| 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: G4BetheBlochModel.cc,v 1.25 2009/02/20 12:06:37 vnivanch Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-02-ref-02 $
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| 28 | //
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| 29 | // -------------------------------------------------------------------
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| 30 | //
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| 31 | // GEANT4 Class header file
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| 32 | //
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| 33 | //
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| 34 | // File name: G4BetheBlochModel
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| 35 | //
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| 36 | // Author: Vladimir Ivanchenko on base of Laszlo Urban code
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| 37 | //
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| 38 | // Creation date: 03.01.2002
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| 39 | //
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| 40 | // Modifications:
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| 41 | //
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| 42 | // 04-12-02 Fix problem of G4DynamicParticle constructor (V.Ivanchenko)
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| 43 | // 23-12-02 Change interface in order to move to cut per region (V.Ivanchenko)
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| 44 | // 27-01-03 Make models region aware (V.Ivanchenko)
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| 45 | // 13-02-03 Add name (V.Ivanchenko)
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| 46 | // 24-03-05 Add G4EmCorrections (V.Ivanchenko)
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| 47 | // 11-04-05 Major optimisation of internal interfaces (V.Ivanchenko)
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| 48 | // 11-02-06 ComputeCrossSectionPerElectron, ComputeCrossSectionPerAtom (mma)
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| 49 | // 12-02-06 move G4LossTableManager::Instance()->EmCorrections()
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| 50 | // in constructor (mma)
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| 51 | // 12-08-08 Added methods GetParticleCharge, GetChargeSquareRatio,
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| 52 | // CorrectionsAlongStep needed for ions(V.Ivanchenko)
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| 53 | //
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| 54 | // -------------------------------------------------------------------
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| 55 | //
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| 56 |
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| 57 |
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| 58 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 59 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 60 |
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| 61 | #include "G4BetheBlochModel.hh"
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| 62 | #include "Randomize.hh"
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| 63 | #include "G4Electron.hh"
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| 64 | #include "G4LossTableManager.hh"
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| 65 | #include "G4EmCorrections.hh"
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| 66 | #include "G4ParticleChangeForLoss.hh"
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| 67 | #include "G4NistManager.hh"
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| 68 |
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| 69 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 70 |
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| 71 | using namespace std;
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| 72 |
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| 73 | G4BetheBlochModel::G4BetheBlochModel(const G4ParticleDefinition* p,
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| 74 | const G4String& nam)
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| 75 | : G4VEmModel(nam),
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| 76 | particle(0),
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| 77 | tlimit(DBL_MAX),
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| 78 | twoln10(2.0*log(10.0)),
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| 79 | bg2lim(0.0169),
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| 80 | taulim(8.4146e-3),
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| 81 | isIon(false),
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| 82 | isInitialised(false)
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| 83 | {
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| 84 | fParticleChange = 0;
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| 85 | if(p) SetParticle(p);
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| 86 | theElectron = G4Electron::Electron();
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| 87 | corr = G4LossTableManager::Instance()->EmCorrections();
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| 88 | nist = G4NistManager::Instance();
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| 89 | SetLowEnergyLimit(2.0*MeV);
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| 90 | }
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| 91 |
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| 92 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 93 |
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| 94 | G4BetheBlochModel::~G4BetheBlochModel()
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| 95 | {}
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| 96 |
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| 97 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 98 |
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| 99 | G4double G4BetheBlochModel::MinEnergyCut(const G4ParticleDefinition*,
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| 100 | const G4MaterialCutsCouple* couple)
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| 101 | {
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| 102 | return couple->GetMaterial()->GetIonisation()->GetMeanExcitationEnergy();
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| 103 | }
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| 104 |
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| 105 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 106 |
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| 107 | void G4BetheBlochModel::Initialise(const G4ParticleDefinition* p,
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| 108 | const G4DataVector&)
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| 109 | {
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| 110 | if (!particle) SetParticle(p);
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| 111 |
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| 112 | corrFactor = chargeSquare;
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| 113 | // always false before the run
