[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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| 26 | // |
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| 27 | // $Id: G4LowEnergyPolarizedCompton.cc,v 1.22 2006/06/29 19:40:25 gunter Exp $ |
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| 28 | // GEANT4 tag $Name: $ |
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| 29 | // |
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| 30 | // ------------------------------------------------------------ |
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| 31 | // GEANT 4 class implementation file |
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| 32 | // CERN Geneva Switzerland |
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| 33 | // |
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| 34 | |
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| 35 | // --------- G4LowEnergyPolarizedCompton class ----- |
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| 36 | // |
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| 37 | // by G.Depaola & F.Longo (21 may 2001) |
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| 38 | // |
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| 39 | // 21 May 2001 - MGP Modified to inherit from G4VDiscreteProcess |
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| 40 | // Applies same algorithm as LowEnergyCompton |
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| 41 | // if the incoming photon is not polarised |
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| 42 | // Temporary protection to avoid crash in the case |
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| 43 | // of polarisation || incident photon direction |
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| 44 | // |
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| 45 | // 17 October 2001 - F.Longo - Revised according to a design iteration |
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| 46 | // |
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| 47 | // 21 February 2002 - F.Longo Revisions with A.Zoglauer and G.Depaola |
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| 48 | // - better description of parallelism |
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| 49 | // - system of ref change method improved |
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| 50 | // 22 January 2003 - V.Ivanchenko Cut per region |
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| 51 | // 24 April 2003 - V.Ivanchenko Cut per region mfpt |
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| 52 | // |
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| 53 | // |
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| 54 | // ************************************************************ |
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| 55 | // |
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| 56 | // Corrections by Rui Curado da Silva (2000) |
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| 57 | // New Implementation by G.Depaola & F.Longo |
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| 58 | // |
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| 59 | // - sampling of phi |
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| 60 | // - polarization of scattered photon |
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| 61 | // |
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| 62 | // -------------------------------------------------------------- |
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| 63 | |
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| 64 | #include "G4LowEnergyPolarizedCompton.hh" |
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| 65 | #include "Randomize.hh" |
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| 66 | #include "G4ParticleDefinition.hh" |
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| 67 | #include "G4Track.hh" |
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| 68 | #include "G4Step.hh" |
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| 69 | #include "G4ForceCondition.hh" |
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| 70 | #include "G4Gamma.hh" |
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| 71 | #include "G4Electron.hh" |
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| 72 | #include "G4DynamicParticle.hh" |
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| 73 | #include "G4VParticleChange.hh" |
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| 74 | #include "G4ThreeVector.hh" |
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| 75 | #include "G4VCrossSectionHandler.hh" |
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| 76 | #include "G4CrossSectionHandler.hh" |
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| 77 | #include "G4VEMDataSet.hh" |
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| 78 | #include "G4CompositeEMDataSet.hh" |
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| 79 | #include "G4VDataSetAlgorithm.hh" |
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| 80 | #include "G4LogLogInterpolation.hh" |
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| 81 | #include "G4VRangeTest.hh" |
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| 82 | #include "G4RangeTest.hh" |
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| 83 | #include "G4MaterialCutsCouple.hh" |
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| 84 | |
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| 85 | // constructor |
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| 86 | |
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| 87 | G4LowEnergyPolarizedCompton::G4LowEnergyPolarizedCompton(const G4String& processName) |
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| 88 | : G4VDiscreteProcess(processName), |
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| 89 | lowEnergyLimit (250*eV), // initialization |
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| 90 | highEnergyLimit(100*GeV), |
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| 91 | intrinsicLowEnergyLimit(10*eV), |
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| 92 | intrinsicHighEnergyLimit(100*GeV) |
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| 93 | { |
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| 94 | if (lowEnergyLimit < intrinsicLowEnergyLimit || |
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| 95 | highEnergyLimit > intrinsicHighEnergyLimit) |
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| 96 | { |
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| 97 | G4Exception("G4LowEnergyPolarizedCompton::G4LowEnergyPolarizedCompton - energy outside intrinsic process validity range"); |
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| 98 | } |
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| 99 | |
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| 100 | crossSectionHandler = new G4CrossSectionHandler; |
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| 101 | |
