[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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[1315] | 26 | // $Id: G4CoulombScatteringModel.cc,v 1.49 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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[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: G4CoulombScatteringModel |
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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 | // 19.10.06 V.Ivanchenko use inheritance from G4eCoulombScatteringModel |
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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 SelectIsotope is moved to the base class |
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[1196] | 48 | // 16.06.09 Consolandi rows 109, 111-112, 183, 185-186 |
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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 "G4CoulombScatteringModel.hh" |
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| 61 | #include "Randomize.hh" |
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| 62 | #include "G4ParticleChangeForGamma.hh" |
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| 63 | #include "G4ParticleTable.hh" |
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| 64 | #include "G4IonTable.hh" |
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| 65 | #include "G4Proton.hh" |
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[1315] | 66 | #include "G4NucleiProperties.hh" |
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[819] | 67 | |
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| 68 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 69 | |
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| 70 | using namespace std; |
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| 71 | |
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[961] | 72 | G4CoulombScatteringModel::G4CoulombScatteringModel(const G4String& nam) |
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| 73 | : G4eCoulombScatteringModel(nam) |
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| 74 | {} |
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[819] | 75 | |
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| 76 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 77 | |
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| 78 | G4CoulombScatteringModel::~G4CoulombScatteringModel() |
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| 79 | {} |
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| 80 | |
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| 81 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 82 | |
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| 83 | G4double G4CoulombScatteringModel::ComputeCrossSectionPerAtom( |
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| 84 | const G4ParticleDefinition* p, |
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| 85 | G4double kinEnergy, |
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| 86 | G4double Z, |
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[961] | 87 | G4double, |
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[819] | 88 | G4double cutEnergy, |
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| 89 | G4double) |
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| 90 | { |
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[1315] | 91 | //G4cout << "### G4CoulombScatteringModel::ComputeCrossSectionPerAtom for " |
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| 92 | // << p->GetParticleName()<<" Z= "<<Z<<" e(MeV)= "<< kinEnergy/MeV |
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| 93 | // <<" cut(MeV)= " << cutEnergy<< G4endl; |
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| 94 | G4double xsec = 0.0; |
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| 95 | if(p != particle) { SetupParticle(p); } |
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| 96 | if(kinEnergy < lowEnergyLimit) { return 0.0; } |
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| 97 | DefineMaterial(CurrentCouple()); |
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[819] | 98 | |
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[1315] | 99 | // Lab system |
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| 100 | G4int iz = G4int(Z); |
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| 101 | G4double etot = kinEnergy + mass; |
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| 102 | G4double m2 = fNistManager->GetAtomicMassAmu(iz)*amu_c2; |
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[819] | 103 | |
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[1315] | 104 | // 03.09.2009 C.Consaldi suggested to use relativistic reduced mass |
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| 105 | // from publucation |
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| 106 | // A.P. Martynenko, R.N. Faustov, Teoret. mat. Fiz. 64 (1985) 179 |
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| 107 | G4double Ecm = sqrt(mass*mass + m2*m2 + 2.0*etot*m2); |
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| 108 | G4double mu_rel = mass*m2/Ecm; |
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| 109 | G4double tkin = Ecm - mu_rel; |
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| 110 | wokvi->SetRelativisticMass(mu_rel); |
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| 111 | |
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| 112 | cosTetMinNuc = wokvi->SetupKinematic(tkin, currentMaterial); |
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| 113 | if(cosThetaMax < cosTetMinNuc) { |
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| 114 | cosTetMinNuc = wokvi->SetupTarget(iz, cutEnergy); |
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| 115 | cosTetMaxNuc = cosThetaMax; |
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| 116 | if(iz == 1 && cosTetMaxNuc < 0.0 && particle == theProton) { |
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| 117 | cosTetMaxNuc = 0.0; |
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| 118 | } |
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| 119 | xsec = wokvi->ComputeNuclearCrossSection(cosTetMinNuc, cosTetMaxNuc); |
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| 120 | elecRatio = wokvi->ComputeElectronCrossSection(cosTetMinNuc, cosThetaMax); |
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| 121 | xsec += elecRatio; |
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| 122 | if(xsec > 0.0) { elecRatio /= xsec; } |
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| 123 | } |
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| 124 | /* |
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| 125 | G4cout << "e(MeV)= " << kinEnergy/MeV << " xsec(b)= " << xsec/barn |
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| 126 | << "cosTetMinNuc= " << cosTetMinNuc |
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| 127 | << " cosTetMaxNuc= " << cosTetMaxNuc |
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| 128 | << " cosTetMaxElec= " << cosTetMaxElec |
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| 129 | << " screenZ= " << screenZ |
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| 130 | << " formfactA= " << formfactA << G4endl; |
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| 131 | */ |
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[961] | 132 | return xsec; |
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[819] | 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 G4CoulombScatteringModel::SampleSecondaries( |