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| 114 | SetDeexcitationFlag(false);
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| 115 |
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| 116 | if(!isInitialised) {
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| 117 | isInitialised = true;
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| 118 |
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| 119 | if(!fParticleChange) {
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| 120 | if (pParticleChange) {
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| 121 | fParticleChange = reinterpret_cast<G4ParticleChangeForLoss*>
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| 122 | (pParticleChange);
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| 123 | } else {
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| 124 | fParticleChange = new G4ParticleChangeForLoss();
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| 125 | }
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| 126 | }
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| 127 | }
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| 128 | }
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| 129 |
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| 130 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 131 |
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| 132 | void G4BetheBlochModel::SetParticle(const G4ParticleDefinition* p)
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| 133 | {
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| 134 | if(particle != p) {
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| 135 | particle = p;
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| 136 | G4String pname = particle->GetParticleName();
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| 137 | if (particle->GetParticleType() == "nucleus" &&
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| 138 | pname != "deuteron" && pname != "triton") {
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| 139 | isIon = true;
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| 140 | }
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| 141 |
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| 142 | mass = particle->GetPDGMass();
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| 143 | spin = particle->GetPDGSpin();
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| 144 | G4double q = particle->GetPDGCharge()/eplus;
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| 145 | chargeSquare = q*q;
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| 146 | ratio = electron_mass_c2/mass;
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| 147 | G4double magmom = particle->GetPDGMagneticMoment()
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| 148 | *mass/(0.5*eplus*hbar_Planck*c_squared);
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| 149 | magMoment2 = magmom*magmom - 1.0;
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| 150 | formfact = 0.0;
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| 151 | if(particle->GetLeptonNumber() == 0) {
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| 152 | G4double x = 0.8426*GeV;
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| 153 | if(spin == 0.0 && mass < GeV) {x = 0.736*GeV;}
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| 154 | else if(mass > GeV) {
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| 155 | x /= nist->GetZ13(mass/proton_mass_c2);
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| 156 | // tlimit = 51.2*GeV*A13[iz]*A13[iz];
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| 157 | }
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| 158 | formfact = 2.0*electron_mass_c2/(x*x);
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| 159 | tlimit = 2.0/formfact;
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| 160 | }
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| 161 | }
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| 162 | }
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| 163 |
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| 164 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 165 |
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| 166 | G4double G4BetheBlochModel::GetChargeSquareRatio(const G4ParticleDefinition* p,
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| 167 | const G4Material* mat,
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| 168 | G4double kineticEnergy)
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| 169 | {
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| 170 | // this method is called only for ions
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| 171 | G4double q2 = corr->EffectiveChargeSquareRatio(p,mat,kineticEnergy);
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| 172 | corrFactor = q2*corr->EffectiveChargeCorrection(p,mat,kineticEnergy);
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| 173 | return corrFactor;
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| 174 | }
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| 175 |
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| 176 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 177 |
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| 178 | G4double G4BetheBlochModel::GetParticleCharge(const G4ParticleDefinition* p,
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| 179 | const G4Material* mat,
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| 180 | G4double kineticEnergy)
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| 181 | {
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| 182 | // this method is called only for ions
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| 183 | return corr->GetParticleCharge(p,mat,kineticEnergy);
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| 184 | }
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| 185 |
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| 186 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 187 |
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| 188 | G4double
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| 189 | G4BetheBlochModel::ComputeCrossSectionPerElectron(const G4ParticleDefinition* p,
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| 190 | G4double kineticEnergy,
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| 191 | G4double cutEnergy,
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| 192 | G4double maxKinEnergy)
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| 193 | {
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| 194 | G4double cross = 0.0;
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| 195 | G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
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| 196 | G4double maxEnergy = min(tmax,maxKinEnergy);
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| 197 | if(cutEnergy < maxEnergy) {
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| 198 |
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| 199 | G4double totEnergy = kineticEnergy + mass;
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| 200 | G4double energy2 = totEnergy*totEnergy;
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| 201 | G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/energy2;
