| 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: G4PolarizedAnnihilationModel.cc,v 1.6 2007/07/10 09:38:17 schaelic Exp $
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| 27 | // GEANT4 tag $Name: $
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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: G4PolarizedAnnihilationModel
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| 35 | //
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| 36 | // Author: Andreas Schaelicke
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| 37 | //
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| 38 | // Creation date: 01.05.2005
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| 39 | //
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| 40 | // Modifications:
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| 41 | // 18-07-06 use newly calculated cross sections (P. Starovoitov)
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| 42 | // 21-08-06 update interface (A. Schaelicke)
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| 43 | // 17-11-06 add protection agaist e+ zero energy PostStep (V.Ivanchenko)
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| 44 | // 10-07-07 copied Initialise() method from G4eeToTwoGammaModel to provide a
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| 45 | // local ParticleChangeForGamma object and reduce overhead
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| 46 | // in SampleSecondaries() (A. Schaelicke)
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| 47 | //
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| 48 | //
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| 49 | // Class Description:
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| 50 | //
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| 51 | // Implementation of polarized gamma Annihilation scattering on free electron
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| 52 | //
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| 53 |
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| 54 | // -------------------------------------------------------------------
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| 55 | #include "G4PolarizedAnnihilationModel.hh"
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| 56 | #include "G4PolarizationManager.hh"
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| 57 | #include "G4PolarizationHelper.hh"
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| 58 | #include "G4StokesVector.hh"
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| 59 | #include "G4PolarizedAnnihilationCrossSection.hh"
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| 60 | #include "G4ParticleChangeForGamma.hh"
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| 61 | #include "G4TrackStatus.hh"
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| 62 | #include "G4Gamma.hh"
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| 63 |
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| 64 | G4PolarizedAnnihilationModel::G4PolarizedAnnihilationModel(const G4ParticleDefinition* p,
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| 65 | const G4String& nam)
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| 66 | : G4eeToTwoGammaModel(p,nam),crossSectionCalculator(0),gParticleChange(0),
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| 67 | gIsInitialised(false)
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| 68 | {
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| 69 | crossSectionCalculator=new G4PolarizedAnnihilationCrossSection();
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| 70 | }
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| 71 |
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| 72 | G4PolarizedAnnihilationModel::~G4PolarizedAnnihilationModel()
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| 73 | {
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| 74 | if (crossSectionCalculator) delete crossSectionCalculator;
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| 75 | }
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| 76 |
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| 77 |
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| 78 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 79 |
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| 80 | void G4PolarizedAnnihilationModel::Initialise(const G4ParticleDefinition*,
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| 81 | const G4DataVector&)
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| 82 | {
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| 83 | // G4eeToTwoGammaModel::Initialise(part,dv);
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| 84 | if(gIsInitialised) return;
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| 85 |
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| 86 | if(pParticleChange)
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| 87 | gParticleChange =
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| 88 | reinterpret_cast<G4ParticleChangeForGamma*>(pParticleChange);
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| 89 | else
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| 90 | gParticleChange = new G4ParticleChangeForGamma();
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| 91 |
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| 92 | gIsInitialised = true;
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| 93 | }
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| 94 |
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| 95 | G4double G4PolarizedAnnihilationModel::ComputeCrossSectionPerElectron(
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| 96 | const G4ParticleDefinition* pd,
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| 97 | G4double kinEnergy,
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| 98 | G4double cut,
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| 99 | G4double emax)
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| 100 | {
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| 101 | G4double xs = G4eeToTwoGammaModel::ComputeCrossSectionPerElectron(pd,kinEnergy,
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| 102 | cut,emax);
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| 103 |
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| 104 | G4double polzz = theBeamPolarization.z()*theTargetPolarization.z();
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| 105 | G4double poltt = theBeamPolarization.x()*theTargetPolarization.x()
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| 106 | + theBeamPolarization.y()*theTargetPolarization.y();