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| 138 | std::vector<G4DynamicParticle*>* fvect, |
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| 139 | const G4MaterialCutsCouple* couple, |
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| 140 | const G4DynamicParticle* dp, |
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| 141 | G4double cutEnergy, |
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[961] | 142 | G4double) |
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[819] | 143 | { |
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| 144 | G4double kinEnergy = dp->GetKineticEnergy(); |
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[1315] | 145 | if(kinEnergy < lowEnergyLimit) { return; } |
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[961] | 146 | DefineMaterial(couple); |
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| 147 | SetupParticle(dp->GetDefinition()); |
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[819] | 148 | |
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[961] | 149 | // Choose nucleus |
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[1196] | 150 | currentElement = SelectRandomAtom(couple,particle, |
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[1315] | 151 | kinEnergy,cutEnergy,kinEnergy); |
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[961] | 152 | |
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[1315] | 153 | G4double Z = currentElement->GetZ(); |
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| 154 | G4int iz = G4int(Z); |
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| 155 | G4int ia = SelectIsotopeNumber(currentElement); |
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| 156 | G4double targetMass = G4NucleiProperties::GetNuclearMass(ia, iz); |
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| 157 | |
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| 158 | if(ComputeCrossSectionPerAtom(particle,kinEnergy, Z, |
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| 159 | kinEnergy, cutEnergy, kinEnergy) == 0.0) |
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| 160 | { return; } |
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[819] | 161 | |
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[1315] | 162 | G4ThreeVector newDirection = |
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| 163 | wokvi->SampleSingleScattering(cosTetMinNuc, cosTetMaxNuc, elecRatio); |
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[819] | 164 | |
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[1315] | 165 | // kinematics in the Lab system |
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| 166 | G4double etot = mass + kinEnergy; |
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| 167 | G4double ptot = sqrt(kinEnergy*(etot + mass)); |
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| 168 | G4double bet = ptot/(etot + targetMass); |
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| 169 | G4double gam = 1.0/sqrt((1.0 - bet)*(1.0 + bet)); |
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| 170 | G4double eCM = sqrt(mass*mass + targetMass*targetMass + 2*targetMass*etot); |
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| 171 | G4double pCM = ptot*targetMass/eCM; |
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| 172 | G4double e1 = sqrt(mass*mass + pCM*pCM); |
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[819] | 173 | |
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[1315] | 174 | newDirection *= pCM; |
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[819] | 175 | |
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[1315] | 176 | G4ThreeVector v1(newDirection.x(),newDirection.y(),gam*(newDirection.z() + bet*e1)); |
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| 177 | G4double finalT = gam*(e1 + bet*newDirection.z()) - mass; |
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| 178 | newDirection = v1.unit(); |
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[1228] | 179 | |
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[819] | 180 | G4ThreeVector dir = dp->GetMomentumDirection(); |
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| 181 | newDirection.rotateUz(dir); |
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| 182 | fParticleChange->ProposeMomentumDirection(newDirection); |
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[1196] | 183 | |
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[1315] | 184 | // recoil |
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| 185 | G4double trec = kinEnergy - finalT; |
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| 186 | if(finalT <= lowEnergyLimit) { |
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| 187 | trec = kinEnergy; |
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| 188 | finalT = 0.0; |
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| 189 | } |
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| 190 | |
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[1196] | 191 | fParticleChange->SetProposedKineticEnergy(finalT); |
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| 192 | |
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[1315] | 193 | // G4cout << "sint= " << sint << " Erec(eV)= " << erec/eV << G4endl; |
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[961] | 194 | |
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[1196] | 195 | G4double tcut = recoilThreshold; |
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| 196 | if(pCuts) { tcut= std::max(tcut,(*pCuts)[currentMaterialIndex]); } |
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[1315] | 197 | /* |
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| 198 | G4cout << "sint= " << sint << " Erec(eV)= " << erec/eV |
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| 199 | << " tcut(eV)= " << tcut/eV << " th(eV)= " << recoilThreshold/eV |
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| 200 | << " cut(eV)= " << (*pCuts)[currentMaterialIndex]/eV |
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| 201 | << " " << fvect->size() |
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| 202 | << G4endl; |
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| 203 | */ |
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| 204 | if(trec > tcut) { |
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[819] | 205 | G4ParticleDefinition* ion = theParticleTable->FindIon(iz, ia, 0, iz); |
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[1196] | 206 | G4double plab = sqrt(finalT*(finalT + 2.0*mass)); |
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[819] | 207 | G4ThreeVector p2 = (ptot*dir - plab*newDirection).unit(); |
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[1315] | 208 | G4DynamicParticle* newdp = new G4DynamicParticle(ion, p2, trec); |
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[819] | 209 | fvect->push_back(newdp); |
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[1315] | 210 | } else if(trec > 0.0) { |
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| 211 | fParticleChange->ProposeLocalEnergyDeposit(trec); |
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| 212 | fParticleChange->ProposeNonIonizingEnergyDeposit(trec); |
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[819] | 213 | } |
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| 214 | } |
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| 215 | |
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| 216 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... |
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| 217 | |
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