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| 202 |
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| 203 | cross = 1.0/cutEnergy - 1.0/maxEnergy
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| 204 | - beta2*log(maxEnergy/cutEnergy)/tmax;
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| 205 |
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| 206 | // +term for spin=1/2 particle
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| 207 | if( 0.5 == spin ) cross += 0.5*(maxEnergy - cutEnergy)/energy2;
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| 208 |
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| 209 | // High order correction different for hadrons and ions
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| 210 | // nevetheless they are applied to reduce high energy transfers
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| 211 | // if(!isIon)
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| 212 | //cross += corr->FiniteSizeCorrectionXS(p,currentMaterial,
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| 213 | // kineticEnergy,cutEnergy);
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| 214 |
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| 215 | cross *= twopi_mc2_rcl2*chargeSquare/beta2;
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| 216 | }
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| 217 |
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| 218 | // G4cout << "BB: e= " << kineticEnergy << " tmin= " << cutEnergy
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| 219 | // << " tmax= " << tmax << " cross= " << cross << G4endl;
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| 220 |
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| 221 | return cross;
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| 222 | }
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| 223 |
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| 224 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 225 |
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| 226 | G4double G4BetheBlochModel::ComputeCrossSectionPerAtom(
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| 227 | const G4ParticleDefinition* p,
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| 228 | G4double kineticEnergy,
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| 229 | G4double Z, G4double,
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| 230 | G4double cutEnergy,
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| 231 | G4double maxEnergy)
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| 232 | {
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| 233 | G4double cross = Z*ComputeCrossSectionPerElectron
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| 234 | (p,kineticEnergy,cutEnergy,maxEnergy);
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| 235 | return cross;
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| 236 | }
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| 237 |
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| 238 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 239 |
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| 240 | G4double G4BetheBlochModel::CrossSectionPerVolume(
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| 241 | const G4Material* material,
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| 242 | const G4ParticleDefinition* p,
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| 243 | G4double kineticEnergy,
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| 244 | G4double cutEnergy,
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| 245 | G4double maxEnergy)
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| 246 | {
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| 247 | currentMaterial = material;
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| 248 | G4double eDensity = material->GetElectronDensity();
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| 249 | G4double cross = eDensity*ComputeCrossSectionPerElectron
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| 250 | (p,kineticEnergy,cutEnergy,maxEnergy);
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| 251 | return cross;
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| 252 | }
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| 253 |
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| 254 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 255 |
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| 256 | G4double G4BetheBlochModel::ComputeDEDXPerVolume(const G4Material* material,
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| 257 | const G4ParticleDefinition* p,
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| 258 | G4double kineticEnergy,
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| 259 | G4double cut)
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| 260 | {
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| 261 | G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
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| 262 | G4double cutEnergy = min(cut,tmax);
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| 263 |
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| 264 | G4double tau = kineticEnergy/mass;
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| 265 | G4double gam = tau + 1.0;
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| 266 | G4double bg2 = tau * (tau+2.0);
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| 267 | G4double beta2 = bg2/(gam*gam);
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| 268 |
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| 269 | G4double eexc = material->GetIonisation()->GetMeanExcitationEnergy();
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| 270 | G4double eexc2 = eexc*eexc;
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| 271 | G4double cden = material->GetIonisation()->GetCdensity();
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| 272 | G4double mden = material->GetIonisation()->GetMdensity();
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| 273 | G4double aden = material->GetIonisation()->GetAdensity();
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| 274 | G4double x0den = material->GetIonisation()->GetX0density();
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| 275 | G4double x1den = material->GetIonisation()->GetX1density();
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| 276 |
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| 277 | G4double eDensity = material->GetElectronDensity();
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| 278 |
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| 279 | G4double dedx = log(2.0*electron_mass_c2*bg2*cutEnergy/eexc2)
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| 280 | - (1.0 + cutEnergy/tmax)*beta2;
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| 281 |
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| 282 | if(0.5 == spin) {
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| 283 | G4double del = 0.5*cutEnergy/(kineticEnergy + mass);
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| 284 | dedx += del*del;
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| 285 | }
