| 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | // $Id: G4eeToHadronsMultiModel.cc,v 1.8 2009/04/12 17:48:21 vnivanch Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 28 | //
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| 29 | // -------------------------------------------------------------------
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| 30 | //
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| 31 | // GEANT4 Class file
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| 32 | //
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| 33 | //
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| 34 | // File name: G4eeToHadronsMultiModel
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| 35 | //
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| 36 | // Author: Vladimir Ivanchenko
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| 37 | //
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| 38 | // Creation date: 02.08.2004
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| 39 | //
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| 40 | // Modifications:
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| 41 | // 08-11-04 Migration to new interface of Store/Retrieve tables (V.Ivantchenko)
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| 42 | // 08-04-05 Major optimisation of internal interfaces (V.Ivantchenko)
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| 43 | //
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| 44 |
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| 45 | //
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| 46 | // -------------------------------------------------------------------
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| 47 | //
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| 48 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 49 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 50 |
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| 51 | #include "G4eeToHadronsMultiModel.hh"
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| 52 | #include "G4eeToTwoPiModel.hh"
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| 53 | #include "G4eeTo3PiModel.hh"
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| 54 | #include "G4eeToPGammaModel.hh"
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| 55 | #include "G4ee2KNeutralModel.hh"
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| 56 | #include "G4ee2KChargedModel.hh"
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| 57 | #include "G4eeCrossSections.hh"
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| 58 | #include "G4Vee2hadrons.hh"
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| 59 |
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| 60 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 61 |
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| 62 | using namespace std;
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| 63 |
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| 64 | G4eeToHadronsMultiModel::G4eeToHadronsMultiModel(G4int ver, const G4String& name)
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| 65 | : G4VEmModel(name),
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| 66 | csFactor(1.0),
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| 67 | nModels(0),
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| 68 | verbose(ver),
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| 69 | isInitialised(false)
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| 70 | {}
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| 71 |
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| 72 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 73 |
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| 74 | G4eeToHadronsMultiModel::~G4eeToHadronsMultiModel()
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| 75 | {
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| 76 | G4int n = models.size();
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| 77 | if(n>0) {
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| 78 | for(G4int i=0; i<n; i++) {
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| 79 | delete models[i];
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| 80 | }
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| 81 | }
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| 82 | delete cross;
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| 83 | }
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| 84 |
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| 85 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 86 |
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| 87 | void G4eeToHadronsMultiModel::Initialise(const G4ParticleDefinition*,
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| 88 | const G4DataVector&)
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| 89 | {
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| 90 | if(!isInitialised) {
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| 91 | isInitialised = true;
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| 92 |
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| 93 | thKineticEnergy = DBL_MAX;
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| 94 | maxKineticEnergy = 1.2*GeV;
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| 95 |
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| 96 | cross = new G4eeCrossSections();
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| 97 |
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| 98 | G4eeToTwoPiModel* m2pi = new G4eeToTwoPiModel(cross);
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| 99 | m2pi->SetHighEnergy(maxKineticEnergy);
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| 100 | AddEEModel(m2pi);
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| 101 |
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| 102 | G4eeTo3PiModel* m3pi1 = new G4eeTo3PiModel(cross);
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| 103 | m3pi1->SetHighEnergy(0.95*GeV);
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| 104 | AddEEModel(m3pi1);
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| 105 |
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| 106 | G4eeTo3PiModel* m3pi2 = new G4eeTo3PiModel(cross);
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| 107 | m3pi2->SetLowEnergy(0.95*GeV);
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| 108 | m3pi2->SetHighEnergy(maxKineticEnergy);
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| 109 | AddEEModel(m3pi2);
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| 110 |
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| 111 | G4ee2KChargedModel* m2kc = new G4ee2KChargedModel(cross);
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| 112 | m2kc->SetHighEnergy(maxKineticEnergy);
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| 113 | AddEEModel(m2kc);
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| 114 |
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| 115 | G4ee2KNeutralModel* m2kn = new G4ee2KNeutralModel(cross);
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| 116 | m2kn->SetHighEnergy(maxKineticEnergy);
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| 117 | AddEEModel(m2kn);
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| 118 |
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| 119 | G4eeToPGammaModel* mpg1 = new G4eeToPGammaModel(cross,"pi0");
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| 120 | mpg1->SetLowEnergy(0.7*GeV);
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| 121 | mpg1->SetHighEnergy(maxKineticEnergy);
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| 122 | AddEEModel(mpg1);
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| 123 |
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| 124 | G4eeToPGammaModel* mpg2 = new G4eeToPGammaModel(cross,"eta");
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| 125 | mpg2->SetLowEnergy(0.7*GeV);
