[819] | 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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[1340] | 26 | // $Id: G4eCoulombScatteringModel.cc,v 1.90 2010/10/26 10:35:22 vnivanch Exp $ |
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| 27 | // GEANT4 tag $Name: emstand-V09-03-24 $ |
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[819] | 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: G4eCoulombScatteringModel |
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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: 22.08.2005 |
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| 39 | // |
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| 40 | // Modifications: |
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[1196] | 41 | // |
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[819] | 42 | // 01.08.06 V.Ivanchenko extend upper limit of table to TeV and review the |
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| 43 | // logic of building - only elements from G4ElementTable |
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| 44 | // 08.08.06 V.Ivanchenko build internal table in ekin scale, introduce faclim |
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| 45 | // 19.08.06 V.Ivanchenko add inline function ScreeningParameter |
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| 46 | // 09.10.07 V.Ivanchenko reorganized methods, add cut dependence in scattering off e- |
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[961] | 47 | // 09.06.08 V.Ivanchenko add SelectIsotope and sampling of the recoil ion |
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[1196] | 48 | // 16.06.09 C.Consolandi fixed computation of effective mass |
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[1315] | 49 | // 27.05.10 V.Ivanchenko added G4WentzelOKandVIxSection class to |
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| 50 | // compute cross sections and sample scattering angle |
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[819] | 51 | // |
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[1196] | 52 | // |
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[819] | 53 | // Class Description: |
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| 54 | // |
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| 55 | // ------------------------------------------------------------------- |
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| 56 | // |
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| 57 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 58 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 59 | |
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| 60 | #include "G4eCoulombScatteringModel.hh" |
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| 61 | #include "Randomize.hh" |
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| 62 | #include "G4DataVector.hh" |
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| 63 | #include "G4ElementTable.hh" |
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| 64 | #include "G4ParticleChangeForGamma.hh" |
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| 65 | #include "G4Proton.hh" |
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[961] | 66 | #include "G4ParticleTable.hh" |
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[1196] | 67 | #include "G4ProductionCutsTable.hh" |
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| 68 | #include "G4NucleiProperties.hh" |
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[1315] | 69 | #include "G4Pow.hh" |
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| 70 | #include "G4LossTableManager.hh" |
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| 71 | #include "G4NistManager.hh" |
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[819] | 72 | |
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| 73 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 74 | |
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| 75 | using namespace std; |
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| 76 | |
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[961] | 77 | G4eCoulombScatteringModel::G4eCoulombScatteringModel(const G4String& nam) |
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[819] | 78 | : G4VEmModel(nam), |
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[961] | 79 | cosThetaMin(1.0), |
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| 80 | cosThetaMax(-1.0), |
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[819] | 81 | isInitialised(false) |
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| 82 | { |
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| 83 | fNistManager = G4NistManager::Instance(); |
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[961] | 84 | theParticleTable = G4ParticleTable::GetParticleTable(); |
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[819] | 85 | theProton = G4Proton::Proton(); |
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[961] | 86 | currentMaterial = 0; |
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| 87 | currentElement = 0; |
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[1315] | 88 | lowEnergyLimit = 1*eV; |
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[1196] | 89 | recoilThreshold = 0.*keV; |
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[819] | 90 | particle = 0; |
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[961] | 91 | currentCouple = 0; |
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[1315] | 92 | wokvi = new G4WentzelOKandVIxSection(); |
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[1340] | 93 | |
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| 94 | currentMaterialIndex = 0; |
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| 95 | |
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| 96 | cosTetMinNuc = 1.0; |
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| 97 | cosTetMaxNuc = -1.0; |
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| 98 | elecRatio = 0.0; |
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| 99 | mass = proton_mass_c2; |
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[819] | 100 | } |
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| 101 | |
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| 102 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 103 | |
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| 104 | G4eCoulombScatteringModel::~G4eCoulombScatteringModel() |
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[1315] | 105 | { |
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| 106 | delete wokvi; |
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| 107 | } |
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[819] | 108 | |