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| 102 | |
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| 103 | G4VDataSetAlgorithm* scatterInterpolation = new G4LogLogInterpolation; |
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| 104 | G4String scatterFile = "comp/ce-sf-"; |
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| 105 | scatterFunctionData = new G4CompositeEMDataSet(scatterInterpolation,1.,1.); |
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| 106 | scatterFunctionData->LoadData(scatterFile); |
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| 107 | |
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| 108 | meanFreePathTable = 0; |
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| 109 | |
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| 110 | rangeTest = new G4RangeTest; |
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| 111 | |
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| 112 | if (verboseLevel > 0) |
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| 113 | { |
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| 114 | G4cout << GetProcessName() << " is created " << G4endl |
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| 115 | << "Energy range: " |
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| 116 | << lowEnergyLimit / keV << " keV - " |
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| 117 | << highEnergyLimit / GeV << " GeV" |
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| 118 | << G4endl; |
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| 119 | } |
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| 120 | } |
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| 121 | |
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| 122 | // destructor |
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| 123 | |
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| 124 | G4LowEnergyPolarizedCompton::~G4LowEnergyPolarizedCompton() |
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| 125 | { |
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| 126 | delete meanFreePathTable; |
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| 127 | delete crossSectionHandler; |
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| 128 | delete scatterFunctionData; |
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| 129 | delete rangeTest; |
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| 130 | } |
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| 131 | |
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| 132 | |
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| 133 | void G4LowEnergyPolarizedCompton::BuildPhysicsTable(const G4ParticleDefinition& ) |
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| 134 | { |
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| 135 | |
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| 136 | crossSectionHandler->Clear(); |
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| 137 | G4String crossSectionFile = "comp/ce-cs-"; |
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| 138 | crossSectionHandler->LoadData(crossSectionFile); |
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| 139 | delete meanFreePathTable; |
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| 140 | meanFreePathTable = crossSectionHandler->BuildMeanFreePathForMaterials(); |
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| 141 | } |
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| 142 | |
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| 143 | G4VParticleChange* G4LowEnergyPolarizedCompton::PostStepDoIt(const G4Track& aTrack, |
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| 144 | const G4Step& aStep) |
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| 145 | { |
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| 146 | // The scattered gamma energy is sampled according to Klein - Nishina formula. |
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| 147 | // The random number techniques of Butcher & Messel are used (Nuc Phys 20(1960),15). |
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| 148 | // GEANT4 internal units |
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| 149 | // |
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| 150 | // Note : Effects due to binding of atomic electrons are negliged. |
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| 151 | |
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| 152 | aParticleChange.Initialize(aTrack); |
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| 153 | |
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| 154 | // Dynamic particle quantities |
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| 155 | const G4DynamicParticle* incidentPhoton = aTrack.GetDynamicParticle(); |
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| 156 | G4double gammaEnergy0 = incidentPhoton->GetKineticEnergy(); |
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| 157 | G4ThreeVector gammaPolarization0 = incidentPhoton->GetPolarization(); |
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| 158 | |
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| 159 | // gammaPolarization0 = gammaPolarization0.unit(); // |
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| 160 | |
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| 161 | // Protection: a polarisation parallel to the |
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| 162 | // direction causes problems; |
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| 163 | // in that case find a random polarization |
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| 164 | |
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| 165 | G4ThreeVector gammaDirection0 = incidentPhoton->GetMomentumDirection(); |
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| 166 | // ---- MGP ---- Next two lines commented out to remove compilation warnings |
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| 167 | // G4double scalarproduct = gammaPolarization0.dot(gammaDirection0); |
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| 168 | // G4double angle = gammaPolarization0.angle(gammaDirection0); |
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| 169 | |
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| 170 | // Make sure that the polarization vector is perpendicular to the |
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| 171 | // gamma direction. If not |
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| 172 | |
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| 173 | if(!(gammaPolarization0.isOrthogonal(gammaDirection0, 1e-6))||(gammaPolarization0.mag()==0)) |
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| 174 | { // only for testing now |
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| 175 | gammaPolarization0 = GetRandomPolarization(gammaDirection0); |
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| 176 | } |
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| 177 | else |
