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9.6.p02
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geant4_9_6_p02
source
processes
hadronic
models
de_excitation
gem_evaporation
src
G4Be9GEMProbability.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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// $Id$
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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 "
G4Be9GEMProbability.hh
"
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#include "
G4SystemOfUnits.hh
"
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G4Be9GEMProbability::G4Be9GEMProbability
() :
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G4GEMProbability
(9,4,3.0/2.0)
// A,Z,Spin
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{
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ExcitEnergies
.push_back(1685.0*
keV
);
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ExcitSpins
.push_back(1.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(150.0*
keV
));
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ExcitEnergies
.push_back(2429.4*
keV
);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(0.77*
keV
));
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ExcitEnergies
.push_back(2.78e3*
keV
);
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ExcitSpins
.push_back(1.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1080.0*keV));
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ExcitEnergies
.push_back(3049.0*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(282.0*keV));
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ExcitEnergies
.push_back(4704.0*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(743.0*keV));
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ExcitEnergies
.push_back(6760.0*keV);
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ExcitSpins
.push_back(7.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1540.0*keV));
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ExcitEnergies
.push_back(7940.0*keV);
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ExcitSpins
.push_back(1.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1000.0*keV));
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ExcitEnergies
.push_back(11283.0*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(575.0*keV));
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ExcitEnergies
.push_back(11810.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(400.0*keV));
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ExcitEnergies
.push_back(13790.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(590.0*keV));
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ExcitEnergies
.push_back(14392.9*keV);
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ExcitSpins
.push_back(3.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(0.381*keV));
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ExcitEnergies
.push_back(14.4e3*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(800*keV));
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ExcitEnergies
.push_back(15970.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(300.0*keV));
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90
ExcitEnergies
.push_back(16671.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(41.0*keV));
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ExcitEnergies
.push_back(16975.0*keV);
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ExcitSpins
.push_back(1.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(0.47*keV));
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ExcitEnergies
.push_back(17298.0*keV);
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ExcitSpins
.push_back(5.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(200.0*keV));
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ExcitEnergies
.push_back(17493.0*keV);
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ExcitSpins
.push_back(7.0/2.0);
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ExcitLifetimes
.push_back(
fPlanck
/(47.0*keV));
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ExcitEnergies
.push_back(19200.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(310.0*keV));
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ExcitEnergies
.push_back(20740.0*keV);
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ExcitSpins
.push_back(0.0);
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ExcitLifetimes
.push_back(
fPlanck
/(1000.0*keV));
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}
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G4Be9GEMProbability::~G4Be9GEMProbability
()
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{}
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