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| 286 |
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| 287 | // density correction
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| 288 | G4double x = log(bg2)/twoln10;
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| 289 | if ( x >= x0den ) {
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| 290 | dedx -= twoln10*x - cden ;
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| 291 | if ( x < x1den ) dedx -= aden*pow((x1den-x),mden) ;
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| 292 | }
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| 293 |
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| 294 | // shell correction
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| 295 | dedx -= 2.0*corr->ShellCorrection(p,material,kineticEnergy);
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| 296 |
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| 297 | // now compute the total ionization loss
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| 298 |
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| 299 | if (dedx < 0.0) dedx = 0.0 ;
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| 300 |
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| 301 | dedx *= twopi_mc2_rcl2*chargeSquare*eDensity/beta2;
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| 302 |
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| 303 | //High order correction different for hadrons and ions
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| 304 | if(isIon) {
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| 305 | dedx += corr->IonBarkasCorrection(p,material,kineticEnergy);
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| 306 | } else {
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| 307 | dedx += corr->HighOrderCorrections(p,material,kineticEnergy,cutEnergy);
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| 308 | }
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| 309 | return dedx;
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| 310 | }
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| 311 |
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| 312 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 313 |
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| 314 | void G4BetheBlochModel::CorrectionsAlongStep(const G4MaterialCutsCouple* couple,
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| 315 | const G4DynamicParticle* dp,
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| 316 | G4double& eloss,
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| 317 | G4double&,
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| 318 | G4double length)
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| 319 | {
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| 320 | const G4ParticleDefinition* p = dp->GetDefinition();
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| 321 | const G4Material* mat = couple->GetMaterial();
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| 322 | G4double preKinEnergy = dp->GetKineticEnergy();
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| 323 | G4double e = preKinEnergy - eloss*0.5;
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| 324 | if(e < 0.0) e = preKinEnergy*0.5;
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| 325 |
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| 326 | if(isIon) {
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| 327 | G4double q2 = corr->EffectiveChargeSquareRatio(p,mat,e);
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| 328 | GetModelOfFluctuations()->SetParticleAndCharge(p, q2);
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| 329 | eloss *= q2*corr->EffectiveChargeCorrection(p,mat,e)/corrFactor;
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| 330 | eloss += length*corr->IonHighOrderCorrections(p,couple,e);
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| 331 | }
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| 332 |
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| 333 | if(nuclearStopping && preKinEnergy*proton_mass_c2/mass < chargeSquare*100.*MeV) {
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| 334 |
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| 335 | G4double nloss = length*corr->NuclearDEDX(p,mat,e,false);
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| 336 |
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| 337 | // too big energy loss
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| 338 | if(eloss + nloss > preKinEnergy) {
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| 339 | nloss *= (preKinEnergy/(eloss + nloss));
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| 340 | eloss = preKinEnergy;
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| 341 | } else {
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| 342 | eloss += nloss;
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| 343 | }
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| 344 | /*
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| 345 | G4cout << "G4ionIonisation::CorrectionsAlongStep: e= " << preKinEnergy
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| 346 | << " de= " << eloss << " NIEL= " << nloss
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| 347 | << " dynQ= " << dp->GetCharge()/eplus << G4endl;
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| 348 | */
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| 349 | fParticleChange->ProposeNonIonizingEnergyDeposit(nloss);
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| 350 | }
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| 351 |
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| 352 | }
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| 353 |
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| 354 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 355 |
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| 356 | void G4BetheBlochModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
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| 357 | const G4MaterialCutsCouple*,
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| 358 | const G4DynamicParticle* dp,
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| 359 | G4double minKinEnergy,
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| 360 | G4double maxEnergy)
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| 361 | {
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| 362 | G4double kineticEnergy = dp->GetKineticEnergy();
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| 363 | G4double tmax = MaxSecondaryEnergy(dp->GetDefinition(),kineticEnergy);
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| 364 |
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| 365 | G4double maxKinEnergy = std::min(maxEnergy,tmax);
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| 366 | if(minKinEnergy >= maxKinEnergy) return;
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| 367 |
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| 368 | G4double totEnergy = kineticEnergy + mass;
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| 369 | G4double etot2 = totEnergy*totEnergy;
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| 370 | G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/etot2;
