| 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: G4eCoulombScatteringModel.cc,v 1.89 2010/05/27 14:22:05 vnivanch Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-04-beta-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: 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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| 41 | //
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| 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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| 47 | // 09.06.08 V.Ivanchenko add SelectIsotope and sampling of the recoil ion
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| 48 | // 16.06.09 C.Consolandi fixed computation of effective mass
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| 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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| 51 | //
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| 52 | //
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| 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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| 66 | #include "G4ParticleTable.hh"
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| 67 | #include "G4ProductionCutsTable.hh"
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| 68 | #include "G4NucleiProperties.hh"
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| 69 | #include "G4Pow.hh"
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| 70 | #include "G4LossTableManager.hh"
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| 71 | #include "G4NistManager.hh"
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| 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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| 77 | G4eCoulombScatteringModel::G4eCoulombScatteringModel(const G4String& nam)
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| 78 | : G4VEmModel(nam),
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| 79 | cosThetaMin(1.0),
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| 80 | cosThetaMax(-1.0),
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| 81 | isInitialised(false)
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| 82 | {
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| 83 | fNistManager = G4NistManager::Instance();
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| 84 | theParticleTable = G4ParticleTable::GetParticleTable();
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| 85 | theProton = G4Proton::Proton();
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| 86 | currentMaterial = 0;
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| 87 | currentElement = 0;
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| 88 | lowEnergyLimit = 1*eV;
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| 89 | recoilThreshold = 0.*keV;
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| 90 | particle = 0;
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| 91 | currentCouple = 0;
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| 92 | wokvi = new G4WentzelOKandVIxSection();
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| 93 | }
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| 94 |
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| 95 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 96 |
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| 97 | G4eCoulombScatteringModel::~G4eCoulombScatteringModel()
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| 98 | {
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| 99 | delete wokvi;
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| 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 | void G4eCoulombScatteringModel::Initialise(const G4ParticleDefinition* p,
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| 105 | const G4DataVector& cuts)
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| 106 | {
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| 107 | SetupParticle(p);
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| 108 | currentCouple = 0;
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| 109 | cosThetaMin = cos(PolarAngleLimit());
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| 110 | wokvi->Initialise(p, cosThetaMin);
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| 111 | /*
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| 112 | G4cout << "G4eCoulombScatteringModel: factorA2(GeV^2) = " << factorA2/(GeV*GeV)
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| 113 | << " 1-cos(ThetaLimit)= " << 1 - cosThetaMin
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| 114 | << " cos(thetaMax)= " << cosThetaMax
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| 115 | << G4endl;
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| 116 | */
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| 117 | pCuts = G4ProductionCutsTable::GetProductionCutsTable()->GetEnergyCutsVector(3);
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| 118 | //G4cout << "!!! G4eCoulombScatteringModel::Initialise for "
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| 119 | // << p->GetParticleName() << " cos(TetMin)= " << cosThetaMin
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| 120 | // << " cos(TetMax)= " << cosThetaMax <<G4endl;
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| 121 | // G4cout << "cut0= " << cuts[0] << " cut1= " << cuts[1] << G4endl;
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| 122 | if(!isInitialised) {
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| 123 | isInitialised = true;
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| 124 | fParticleChange = GetParticleChangeForGamma();
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| 125 | }
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| 126 | if(mass < GeV && particle->GetParticleType() != "nucleus") {
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| 127 | InitialiseElementSelectors(p,cuts);
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| 128 | }
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| 129 | }
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| 130 |
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| 131 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 132 |
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| 133 | G4double G4eCoulombScatteringModel::ComputeCrossSectionPerAtom(
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| 134 | const G4ParticleDefinition* p,
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| 135 | G4double kinEnergy,
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| 136 | G4double Z, G4double,
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| 137 | G4double cutEnergy, G4double)
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| 138 | {
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| 139 | //G4cout << "### G4eCoulombScatteringModel::ComputeCrossSectionPerAtom for "
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| 140 | // << p->GetParticleName()<<" Z= "<<Z<<" e(MeV)= "<< kinEnergy/MeV << G4endl;
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| 141 | G4double xsec = 0.0;
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| 142 | if(p != particle) { SetupParticle(p); }
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| 143 |
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| 144 | // cross section is set to zero to avoid problems in sample secondary
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| 145 | if(kinEnergy < lowEnergyLimit) { return xsec; }
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| 146 | DefineMaterial(CurrentCouple());
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| 147 | cosTetMinNuc = wokvi->SetupKinematic(kinEnergy, currentMaterial);
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| 148 | if(cosThetaMax < cosTetMinNuc) {
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| 149 | G4int iz = G4int(Z);
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| 150 | cosTetMinNuc = wokvi->SetupTarget(iz, cutEnergy);
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| 151 | cosTetMaxNuc = cosThetaMax;