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| 107 | if (polzz!=0 || poltt!=0) {
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| 108 | G4double xval,lasym,tasym;
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| 109 | ComputeAsymmetriesPerElectron(kinEnergy,xval,lasym,tasym);
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| 110 | xs*=(1.+polzz*lasym+poltt*tasym);
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| 111 | }
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| 112 |
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| 113 | return xs;
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| 114 | }
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| 115 |
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| 116 | void G4PolarizedAnnihilationModel::ComputeAsymmetriesPerElectron(G4double ene,
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| 117 | G4double & valueX,
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| 118 | G4double & valueA,
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| 119 | G4double & valueT)
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| 120 | {
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| 121 | // *** calculate asymmetries
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| 122 | G4double gam = 1. + ene/electron_mass_c2;
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| 123 | G4double xs0=crossSectionCalculator->TotalXSection(0.,1.,gam,
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| 124 | G4StokesVector::ZERO,
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| 125 | G4StokesVector::ZERO);
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| 126 | G4double xsA=crossSectionCalculator->TotalXSection(0.,1.,gam,
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| 127 | G4StokesVector::P3,
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| 128 | G4StokesVector::P3);
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| 129 | G4double xsT1=crossSectionCalculator->TotalXSection(0.,1.,gam,
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| 130 | G4StokesVector::P1,
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| 131 | G4StokesVector::P1);
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| 132 | G4double xsT2=crossSectionCalculator->TotalXSection(0.,1.,gam,
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| 133 | G4StokesVector::P2,
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| 134 | G4StokesVector::P2);
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| 135 | G4double xsT=0.5*(xsT1+xsT2);
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| 136 |
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| 137 | valueX=xs0;
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| 138 | valueA=xsA/xs0-1.;
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| 139 | valueT=xsT/xs0-1.;
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| 140 | // G4cout<<valueX<<"\t"<<valueA<<"\t"<<valueT<<" energy = "<<gam<<G4endl;
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| 141 | if ( (valueA < -1) || (1 < valueA)) {
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| 142 | G4cout<< " ERROR PolarizedAnnihilationPS::ComputeAsymmetries \n";
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| 143 | G4cout<< " something wrong in total cross section calculation (valueA)\n";
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| 144 | G4cout<<"*********** LONG "<<valueX<<"\t"<<valueA<<"\t"<<valueT<<" energy = "<<gam<<G4endl;
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| 145 | }
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| 146 | if ( (valueT < -1) || (1 < valueT)) {
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| 147 | G4cout<< " ERROR PolarizedAnnihilationPS::ComputeAsymmetries \n";
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| 148 | G4cout<< " something wrong in total cross section calculation (valueT)\n";
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| 149 | G4cout<<"****** TRAN "<<valueX<<"\t"<<valueA<<"\t"<<valueT<<" energy = "<<gam<<G4endl;
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| 150 | }
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| 151 | }
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| 152 |
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| 153 |
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| 154 | void G4PolarizedAnnihilationModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
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| 155 | const G4MaterialCutsCouple* /*couple*/,
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| 156 | const G4DynamicParticle* dp,
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| 157 | G4double /*tmin*/,
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| 158 | G4double /*maxEnergy*/)
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| 159 | {
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| 160 | // G4ParticleChangeForGamma* gParticleChange
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| 161 | // = dynamic_cast<G4ParticleChangeForGamma*>(pParticleChange);
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| 162 | const G4Track * aTrack = gParticleChange->GetCurrentTrack();
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| 163 |
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| 164 | // kill primary
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| 165 | gParticleChange->SetProposedKineticEnergy(0.);
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| 166 | gParticleChange->ProposeTrackStatus(fStopAndKill);
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| 167 |
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| 168 | // V.Ivanchenko add protection against zero kin energy
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| 169 | G4double PositKinEnergy = dp->GetKineticEnergy();
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| 170 |
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| 171 | if(PositKinEnergy < DBL_MIN) {
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| 172 |
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| 173 | G4double cosTeta = 2.*G4UniformRand()-1.;
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| 174 | G4double sinTeta = std::sqrt((1.0 - cosTeta)*(1.0 + cosTeta));
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| 175 | G4double phi = twopi * G4UniformRand();
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| 176 | G4ThreeVector dir(sinTeta*std::cos(phi), sinTeta*std::sin(phi), cosTeta);
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| 177 | fvect->push_back( new G4DynamicParticle(G4Gamma::Gamma(), dir, electron_mass_c2));
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| 178 | fvect->push_back( new G4DynamicParticle(G4Gamma::Gamma(),-dir, electron_mass_c2));