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| 109 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 110 | |
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| 111 | void G4eCoulombScatteringModel::Initialise(const G4ParticleDefinition* p, |
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[961] | 112 | const G4DataVector& cuts) |
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[819] | 113 | { |
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[961] | 114 | SetupParticle(p); |
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| 115 | currentCouple = 0; |
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| 116 | cosThetaMin = cos(PolarAngleLimit()); |
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[1315] | 117 | wokvi->Initialise(p, cosThetaMin); |
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| 118 | /* |
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| 119 | G4cout << "G4eCoulombScatteringModel: factorA2(GeV^2) = " << factorA2/(GeV*GeV) |
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| 120 | << " 1-cos(ThetaLimit)= " << 1 - cosThetaMin |
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| 121 | << " cos(thetaMax)= " << cosThetaMax |
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| 122 | << G4endl; |
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| 123 | */ |
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[1196] | 124 | pCuts = G4ProductionCutsTable::GetProductionCutsTable()->GetEnergyCutsVector(3); |
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[961] | 125 | //G4cout << "!!! G4eCoulombScatteringModel::Initialise for " |
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| 126 | // << p->GetParticleName() << " cos(TetMin)= " << cosThetaMin |
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| 127 | // << " cos(TetMax)= " << cosThetaMax <<G4endl; |
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[1196] | 128 | // G4cout << "cut0= " << cuts[0] << " cut1= " << cuts[1] << G4endl; |
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[819] | 129 | if(!isInitialised) { |
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| 130 | isInitialised = true; |
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[1055] | 131 | fParticleChange = GetParticleChangeForGamma(); |
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[819] | 132 | } |
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[961] | 133 | if(mass < GeV && particle->GetParticleType() != "nucleus") { |
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| 134 | InitialiseElementSelectors(p,cuts); |
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| 135 | } |
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| 136 | } |
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[819] | 137 | |
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[961] | 138 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... |
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[819] | 139 | |
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| 140 | G4double G4eCoulombScatteringModel::ComputeCrossSectionPerAtom( |
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| 141 | const G4ParticleDefinition* p, |
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| 142 | G4double kinEnergy, |
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[961] | 143 | G4double Z, G4double, |
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[819] | 144 | G4double cutEnergy, G4double) |
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| 145 | { |
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| 146 | //G4cout << "### G4eCoulombScatteringModel::ComputeCrossSectionPerAtom for " |
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[961] | 147 | // << p->GetParticleName()<<" Z= "<<Z<<" e(MeV)= "<< kinEnergy/MeV << G4endl; |
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| 148 | G4double xsec = 0.0; |
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[1315] | 149 | if(p != particle) { SetupParticle(p); } |
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| 150 | |
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| 151 | // cross section is set to zero to avoid problems in sample secondary |
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| 152 | if(kinEnergy < lowEnergyLimit) { return xsec; } |
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| 153 | DefineMaterial(CurrentCouple()); |
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| 154 | cosTetMinNuc = wokvi->SetupKinematic(kinEnergy, currentMaterial); |
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| 155 | if(cosThetaMax < cosTetMinNuc) { |
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| 156 | G4int iz = G4int(Z); |
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| 157 | cosTetMinNuc = wokvi->SetupTarget(iz, cutEnergy); |
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| 158 | cosTetMaxNuc = cosThetaMax; |
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| 159 | if(iz == 1 && cosTetMaxNuc < 0.0 && particle == theProton) { |
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| 160 | cosTetMaxNuc = 0.0; |
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| 161 | } |
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| 162 | xsec = wokvi->ComputeNuclearCrossSection(cosTetMinNuc, cosTetMaxNuc); |
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| 163 | elecRatio = wokvi->ComputeElectronCrossSection(cosTetMinNuc, cosThetaMax); |
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| 164 | xsec += elecRatio; |
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| 165 | if(xsec > 0.0) { elecRatio /= xsec; } |
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[961] | 166 | } |
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| 167 | /* |
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[1315] | 168 | G4cout << "e(MeV)= " << kinEnergy/MeV << " xsec(b)= " << xsec/barn |
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| 169 | << " 1-cosTetMinNuc= " << 1-cosTetMinNuc |
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| 170 | << " 1-cosTetMaxNuc2= " << 1-cosTetMaxNuc2 |
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| 171 | << " 1-cosTetMaxElec= " << 1-cosTetMaxElec |
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[961] | 172 | << " screenZ= " << screenZ |
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[1196] | 173 | << " formfactA= " << formfactA << G4endl; |
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[961] | 174 | */ |
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| 175 | return xsec; |
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[819] | 176 | } |
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| 177 | |
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| 178 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 179 | |