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| 152 | if(iz == 1 && cosTetMaxNuc < 0.0 && particle == theProton) {
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| 153 | cosTetMaxNuc = 0.0;
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| 154 | }
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| 155 | xsec = wokvi->ComputeNuclearCrossSection(cosTetMinNuc, cosTetMaxNuc);
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| 156 | elecRatio = wokvi->ComputeElectronCrossSection(cosTetMinNuc, cosThetaMax);
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| 157 | xsec += elecRatio;
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| 158 | if(xsec > 0.0) { elecRatio /= xsec; }
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| 159 | }
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| 160 | /*
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| 161 | G4cout << "e(MeV)= " << kinEnergy/MeV << " xsec(b)= " << xsec/barn
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| 162 | << " 1-cosTetMinNuc= " << 1-cosTetMinNuc
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| 163 | << " 1-cosTetMaxNuc2= " << 1-cosTetMaxNuc2
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| 164 | << " 1-cosTetMaxElec= " << 1-cosTetMaxElec
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| 165 | << " screenZ= " << screenZ
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| 166 | << " formfactA= " << formfactA << G4endl;
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| 167 | */
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| 168 | return xsec;
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| 169 | }
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| 170 |
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| 171 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 172 |
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| 173 | void G4eCoulombScatteringModel::SampleSecondaries(
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| 174 | std::vector<G4DynamicParticle*>* fvect,
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| 175 | const G4MaterialCutsCouple* couple,
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| 176 | const G4DynamicParticle* dp,
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| 177 | G4double cutEnergy,
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| 178 | G4double)
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| 179 | {
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| 180 | G4double kinEnergy = dp->GetKineticEnergy();
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| 181 | if(kinEnergy < lowEnergyLimit) { return; }
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| 182 | SetupParticle(dp->GetDefinition());
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| 183 |
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| 184 | //G4cout << "G4eCoulombScatteringModel::SampleSecondaries e(MeV)= "
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| 185 | // << kinEnergy << " " << particle->GetParticleName()
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| 186 | // << " cut= " << cutEnergy<< G4endl;
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| 187 |
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| 188 | // Choose nucleus
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| 189 | currentElement = SelectRandomAtom(couple,particle,
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| 190 | kinEnergy,cutEnergy,kinEnergy);
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| 191 |
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| 192 | G4double Z = currentElement->GetZ();
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| 193 |
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| 194 | if(ComputeCrossSectionPerAtom(particle,kinEnergy, Z,
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| 195 | kinEnergy, cutEnergy, kinEnergy) == 0.0)
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| 196 | { return; }
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| 197 |
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| 198 | G4int iz = G4int(Z);
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| 199 | G4int ia = SelectIsotopeNumber(currentElement);
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| 200 | G4double targetMass = G4NucleiProperties::GetNuclearMass(ia, iz);
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| 201 |
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| 202 | G4ThreeVector newDirection =
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| 203 | wokvi->SampleSingleScattering(cosTetMinNuc, cosThetaMax, elecRatio);
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| 204 | G4double cost = newDirection.z();
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| 205 |
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| 206 | G4ThreeVector direction = dp->GetMomentumDirection();
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| 207 | newDirection.rotateUz(direction);
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| 208 |
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| 209 | fParticleChange->ProposeMomentumDirection(newDirection);
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| 210 |
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| 211 | // recoil sampling assuming a small recoil
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| 212 | // and first order correction to primary 4-momentum
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| 213 | G4double mom2 = wokvi->GetMomentumSquare();
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| 214 | G4double trec = mom2*(1.0 - cost)/(targetMass + (mass + kinEnergy)*(1.0 + cost));
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| 215 | G4double finalT = kinEnergy - trec;
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| 216 | //G4cout<<"G4eCoulombScatteringModel: finalT= "<<finalT<<" Trec= "<<trec<<G4endl;
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| 217 | if(finalT <= lowEnergyLimit) {
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| 218 | trec = kinEnergy;
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| 219 | finalT = 0.0;
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| 220 | }
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| 221 |
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| 222 | fParticleChange->SetProposedKineticEnergy(finalT);
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| 223 | G4double tcut = recoilThreshold;
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| 224 | if(pCuts) { tcut= std::max(tcut,(*pCuts)[currentMaterialIndex]); }
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| 225 |
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| 226 | if(trec > tcut) {
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| 227 | G4ParticleDefinition* ion = theParticleTable->FindIon(iz, ia, 0, iz);
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| 228 | G4ThreeVector dir = (direction*sqrt(mom2) -
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| 229 | newDirection*sqrt(finalT*(2*mass + finalT))).unit();
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| 230 | G4DynamicParticle* newdp = new G4DynamicParticle(ion, dir, trec);
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| 231 | fvect->push_back(newdp);
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| 232 | } else {
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| 233 | fParticleChange->ProposeLocalEnergyDeposit(trec);
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| 234 | fParticleChange->ProposeNonIonizingEnergyDeposit(trec);
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| 235 | }
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| 236 |
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| 237 | return;
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| 238 | }
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| 239 |
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| 240 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 241 |
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| 242 |
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