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| 126 | mpg2->SetHighEnergy(maxKineticEnergy);
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| 127 | AddEEModel(mpg2);
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| 128 |
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| 129 | nModels = models.size();
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| 130 |
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| 131 | fParticleChange = GetParticleChangeForGamma();
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| 132 | }
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| 133 | }
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| 134 |
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| 135 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 136 |
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| 137 | void G4eeToHadronsMultiModel::AddEEModel(G4Vee2hadrons* mod)
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| 138 | {
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| 139 | G4eeToHadronsModel* model = new G4eeToHadronsModel(mod, verbose);
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| 140 | model->SetLowEnergyLimit(LowEnergyLimit());
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| 141 | model->SetHighEnergyLimit(HighEnergyLimit());
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| 142 | models.push_back(model);
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| 143 | G4double elow = mod->ThresholdEnergy();
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| 144 | ekinMin.push_back(elow);
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| 145 | if(thKineticEnergy > elow) thKineticEnergy = elow;
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| 146 | ekinMax.push_back(mod->HighEnergy());
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| 147 | ekinPeak.push_back(mod->PeakEnergy());
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| 148 | cumSum.push_back(0.0);
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| 149 | }
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| 150 |
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| 151 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 152 |
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| 153 | G4double G4eeToHadronsMultiModel::CrossSectionPerVolume(
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| 154 | const G4Material* mat,
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| 155 | const G4ParticleDefinition* p,
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| 156 | G4double kineticEnergy,
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| 157 | G4double, G4double)
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| 158 | {
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| 159 | return mat->GetElectronDensity()*
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| 160 | ComputeCrossSectionPerElectron(p, kineticEnergy);
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| 161 | }
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| 162 |
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| 163 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 164 |
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| 165 | G4double G4eeToHadronsMultiModel::ComputeCrossSectionPerAtom(
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| 166 | const G4ParticleDefinition* p,
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| 167 | G4double kineticEnergy,
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| 168 | G4double Z, G4double,
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| 169 | G4double, G4double)
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| 170 | {
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| 171 | return Z*ComputeCrossSectionPerElectron(p, kineticEnergy);
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| 172 | }
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| 173 |
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| 174 |
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| 175 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 176 |
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| 177 | void G4eeToHadronsMultiModel::SampleSecondaries(std::vector<G4DynamicParticle*>* newp,
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| 178 | const G4MaterialCutsCouple* couple,
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| 179 | const G4DynamicParticle* dp,
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| 180 | G4double, G4double)
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| 181 | {
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| 182 | G4double kinEnergy = dp->GetKineticEnergy();
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| 183 | if (kinEnergy > thKineticEnergy) {
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| 184 | G4double q = cumSum[nModels-1]*G4UniformRand();
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| 185 | for(G4int i=0; i<nModels; i++) {
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| 186 | if(q <= cumSum[i]) {
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| 187 | (models[i])->SampleSecondaries(newp, couple,dp);
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| 188 | if(newp->size() > 0) fParticleChange->ProposeTrackStatus(fStopAndKill);
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| 189 | break;
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| 190 | }
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| 191 | }
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| 192 | }
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| 193 | }
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| 194 |
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| 195 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 196 |
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| 197 | void G4eeToHadronsMultiModel::PrintInfo()
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| 198 | {
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| 199 | if(verbose > 0) {
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| 200 | G4double e1 = 0.5*thKineticEnergy*thKineticEnergy/electron_mass_c2
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| 201 | - 2.0*electron_mass_c2;
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| 202 | G4double e2 = 0.5*maxKineticEnergy*maxKineticEnergy/electron_mass_c2
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| 203 | - 2.0*electron_mass_c2;
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| 204 | G4cout << " e+ annihilation into hadrons active from "
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| 205 | << e1/GeV << " GeV to " << e2/GeV << " GeV"
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| 206 | << G4endl;
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| 207 | }
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| 208 | }
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| 209 |
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| 210 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 211 |
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| 212 | void G4eeToHadronsMultiModel::SetCrossSecFactor(G4double fac)
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| 213 | {
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| 214 | if(fac > 1.0) {
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| 215 | csFactor = fac;
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| 216 | if(verbose > 0)
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| 217 | G4cout << "### G4eeToHadronsMultiModel: The cross section for G4eeToHadronsMultiModel "
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| 218 | << " is increased by the Factor= " << csFactor << G4endl;
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| 219 | }
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| 220 | }
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| 221 |
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| 222 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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