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| 179 | return;
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| 180 | }
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| 181 |
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| 182 | // *** obtain and save target and beam polarization ***
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| 183 | G4PolarizationManager * polarizationManager = G4PolarizationManager::GetInstance();
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| 184 |
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| 185 | // obtain polarization of the beam
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| 186 | theBeamPolarization = aTrack->GetPolarization();
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| 187 |
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| 188 | // obtain polarization of the media
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| 189 | G4VPhysicalVolume* aPVolume = aTrack->GetVolume();
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| 190 | G4LogicalVolume* aLVolume = aPVolume->GetLogicalVolume();
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| 191 | const G4bool targetIsPolarized = polarizationManager->IsPolarized(aLVolume);
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| 192 | theTargetPolarization = polarizationManager->GetVolumePolarization(aLVolume);
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| 193 |
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| 194 | // transfer target electron polarization in frame of positron
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| 195 | if (targetIsPolarized)
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| 196 | theTargetPolarization.rotateUz(dp->GetMomentumDirection());
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| 197 |
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| 198 | G4ParticleMomentum PositDirection = dp->GetMomentumDirection();
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| 199 |
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| 200 | // polar asymmetry:
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| 201 | G4double polarization = theBeamPolarization.p3()*theTargetPolarization.p3();
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| 202 |
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| 203 | G4double gamam1 = PositKinEnergy/electron_mass_c2;
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| 204 | G4double gama = gamam1+1. , gamap1 = gamam1+2.;
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| 205 | G4double sqgrate = std::sqrt(gamam1/gamap1)/2. , sqg2m1 = std::sqrt(gamam1*gamap1);
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| 206 |
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| 207 | // limits of the energy sampling
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| 208 | G4double epsilmin = 0.5 - sqgrate , epsilmax = 0.5 + sqgrate;
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| 209 | G4double epsilqot = epsilmax/epsilmin;
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| 210 |
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| 211 | //
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| 212 | // sample the energy rate of the created gammas
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| 213 | // note: for polarized partices, the actual dicing strategy
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| 214 | // will depend on the energy, and the degree of polarization !!
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| 215 | //
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| 216 | G4double epsil;
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| 217 | G4double gmax=1. + std::fabs(polarization); // crude estimate
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| 218 |
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| 219 | G4bool check_range=true;
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| 220 |
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| 221 | crossSectionCalculator->Initialize(epsilmin, gama, 0., theBeamPolarization, theTargetPolarization);
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| 222 | if (crossSectionCalculator->DiceEpsilon()<0) {
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| 223 | G4cout<<"ERROR in PolarizedAnnihilationPS::PostStepDoIt\n"
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| 224 | <<"epsilmin DiceRoutine not appropriate ! "<<crossSectionCalculator->DiceEpsilon()<<G4endl;
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| 225 | check_range=false;
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| 226 | }
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| 227 |
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| 228 | crossSectionCalculator->Initialize(epsilmax, gama, 0., theBeamPolarization, theTargetPolarization);
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| 229 | if (crossSectionCalculator->DiceEpsilon()<0) {
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| 230 | G4cout<<"ERROR in PolarizedAnnihilationPS::PostStepDoIt\n"
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| 231 | <<"epsilmax DiceRoutine not appropriate ! "<<crossSectionCalculator->DiceEpsilon()<<G4endl;
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| 232 | check_range=false;
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| 233 | }
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| 234 |
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| 235 | G4int ncount=0;
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| 236 | G4double trejectmax=0.;
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| 237 | G4double treject;
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| 238 |
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| 239 |
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| 240 | do {
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| 241 | //
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| 242 | epsil = epsilmin*std::pow(epsilqot,G4UniformRand());
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| 243 |
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| 244 | crossSectionCalculator->Initialize(epsil, gama, 0., theBeamPolarization, theTargetPolarization,1);
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| 245 |
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| 246 | treject = crossSectionCalculator->DiceEpsilon();
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| 247 | treject*=epsil;
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| 248 |
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| 249 | if (treject>gmax || treject<0.)