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| 371 |
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| 372 | G4double deltaKinEnergy, f;
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| 373 | G4double f1 = 0.0;
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| 374 | G4double fmax = 1.0;
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| 375 | if( 0.5 == spin ) fmax += 0.5*maxKinEnergy*maxKinEnergy/etot2;
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| 376 |
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| 377 | // sampling without nuclear size effect
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| 378 | do {
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| 379 | G4double q = G4UniformRand();
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| 380 | deltaKinEnergy = minKinEnergy*maxKinEnergy
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| 381 | /(minKinEnergy*(1.0 - q) + maxKinEnergy*q);
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| 382 |
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| 383 | f = 1.0 - beta2*deltaKinEnergy/tmax;
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| 384 | if( 0.5 == spin ) {
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| 385 | f1 = 0.5*deltaKinEnergy*deltaKinEnergy/etot2;
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| 386 | f += f1;
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| 387 | }
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| 388 |
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| 389 | } while( fmax*G4UniformRand() > f);
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| 390 |
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| 391 | // projectile formfactor - suppresion of high energy
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| 392 | // delta-electron production at high energy
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| 393 |
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| 394 | G4double x = formfact*deltaKinEnergy;
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| 395 | if(x > 1.e-6) {
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| 396 |
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| 397 | G4double x1 = 1.0 + x;
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| 398 | G4double g = 1.0/(x1*x1);
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| 399 | if( 0.5 == spin ) {
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| 400 | G4double x2 = 0.5*electron_mass_c2*deltaKinEnergy/(mass*mass);
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| 401 | g *= (1.0 + magMoment2*(x2 - f1/f)/(1.0 + x2));
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| 402 | }
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| 403 | if(g > 1.0) {
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| 404 | G4cout << "### G4BetheBlochModel WARNING: g= " << g
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| 405 | << dp->GetDefinition()->GetParticleName()
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| 406 | << " Ekin(MeV)= " << kineticEnergy
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| 407 | << " delEkin(MeV)= " << deltaKinEnergy
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| 408 | << G4endl;
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| 409 | }
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| 410 | if(G4UniformRand() > g) return;
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| 411 | }
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| 412 |
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| 413 | // delta-electron is produced
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| 414 | G4double totMomentum = totEnergy*sqrt(beta2);
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| 415 | G4double deltaMomentum =
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| 416 | sqrt(deltaKinEnergy * (deltaKinEnergy + 2.0*electron_mass_c2));
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| 417 | G4double cost = deltaKinEnergy * (totEnergy + electron_mass_c2) /
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| 418 | (deltaMomentum * totMomentum);
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| 419 | if(cost > 1.0) {
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| 420 | G4cout << "### G4BetheBlochModel WARNING: cost= "
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| 421 | << cost << " > 1 for "
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| 422 | << dp->GetDefinition()->GetParticleName()
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| 423 | << " Ekin(MeV)= " << kineticEnergy
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| 424 | << " p(MeV/c)= " << totMomentum
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| 425 | << " delEkin(MeV)= " << deltaKinEnergy
|
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| 426 | << " delMom(MeV/c)= " << deltaMomentum
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| 427 | << " tmin(MeV)= " << minKinEnergy
|
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| 428 | << " tmax(MeV)= " << maxKinEnergy
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| 429 | << " dir= " << dp->GetMomentumDirection()
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| 430 | << G4endl;
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| 431 | cost = 1.0;
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| 432 | }
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| 433 | G4double sint = sqrt((1.0 - cost)*(1.0 + cost));
|
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| 434 |
|
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| 435 | G4double phi = twopi * G4UniformRand() ;
|
|---|
| 436 |
|
|---|
| 437 |
|
|---|
| 438 | G4ThreeVector deltaDirection(sint*cos(phi),sint*sin(phi), cost);
|
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| 439 | G4ThreeVector direction = dp->GetMomentumDirection();
|
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| 440 | deltaDirection.rotateUz(direction);
|
|---|
| 441 |
|
|---|
| 442 | // create G4DynamicParticle object for delta ray
|
|---|
| 443 | G4DynamicParticle* delta = new G4DynamicParticle(theElectron,
|
|---|
| 444 | deltaDirection,deltaKinEnergy);
|
|---|
| 445 |
|
|---|
| 446 | vdp->push_back(delta);
|
|---|
| 447 |
|
|---|
| 448 | // Change kinematics of primary particle
|
|---|
| 449 | kineticEnergy -= deltaKinEnergy;
|
|---|
| 450 | G4ThreeVector finalP = direction*totMomentum - deltaDirection*deltaMomentum;
|
|---|
| 451 | finalP = finalP.unit();
|
|---|
| 452 |
|
|---|
| 453 | fParticleChange->SetProposedKineticEnergy(kineticEnergy);
|
|---|
| 454 | fParticleChange->SetProposedMomentumDirection(finalP);
|
|---|
| 455 | }
|
|---|
| 456 |
|
|---|
| 457 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
|
|---|
| 458 |
|
|---|
| 459 | G4double G4BetheBlochModel::MaxSecondaryEnergy(const G4ParticleDefinition* pd,
|
|---|
| 460 | G4double kinEnergy)
|
|---|
| 461 | {
|
|---|
| 462 | if(isIon) SetParticle(pd);
|
|---|
| 463 | G4double tau = kinEnergy/mass;
|
|---|
| 464 | G4double tmax = 2.0*electron_mass_c2*tau*(tau + 2.) /
|
|---|
| 465 | (1. + 2.0*(tau + 1.)*ratio + ratio*ratio);
|
|---|
| 466 | return std::min(tmax,tlimit);
|
|---|
| 467 | }
|
|---|
| 468 |
|
|---|
| 469 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
|
|---|