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| 178 | { |
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| 179 | if ( gammaPolarization0.howOrthogonal(gammaDirection0) != 0) |
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| 180 | { |
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| 181 | gammaPolarization0 = GetPerpendicularPolarization(gammaDirection0, gammaPolarization0); |
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| 182 | } |
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| 183 | } |
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| 184 | |
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| 185 | // End of Protection |
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| 186 | |
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| 187 | // Within energy limit? |
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| 188 | |
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| 189 | if(gammaEnergy0 <= lowEnergyLimit) |
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| 190 | { |
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| 191 | aParticleChange.ProposeTrackStatus(fStopAndKill); |
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| 192 | aParticleChange.ProposeEnergy(0.); |
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| 193 | aParticleChange.ProposeLocalEnergyDeposit(gammaEnergy0); |
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| 194 | return G4VDiscreteProcess::PostStepDoIt(aTrack,aStep); |
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| 195 | } |
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| 196 | |
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| 197 | G4double E0_m = gammaEnergy0 / electron_mass_c2 ; |
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| 198 | |
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| 199 | // Select randomly one element in the current material |
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| 200 | |
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| 201 | const G4MaterialCutsCouple* couple = aTrack.GetMaterialCutsCouple(); |
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| 202 | G4int Z = crossSectionHandler->SelectRandomAtom(couple,gammaEnergy0); |
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| 203 | |
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| 204 | // Sample the energy and the polarization of the scattered photon |
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| 205 | |
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| 206 | G4double epsilon, epsilonSq, onecost, sinThetaSqr, greject ; |
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| 207 | |
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| 208 | G4double epsilon0 = 1./(1. + 2*E0_m); |
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| 209 | G4double epsilon0Sq = epsilon0*epsilon0; |
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| 210 | G4double alpha1 = - std::log(epsilon0); |
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| 211 | G4double alpha2 = 0.5*(1.- epsilon0Sq); |
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| 212 | |
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| 213 | G4double wlGamma = h_Planck*c_light/gammaEnergy0; |
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| 214 | G4double gammaEnergy1; |
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| 215 | G4ThreeVector gammaDirection1; |
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| 216 | |
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| 217 | do { |
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| 218 | if ( alpha1/(alpha1+alpha2) > G4UniformRand() ) |
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| 219 | { |
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| 220 | epsilon = std::exp(-alpha1*G4UniformRand()); |
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| 221 | epsilonSq = epsilon*epsilon; |
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| 222 | } |
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| 223 | else |
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| 224 | { |
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| 225 | epsilonSq = epsilon0Sq + (1.- epsilon0Sq)*G4UniformRand(); |
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| 226 | epsilon = std::sqrt(epsilonSq); |
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| 227 | } |
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| 228 | |
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| 229 | onecost = (1.- epsilon)/(epsilon*E0_m); |
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| 230 | sinThetaSqr = onecost*(2.-onecost); |
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| 231 | |
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| 232 | // Protection |
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| 233 | if (sinThetaSqr > 1.) |
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| 234 | { |
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| 235 | if (verboseLevel>0) G4cout |
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| 236 | << " -- Warning -- G4LowEnergyPolarizedCompton::PostStepDoIt " |
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| 237 | << "sin(theta)**2 = " |
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| 238 | << sinThetaSqr |
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| 239 | << "; set to 1" |
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| 240 | << G4endl; |
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| 241 | sinThetaSqr = 1.; |
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| 242 | } |
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| 243 | if (sinThetaSqr < 0.) |
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| 244 | { |
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| 245 | if (verboseLevel>0) G4cout |
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| 246 | << " -- Warning -- G4LowEnergyPolarizedCompton::PostStepDoIt " |
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| 247 | << "sin(theta)**2 = " |
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| 248 | << sinThetaSqr |
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| 249 | << "; set to 0" |
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| 250 | << G4endl; |
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| 251 | sinThetaSqr = 0.; |
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| 252 | } |
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| 253 | // End protection |
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| 254 | |
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| 255 | G4double x = std::sqrt(onecost/2.) / (wlGamma/cm);; |
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| 256 | G4double scatteringFunction = scatterFunctionData->FindValue(x,Z-1); |
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| 257 | greject = (1. - epsilon*sinThetaSqr/(1.+ epsilonSq))*scatteringFunction; |
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| 258 | |