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| 250 | G4cout<<"ERROR in PolarizedAnnihilationPS::PostStepDoIt\n"
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| 251 | <<" eps ("<<epsil<<") rejection does not work properly: "<<treject<<G4endl;
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| 252 | ++ncount;
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| 253 | if (treject>trejectmax) trejectmax=treject;
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| 254 | if (ncount>1000) {
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| 255 | G4cout<<"WARNING in PolarizedAnnihilationPS::PostStepDoIt\n"
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| 256 | <<"eps dicing very inefficient ="<<trejectmax/gmax
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| 257 | <<", "<<treject/gmax<<". For secondary energy = "<<epsil<<" "<<ncount<<G4endl;
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| 258 | break;
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| 259 | }
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| 260 |
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| 261 | } while( treject < gmax*G4UniformRand() );
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| 262 |
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| 263 | //
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| 264 | // scattered Gamma angles. ( Z - axis along the parent positron)
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| 265 | //
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| 266 |
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| 267 | G4double cost = (epsil*gamap1-1.)/(epsil*sqg2m1);
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| 268 | G4double sint = std::sqrt((1.+cost)*(1.-cost));
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| 269 | G4double phi = 0.;
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| 270 | G4double beamTrans = std::sqrt(sqr(theBeamPolarization.p1()) + sqr(theBeamPolarization.p2()));
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| 271 | G4double targetTrans = std::sqrt(sqr(theTargetPolarization.p1()) + sqr(theTargetPolarization.p2()));
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| 272 |
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| 273 | // G4cout<<"phi dicing START"<<G4endl;
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| 274 | do{
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| 275 | phi = twopi * G4UniformRand();
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| 276 | crossSectionCalculator->Initialize(epsil, gama, 0., theBeamPolarization, theTargetPolarization,2);
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| 277 |
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| 278 | G4double gdiced =crossSectionCalculator->getVar(0);
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| 279 | gdiced += crossSectionCalculator->getVar(3)*theBeamPolarization.p3()*theTargetPolarization.p3();
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| 280 | gdiced += 1.*(std::fabs(crossSectionCalculator->getVar(1))
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| 281 | + std::fabs(crossSectionCalculator->getVar(2)))*beamTrans*targetTrans;
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| 282 | gdiced += 1.*std::fabs(crossSectionCalculator->getVar(4))
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| 283 | *(std::fabs(theBeamPolarization.p3())*targetTrans + std::fabs(theTargetPolarization.p3())*beamTrans);
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| 284 |
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| 285 | G4double gdist = crossSectionCalculator->getVar(0);
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| 286 | gdist += crossSectionCalculator->getVar(3)*theBeamPolarization.p3()*theTargetPolarization.p3();
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| 287 | gdist += crossSectionCalculator->getVar(1)*(std::cos(phi)*theBeamPolarization.p1()
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| 288 | + std::sin(phi)*theBeamPolarization.p2())
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| 289 | *(std::cos(phi)*theTargetPolarization.p1()
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| 290 | + std::sin(phi)*theTargetPolarization.p2());
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| 291 | gdist += crossSectionCalculator->getVar(2)*(std::cos(phi)*theBeamPolarization.p2()
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| 292 | - std::sin(phi)*theBeamPolarization.p1())
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| 293 | *(std::cos(phi)*theTargetPolarization.p2()
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| 294 | - std::sin(phi)*theTargetPolarization.p1());
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| 295 | gdist += crossSectionCalculator->getVar(4)
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| 296 | *(std::cos(phi)*theBeamPolarization.p3()*theTargetPolarization.p1()
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| 297 | + std::cos(phi)*theBeamPolarization.p1()*theTargetPolarization.p3()
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| 298 | + std::sin(phi)*theBeamPolarization.p3()*theTargetPolarization.p2()
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| 299 | + std::sin(phi)*theBeamPolarization.p2()*theTargetPolarization.p3());
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| 300 |
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| 301 | treject = gdist/gdiced;
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| 302 | //G4cout<<" treject = "<<treject<<" at phi = "<<phi<<G4endl;
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| 303 | if (treject>1.+1.e-10 || treject<0){
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| 304 | G4cout<<"!!!ERROR in PolarizedAnnihilationPS::PostStepDoIt\n"
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| 305 | <<" phi rejection does not work properly: "<<treject<<G4endl;
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| 306 | G4cout<<" gdiced = "<<gdiced<<G4endl;
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| 307 | G4cout<<" gdist = "<<gdist<<G4endl;
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| 308 | G4cout<<" epsil = "<<epsil<<G4endl;
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| 309 | }
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| 310 |
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| 311 | if (treject<1.e-3) {
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| 312 | G4cout<<"!!!ERROR in PolarizedAnnihilationPS::PostStepDoIt\n"
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| 313 | <<" phi rejection does not work properly: "<<treject<<"\n";
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| 314 | G4cout<<" gdiced="<<gdiced<<" gdist="<<gdist<<"\n";
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| 315 | G4cout<<" epsil = "<<epsil<<G4endl;
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| 316 | }
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| 317 |
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| 318 | } while( treject < G4UniformRand() );
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| 319 | // G4cout<<"phi dicing END"<<G4endl;
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| 320 |
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| 321 | G4double dirx = sint*std::cos(phi) , diry = sint*std::sin(phi) , dirz = cost;
