstate newpath
16 16 2416 3054 RectanglePath
clip newpath
/Courier 38 0 MwSetFont
[0 192 192 192 0 <>] UpdateBrush
[0 1 128 128 128] UpdatePen
1054 536 1761 647 FillRectangle
1054 536 1761 647 RectangleOutLine
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[0 1 0 0 0] UpdatePen
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1 UpdateBkMode
[255 255 255] UpdateBkColor
(G4NonEquilibriumEvaporator) 680 -0.00 1068 582 TextOut
[255 255 255] UpdateBkColor
2 UpdateBkMode
[0 192 192 192 0 <>] UpdateBrush
[0 1 128 128 128] UpdatePen
/Courier 38 0 MwSetFont
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[0 192 192 192 0 <>] UpdateBrush
/Courier 43 0 MwSetFont
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1054 596 1761 647 FillRectangle
1054 596 1761 647 RectangleOutLine
1054 619 1761 647 FillRectangle
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[0 192 192 192 0 <>] UpdateBrush
/Courier 43 0 MwSetFont
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1782 72 2281 183 FillRectangle
1782 72 2281 183 RectangleOutLine
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[0 0 0 0 0 <>] UpdateBrush
1 UpdateBkMode
[255 255 255] UpdateBkColor
(G4ExitationHandler) 471 -0.00 1796 118 TextOut
[255 255 255] UpdateBkColor
2 UpdateBkMode
[0 192 192 192 0 <>] UpdateBrush
[0 1 128 128 128] UpdatePen
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1782 132 2281 183 FillRectangle
1782 132 2281 183 RectangleOutLine
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1127 130 1656 285 FillRectangle
1127 130 1656 285 RectangleOutLine
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(G4VPreCompoundModel) 497 -0.00 1143 176 TextOut
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1127 238 1656 285 FillRectangle
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(\(from Geant4\)) 340 -0.00 1222 227 TextOut
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1781 159 LineTo
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1657 174 LineTo
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[0 0 0 0 0] UpdatePen
[1 0 0 0 0 <>] UpdateBrush
[0 1 128 128 128] UpdatePen
pop pop 1405 535
1395 286 LineTo
[0 255 255 255 0 <>] UpdateBrush
1375 347 1419 345 1395 286 3 Polygon
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[0 0 0 0 0] UpdatePen
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1815 312 2312 423 FillRectangle
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1815 372 2312 423 FillRectangle
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1815 395 2312 423 FillRectangle
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[0 192 192 192 0 <>] UpdateBrush
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[0 0 0 0 0] UpdatePen
[1 0 0 0 0 <>] UpdateBrush
[0 1 128 128 128] UpdatePen
[0 128 128 128 0 <>] UpdateBrush
pop pop 1743 290
1657 270 LineTo
pop pop 1657 270
1695 263 LineTo
pop pop 1657 270
1689 293 LineTo
[1 0 0 0 0 <>] UpdateBrush
[0 128 128 128 0 <>] UpdateBrush
pop pop 1743 290
1829 311 LineTo
[1 0 0 0 0 <>] UpdateBrush
[0 255 255 255 0 <>] UpdateBrush
[0 0 0 0 0] UpdatePen
Mwgstate setgstate newpath
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pop pop % pop out coordinates for current pen position
showpage
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% end of the MainWin EPS file