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| 259 | } while(greject < G4UniformRand()*Z); |
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| 260 | |
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| 261 | |
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| 262 | // **************************************************** |
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| 263 | // Phi determination |
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| 264 | // **************************************************** |
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| 265 | |
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| 266 | G4double phi = SetPhi(epsilon,sinThetaSqr); |
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| 267 | |
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| 268 | // |
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| 269 | // scattered gamma angles. ( Z - axis along the parent gamma) |
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| 270 | // |
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| 271 | |
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| 272 | G4double cosTheta = 1. - onecost; |
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| 273 | |
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| 274 | // Protection |
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| 275 | |
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| 276 | if (cosTheta > 1.) |
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| 277 | { |
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| 278 | if (verboseLevel>0) G4cout |
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| 279 | << " -- Warning -- G4LowEnergyPolarizedCompton::PostStepDoIt " |
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| 280 | << "cosTheta = " |
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| 281 | << cosTheta |
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| 282 | << "; set to 1" |
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| 283 | << G4endl; |
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| 284 | cosTheta = 1.; |
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| 285 | } |
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| 286 | if (cosTheta < -1.) |
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| 287 | { |
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| 288 | if (verboseLevel>0) G4cout |
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| 289 | << " -- Warning -- G4LowEnergyPolarizedCompton::PostStepDoIt " |
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| 290 | << "cosTheta = " |
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| 291 | << cosTheta |
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| 292 | << "; set to -1" |
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| 293 | << G4endl; |
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| 294 | cosTheta = -1.; |
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| 295 | } |
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| 296 | // End protection |
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| 297 | |
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| 298 | |
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| 299 | G4double sinTheta = std::sqrt (sinThetaSqr); |
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| 300 | |
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| 301 | // Protection |
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| 302 | if (sinTheta > 1.) |
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| 303 | { |
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| 304 | if (verboseLevel>0) G4cout |
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| 305 | << " -- Warning -- G4LowEnergyPolarizedCompton::PostStepDoIt " |
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| 306 | << "sinTheta = " |
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| 307 | << sinTheta |
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| 308 | << "; set to 1" |
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| 309 | << G4endl; |
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| 310 | sinTheta = 1.; |
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| 311 | } |
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| 312 | if (sinTheta < -1.) |
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| 313 | { |
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| 314 | if (verboseLevel>0) G4cout |
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| 315 | << " -- Warning -- G4LowEnergyPolarizedCompton::PostStepDoIt " |
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| 316 | << "sinTheta = " |
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| 317 | << sinTheta |
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| 318 | << "; set to -1" |
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| 319 | << G4endl; |
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| 320 | sinTheta = -1.; |
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| 321 | } |
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| 322 | // End protection |
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| 323 | |
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| 324 | |
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| 325 | G4double dirx = sinTheta*std::cos(phi); |
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| 326 | G4double diry = sinTheta*std::sin(phi); |
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| 327 | G4double dirz = cosTheta ; |
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| 328 | |
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| 329 | // |
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| 330 | // update G4VParticleChange for the scattered photon |
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| 331 | // |
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| 332 | |
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| 333 | gammaEnergy1 = epsilon*gammaEnergy0; |
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| 334 | |
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| 335 | // New polarization |
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| 336 | |
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| 337 | G4ThreeVector gammaPolarization1 = SetNewPolarization(epsilon, |
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| 338 | sinThetaSqr, |
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| 339 | phi, |
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| 340 | cosTheta); |
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| 341 | |
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| 342 | // Set new direction |
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| 343 | G4ThreeVector tmpDirection1( dirx,diry,dirz ); |
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| 344 | gammaDirection1 = tmpDirection1; |
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| 345 | |
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| 346 | // Change reference frame. |
