Geant4
11.2.2
Toolkit for the simulation of the passage of particles through matter
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G4N13GEMProbability.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 "
G4N13GEMProbability.hh
"
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#include "
G4SystemOfUnits.hh
"
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G4N13GEMProbability::G4N13GEMProbability
() :
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G4GEMProbability
(13,7,1.0/2.0)
// A,Z,Spin
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{
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ExcitEnergies
.push_back(2364.9*keV);
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ExcitSpins
.push_back(1.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(33*keV));
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ExcitEnergies
.push_back(3502*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(66*keV));
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ExcitEnergies
.push_back(3547*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(47*keV));
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ExcitEnergies
.push_back(6364*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(11*keV));
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ExcitEnergies
.push_back(6885*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(115*keV));
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ExcitEnergies
.push_back(7155*keV);
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ExcitSpins
.push_back(7.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(9.0*keV));
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ExcitEnergies
.push_back(7376*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(75*keV));
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ExcitEnergies
.push_back(8000*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1500*keV));
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ExcitEnergies
.push_back(8918*keV);
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ExcitSpins
.push_back(1.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(230*keV));
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ExcitEnergies
.push_back(9476*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(30*keV));
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ExcitEnergies
.push_back(10.25E3*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(270*keV));
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ExcitEnergies
.push_back(10360*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(30*keV));
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ExcitEnergies
.push_back(10360*keV);
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ExcitSpins
.push_back(7.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(76*keV));
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ExcitEnergies
.push_back(11530*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(430*keV));
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ExcitEnergies
.push_back(11740*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(115*keV));
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ExcitEnergies
.push_back(11740*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(250*keV));
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ExcitEnergies
.push_back(11740*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(530*keV));
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ExcitEnergies
.push_back(11878*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(380*keV));
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ExcitEnergies
.push_back(12130*keV);
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ExcitSpins
.push_back(7.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(250*keV));
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ExcitEnergies
.push_back(13.5E3*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(6500*keV));
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ExcitEnergies
.push_back(14050*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(155*keV));
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ExcitEnergies
.push_back(15064.6*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1.10*keV));
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ExcitEnergies
.push_back(15.3E3*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(350*keV));
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ExcitEnergies
.push_back(16020*keV);
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ExcitSpins
.push_back(7.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(130*keV));
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ExcitEnergies
.push_back(18230*keV);
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ExcitSpins
.push_back(1.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(300*keV));
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ExcitEnergies
.push_back(18406*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(66*keV));
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ExcitEnergies
.push_back(18961*keV);
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ExcitSpins
.push_back(7.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(23*keV));
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ExcitEnergies
.push_back(19830*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1000*keV));
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ExcitEnergies
.push_back(19880*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(520*keV));
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ExcitEnergies
.push_back(20.9E3*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1100*keV));
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ExcitEnergies
.push_back(22.4E3*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(2000*keV));
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}
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G4N13GEMProbability::~G4N13GEMProbability
()
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{}
G4N13GEMProbability.hh
G4SystemOfUnits.hh
G4GEMProbability
Definition
G4GEMProbability.hh:54
G4GEMProbability::ExcitSpins
std::vector< G4double > ExcitSpins
Definition
G4GEMProbability.hh:124
G4GEMProbability::ExcitEnergies
std::vector< G4double > ExcitEnergies
Definition
G4GEMProbability.hh:121
G4GEMProbability::fPlanck
G4double fPlanck
Definition
G4GEMProbability.hh:118
G4GEMProbability::ExcitLifetimes
std::vector< G4double > ExcitLifetimes
Definition
G4GEMProbability.hh:127
G4N13GEMProbability::~G4N13GEMProbability
~G4N13GEMProbability()
Definition
G4N13GEMProbability.cc:162
G4N13GEMProbability::G4N13GEMProbability
G4N13GEMProbability()
Definition
G4N13GEMProbability.cc:34
geant4-v11.2.2
source
processes
hadronic
models
de_excitation
gem_evaporation
src
G4N13GEMProbability.cc
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