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| 180 | void G4eCoulombScatteringModel::SampleSecondaries( |
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[961] | 181 | std::vector<G4DynamicParticle*>* fvect, |
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[819] | 182 | const G4MaterialCutsCouple* couple, |
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| 183 | const G4DynamicParticle* dp, |
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| 184 | G4double cutEnergy, |
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[961] | 185 | G4double) |
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[819] | 186 | { |
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| 187 | G4double kinEnergy = dp->GetKineticEnergy(); |
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[1315] | 188 | if(kinEnergy < lowEnergyLimit) { return; } |
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[961] | 189 | SetupParticle(dp->GetDefinition()); |
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[1196] | 190 | |
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[961] | 191 | //G4cout << "G4eCoulombScatteringModel::SampleSecondaries e(MeV)= " |
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[1196] | 192 | // << kinEnergy << " " << particle->GetParticleName() |
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| 193 | // << " cut= " << cutEnergy<< G4endl; |
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[961] | 194 | |
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| 195 | // Choose nucleus |
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[1196] | 196 | currentElement = SelectRandomAtom(couple,particle, |
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| 197 | kinEnergy,cutEnergy,kinEnergy); |
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[819] | 198 | |
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[1315] | 199 | G4double Z = currentElement->GetZ(); |
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| 200 | |
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| 201 | if(ComputeCrossSectionPerAtom(particle,kinEnergy, Z, |
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| 202 | kinEnergy, cutEnergy, kinEnergy) == 0.0) |
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| 203 | { return; } |
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[1196] | 204 | |
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[1315] | 205 | G4int iz = G4int(Z); |
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[1196] | 206 | G4int ia = SelectIsotopeNumber(currentElement); |
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[1315] | 207 | G4double targetMass = G4NucleiProperties::GetNuclearMass(ia, iz); |
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[819] | 208 | |
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[1315] | 209 | G4ThreeVector newDirection = |
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| 210 | wokvi->SampleSingleScattering(cosTetMinNuc, cosThetaMax, elecRatio); |
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| 211 | G4double cost = newDirection.z(); |
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[819] | 212 | |
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[961] | 213 | G4ThreeVector direction = dp->GetMomentumDirection(); |
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| 214 | newDirection.rotateUz(direction); |
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| 215 | |
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| 216 | fParticleChange->ProposeMomentumDirection(newDirection); |
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| 217 | |
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| 218 | // recoil sampling assuming a small recoil |
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| 219 | // and first order correction to primary 4-momentum |
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[1315] | 220 | G4double mom2 = wokvi->GetMomentumSquare(); |
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| 221 | G4double trec = mom2*(1.0 - cost)/(targetMass + (mass + kinEnergy)*(1.0 + cost)); |
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[1196] | 222 | G4double finalT = kinEnergy - trec; |
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| 223 | //G4cout<<"G4eCoulombScatteringModel: finalT= "<<finalT<<" Trec= "<<trec<<G4endl; |
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| 224 | if(finalT <= lowEnergyLimit) { |
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| 225 | trec = kinEnergy; |
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| 226 | finalT = 0.0; |
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| 227 | } |
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[961] | 228 | |
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[1196] | 229 | fParticleChange->SetProposedKineticEnergy(finalT); |
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| 230 | G4double tcut = recoilThreshold; |
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| 231 | if(pCuts) { tcut= std::max(tcut,(*pCuts)[currentMaterialIndex]); } |
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| 232 | |
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| 233 | if(trec > tcut) { |
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| 234 | G4ParticleDefinition* ion = theParticleTable->FindIon(iz, ia, 0, iz); |
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| 235 | G4ThreeVector dir = (direction*sqrt(mom2) - |
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| 236 | newDirection*sqrt(finalT*(2*mass + finalT))).unit(); |
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| 237 | G4DynamicParticle* newdp = new G4DynamicParticle(ion, dir, trec); |
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| 238 | fvect->push_back(newdp); |
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| 239 | } else { |
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| 240 | fParticleChange->ProposeLocalEnergyDeposit(trec); |
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| 241 | fParticleChange->ProposeNonIonizingEnergyDeposit(trec); |
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[961] | 242 | } |
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| 243 | |
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| 244 | return; |
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| 245 | } |
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| 246 | |
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| 247 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... |
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| 248 | |
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| 249 | |
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