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| 322 |
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| 323 | //
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| 324 | // kinematic of the created pair
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| 325 | //
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| 326 | G4double TotalAvailableEnergy = PositKinEnergy + 2*electron_mass_c2;
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| 327 | G4double Phot1Energy = epsil*TotalAvailableEnergy;
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| 328 | G4double Phot2Energy =(1.-epsil)*TotalAvailableEnergy;
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| 329 |
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| 330 | // *** prepare calculation of polarization transfer ***
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| 331 | G4ThreeVector Phot1Direction (dirx, diry, dirz);
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| 332 |
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| 333 | // get interaction frame
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| 334 | G4ThreeVector nInteractionFrame =
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| 335 | G4PolarizationHelper::GetFrame(PositDirection,Phot1Direction);
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| 336 |
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| 337 | // define proper in-plane and out-of-plane component of initial spins
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| 338 | theBeamPolarization.InvRotateAz(nInteractionFrame,PositDirection);
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| 339 | theTargetPolarization.InvRotateAz(nInteractionFrame,PositDirection);
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| 340 |
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| 341 | // calculate spin transfere matrix
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| 342 |
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| 343 | crossSectionCalculator->Initialize(epsil,gama,phi,theBeamPolarization,theTargetPolarization,2);
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| 344 |
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| 345 | // **********************************************************************
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| 346 |
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| 347 | Phot1Direction.rotateUz(PositDirection);
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| 348 | // create G4DynamicParticle object for the particle1
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| 349 | G4DynamicParticle* aParticle1= new G4DynamicParticle (G4Gamma::Gamma(),
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| 350 | Phot1Direction, Phot1Energy);
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| 351 | finalGamma1Polarization=crossSectionCalculator->GetPol2();
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| 352 | G4double n1=finalGamma1Polarization.mag2();
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| 353 | if (n1>1) {
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| 354 | G4cout<<"ERROR: PolarizedAnnihilation Polarization Vector at epsil = "
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| 355 | <<epsil<<" is too large!!! \n"
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| 356 | <<"annihi pol1= "<<finalGamma1Polarization<<", ("<<n1<<")\n";
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| 357 | finalGamma1Polarization+=1./std::sqrt(n1);
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| 358 | }
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| 359 |
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| 360 | // define polarization of first final state photon
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| 361 | finalGamma1Polarization.SetPhoton();
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| 362 | finalGamma1Polarization.RotateAz(nInteractionFrame,Phot1Direction);
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| 363 | aParticle1->SetPolarization(finalGamma1Polarization.p1(),
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| 364 | finalGamma1Polarization.p2(),
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| 365 | finalGamma1Polarization.p3());
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| 366 |
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| 367 | fvect->push_back(aParticle1);
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| 368 |
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| 369 |
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| 370 | // **********************************************************************
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| 371 |
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| 372 | G4double Eratio= Phot1Energy/Phot2Energy;
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| 373 | G4double PositP= std::sqrt(PositKinEnergy*(PositKinEnergy+2.*electron_mass_c2));
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| 374 | G4ThreeVector Phot2Direction (-dirx*Eratio, -diry*Eratio,
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| 375 | (PositP-dirz*Phot1Energy)/Phot2Energy);
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| 376 | Phot2Direction.rotateUz(PositDirection);
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| 377 | // create G4DynamicParticle object for the particle2
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| 378 | G4DynamicParticle* aParticle2= new G4DynamicParticle (G4Gamma::Gamma(),
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| 379 | Phot2Direction, Phot2Energy);
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| 380 |
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| 381 | // define polarization of second final state photon
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| 382 | finalGamma2Polarization=crossSectionCalculator->GetPol3();
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| 383 | G4double n2=finalGamma2Polarization.mag2();
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| 384 | if (n2>1) {
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| 385 | G4cout<<"ERROR: PolarizedAnnihilation Polarization Vector at epsil = "<<epsil<<" is too large!!! \n";
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| 386 | G4cout<<"annihi pol2= "<<finalGamma2Polarization<<", ("<<n2<<")\n";
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| 387 |
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| 388 | finalGamma2Polarization+=1./std::sqrt(n2);
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| 389 | }
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| 390 | finalGamma2Polarization.SetPhoton();
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| 391 | finalGamma2Polarization.RotateAz(nInteractionFrame,Phot2Direction);
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| 392 | aParticle2->SetPolarization(finalGamma2Polarization.p1(),
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| 393 | finalGamma2Polarization.p2(),
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| 394 | finalGamma2Polarization.p3());
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| 395 |
|
|---|
| 396 | fvect->push_back(aParticle2);
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| 397 | }
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