Geant4
10.7.0
Toolkit for the simulation of the passage of particles through matter
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G4C12GEMProbability.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 "
G4C12GEMProbability.hh
"
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#include "
G4SystemOfUnits.hh
"
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G4C12GEMProbability::G4C12GEMProbability
() :
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G4GEMProbability
(12,6,0.0)
// A,Z,Spin
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{
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ExcitEnergies
.push_back(4438.91*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(10.8e-3*eV));
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ExcitEnergies
.push_back(7654.2*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(8.5*keV));
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ExcitEnergies
.push_back(9641*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(
fPlanck
/(34*keV));
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ExcitEnergies
.push_back(1.03E+4*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(3.0e3*keV));
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ExcitEnergies
.push_back(10844*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(315*keV));
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ExcitEnergies
.push_back(1.116E+4*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(430*keV));
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ExcitEnergies
.push_back(1.1828E+4*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(260*keV));
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ExcitEnergies
.push_back(12710*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(18.1*eV));
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ExcitEnergies
.push_back(13352*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(375*keV));
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ExcitEnergies
.push_back(14083*keV);
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ExcitSpins
.push_back(4.0);
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ExcitLifetimes
.push_back(
fPlanck
/(258*keV));
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ExcitEnergies
.push_back(15110*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(42*eV));
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ExcitEnergies
.push_back(16105.8*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(5.2*keV));
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ExcitEnergies
.push_back(16.57E+3*keV);
87
ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(300*keV));
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90
ExcitEnergies
.push_back(17.23E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1150*keV));
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ExcitEnergies
.push_back(17.76E+3*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(80*keV));
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ExcitEnergies
.push_back(18.13E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(600*keV));
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ExcitEnergies
.push_back(18.27E+3*keV);
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ExcitSpins
.push_back(4.0);
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ExcitLifetimes
.push_back(
fPlanck
/(300*keV));
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ExcitEnergies
.push_back(18.38E+3*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(
fPlanck
/(220*keV));
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ExcitEnergies
.push_back(18.39E+3*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(43*keV));
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ExcitEnergies
.push_back(18.6E+3*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(
fPlanck
/(300*keV));
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ExcitEnergies
.push_back(18.80E+3*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(100*keV));
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ExcitEnergies
.push_back(19.2E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1100*keV));
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ExcitEnergies
.push_back(19.39E+3*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(800*keV));
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ExcitEnergies
.push_back(19.55E+3*keV);
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ExcitSpins
.push_back(4.0);
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ExcitLifetimes
.push_back(
fPlanck
/(490*keV));
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ExcitEnergies
.push_back(19.69E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(230*keV));
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ExcitEnergies
.push_back(20.0E+3*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(100*keV));
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ExcitEnergies
.push_back(20.27E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(140*keV));
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ExcitEnergies
.push_back(20.5E+3*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(
fPlanck
/(180*keV));
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ExcitEnergies
.push_back(20.62E+3*keV);
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ExcitSpins
.push_back(3.0);
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ExcitLifetimes
.push_back(
fPlanck
/(200*keV));
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ExcitEnergies
.push_back(21.60E+3*keV);
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ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1200*keV));
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158
ExcitEnergies
.push_back(22.0E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(800*keV));
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ExcitEnergies
.push_back(22.40E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(275*keV));
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ExcitEnergies
.push_back(22.65E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(3200*keV));
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ExcitEnergies
.push_back(23.04E+3 *keV);
171
ExcitSpins
.push_back(2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(60*keV));
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174
ExcitEnergies
.push_back(23.52E+3*keV);
175
ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(230*keV));
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178
ExcitEnergies
.push_back(23.92E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(400*keV));
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ExcitEnergies
.push_back(25.30E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(510*keV));
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ExcitEnergies
.push_back(25.4E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(2000*keV));
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ExcitEnergies
.push_back(27.0E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1400*keV));
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ExcitEnergies
.push_back(27595.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(30*keV));
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ExcitEnergies
.push_back(28.2E+3*keV);
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ExcitSpins
.push_back(1.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1600*keV));
201
}
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G4C12GEMProbability::~G4C12GEMProbability
()
204
{}
G4C12GEMProbability.hh
G4SystemOfUnits.hh
G4C12GEMProbability::~G4C12GEMProbability
~G4C12GEMProbability()
Definition:
G4C12GEMProbability.cc:203
G4C12GEMProbability::G4C12GEMProbability
G4C12GEMProbability()
Definition:
G4C12GEMProbability.cc:34
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-v10.7.0
source
processes
hadronic
models
de_excitation
gem_evaporation
src
G4C12GEMProbability.cc
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