Geant4
11.1.1
Toolkit for the simulation of the passage of particles through matter
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G4F20GEMProbability.cc
Go to the documentation of this file.
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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//
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// Hadronic Process: Nuclear De-excitations
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// by V. Lara (Nov 1999)
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//
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#include "
G4F20GEMProbability.hh
"
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#include "
G4PhysicalConstants.hh
"
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#include "
G4SystemOfUnits.hh
"
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#include "
G4Log.hh
"
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G4F20GEMProbability::G4F20GEMProbability
() :
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G4GEMProbability
(20,9,2.0)
// A,Z,Spin
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{
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ExcitEnergies
.push_back(655.95*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(0.28*picosecond);
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ExcitEnergies
.push_back(822.9*keV);
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ExcitSpins
.push_back(4.0);
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ExcitLifetimes
.push_back(55*picosecond);
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ExcitEnergies
.push_back(983.8*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(1.1*picosecond);
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ExcitEnergies
.push_back(1056.93*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(31.0e-3*picosecond);
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ExcitEnergies
.push_back(1309.22*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(0.62*picosecond);
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ExcitEnergies
.push_back(1843.4*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(21.0e-3*picosecond);
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ExcitEnergies
.push_back(2043.9*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(26.0e-3*picosecond);
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ExcitEnergies
.push_back(2194.6*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(8.0e-3*picosecond);
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ExcitEnergies
.push_back(2966.2*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(42.0e-3*picosecond);
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ExcitEnergies
.push_back(3488.4*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(30.0e-3*picosecond);
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ExcitEnergies
.push_back(3525.9*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(21.0e-3*picosecond);
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ExcitEnergies
.push_back(3587.1*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(21.0e-3*picosecond);
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ExcitEnergies
.push_back(6627.0*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(hbar_Planck*
G4Log
(2.0)/(0.29*keV));
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ExcitEnergies
.push_back(6648.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1.62*keV));
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ExcitEnergies
.push_back(6685.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(3.80*keV));
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ExcitEnergies
.push_back(6692.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(5.23*keV));
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ExcitEnergies
.push_back(6696.0*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1.05*keV));
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ExcitEnergies
.push_back(6699.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(2.85*keV));
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ExcitEnergies
.push_back(6709.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1.14*keV));
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ExcitEnergies
.push_back(6717.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(0.95*keV));
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ExcitEnergies
.push_back(6791.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1.9*keV));
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ExcitEnergies
.push_back(6835.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1.7*keV));
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ExcitEnergies
.push_back(6837.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(0.4*keV));
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ExcitEnergies
.push_back(6856.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1.3*keV));
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ExcitEnergies
.push_back(6858.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(19.0*keV));
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ExcitEnergies
.push_back(7005.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(24.0*keV));
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ExcitEnergies
.push_back(7076.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(24.0*keV));
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ExcitEnergies
.push_back(7171.0*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(14.0*keV));
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ExcitEnergies
.push_back(7311.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(33.0*keV));
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ExcitEnergies
.push_back(7355.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(19.0*keV));
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ExcitEnergies
.push_back(7410.0*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(10.0*keV));
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ExcitEnergies
.push_back(7489.0*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(57.0*keV));
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ExcitEnergies
.push_back(7503.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(85.0*keV));
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ExcitEnergies
.push_back(7670.0*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(60.0*keV));
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ExcitEnergies
.push_back(7800.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(100.0*keV));
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ExcitEnergies
.push_back(8150.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(190.0*keV));
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ExcitEnergies
.push_back(10228.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(200.0*keV));
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ExcitEnergies
.push_back(10641.0*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(60.0*keV));
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ExcitEnergies
.push_back(10807.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(330.0*keV));
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}
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G4F20GEMProbability::~G4F20GEMProbability
()
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{}
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G4F20GEMProbability.hh
G4Log.hh
G4Log
G4double G4Log(G4double x)
Definition:
G4Log.hh:227
G4PhysicalConstants.hh
G4SystemOfUnits.hh
G4F20GEMProbability::~G4F20GEMProbability
~G4F20GEMProbability()
Definition:
G4F20GEMProbability.cc:198
G4F20GEMProbability::G4F20GEMProbability
G4F20GEMProbability()
Definition:
G4F20GEMProbability.cc:36
G4GEMProbability
Definition:
G4GEMProbability.hh:54
G4GEMProbability::ExcitSpins
std::vector< G4double > ExcitSpins
Definition:
G4GEMProbability.hh:117
G4GEMProbability::ExcitEnergies
std::vector< G4double > ExcitEnergies
Definition:
G4GEMProbability.hh:114
G4GEMProbability::fPlanck
G4double fPlanck
Definition:
G4GEMProbability.hh:111
G4GEMProbability::ExcitLifetimes
std::vector< G4double > ExcitLifetimes
Definition:
G4GEMProbability.hh:120
geant4-v11.1.1
source
processes
hadronic
models
de_excitation
gem_evaporation
src
G4F20GEMProbability.cc
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