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| 347 | |
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| 348 | SystemOfRefChange(gammaDirection0,gammaDirection1, |
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| 349 | gammaPolarization0,gammaPolarization1); |
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| 350 | |
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| 351 | if (gammaEnergy1 > 0.) |
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| 352 | { |
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| 353 | aParticleChange.ProposeEnergy( gammaEnergy1 ) ; |
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| 354 | aParticleChange.ProposeMomentumDirection( gammaDirection1 ); |
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| 355 | aParticleChange.ProposePolarization( gammaPolarization1 ); |
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| 356 | } |
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| 357 | else |
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| 358 | { |
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| 359 | aParticleChange.ProposeEnergy(0.) ; |
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| 360 | aParticleChange.ProposeTrackStatus(fStopAndKill); |
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| 361 | } |
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| 362 | |
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| 363 | // |
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| 364 | // kinematic of the scattered electron |
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| 365 | // |
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| 366 | |
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| 367 | G4double ElecKineEnergy = gammaEnergy0 - gammaEnergy1 ; |
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| 368 | |
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| 369 | // Generate the electron only if with large enough range w.r.t. cuts and safety |
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| 370 | |
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| 371 | G4double safety = aStep.GetPostStepPoint()->GetSafety(); |
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| 372 | |
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| 373 | if (rangeTest->Escape(G4Electron::Electron(),couple,ElecKineEnergy,safety)) |
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| 374 | { |
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| 375 | G4double ElecMomentum = std::sqrt(ElecKineEnergy*(ElecKineEnergy+2.*electron_mass_c2)); |
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| 376 | G4ThreeVector ElecDirection((gammaEnergy0 * gammaDirection0 - |
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| 377 | gammaEnergy1 * gammaDirection1) * (1./ElecMomentum)); |
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| 378 | G4DynamicParticle* electron = new G4DynamicParticle (G4Electron::Electron(),ElecDirection.unit(),ElecKineEnergy) ; |
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| 379 | aParticleChange.SetNumberOfSecondaries(1); |
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| 380 | aParticleChange.AddSecondary(electron); |
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| 381 | aParticleChange.ProposeLocalEnergyDeposit(0.); |
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| 382 | } |
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| 383 | else |
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| 384 | { |
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| 385 | aParticleChange.SetNumberOfSecondaries(0); |
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| 386 | aParticleChange.ProposeLocalEnergyDeposit(ElecKineEnergy); |
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| 387 | } |
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| 388 | |
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| 389 | return G4VDiscreteProcess::PostStepDoIt( aTrack, aStep); |
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| 390 | |
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| 391 | } |
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| 392 | |
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| 393 | |
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| 394 | G4double G4LowEnergyPolarizedCompton::SetPhi(G4double energyRate, |
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| 395 | G4double sinSqrTh) |
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| 396 | { |
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| 397 | G4double rand1; |
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| 398 | G4double rand2; |
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| 399 | G4double phiProbability; |
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| 400 | G4double phi; |
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| 401 | G4double a, b; |
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| 402 | |
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| 403 | do |
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| 404 | { |
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| 405 | rand1 = G4UniformRand(); |
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| 406 | rand2 = G4UniformRand(); |
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| 407 | phiProbability=0.; |
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| 408 | phi = twopi*rand1; |
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| 409 | |
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| 410 | a = 2*sinSqrTh; |
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| 411 | b = energyRate + 1/energyRate; |
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| 412 | |
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| 413 | phiProbability = 1 - (a/b)*(std::cos(phi)*std::cos(phi)); |
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| 414 | |
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| 415 | |
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| 416 | |
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| 417 | } |
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| 418 | while ( rand2 > phiProbability ); |
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| 419 | return phi; |
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| 420 | } |
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| 421 | |
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| 422 | |
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| 423 | G4ThreeVector G4LowEnergyPolarizedCompton::SetPerpendicularVector(G4ThreeVector& a) |
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| 424 | { |
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| 425 | G4double dx = a.x(); |
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| 426 | G4double dy = a.y(); |
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| 427 | G4double dz = a.z(); |
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| 428 | G4double x = dx < 0.0 ? -dx : dx; |
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| 429 | G4double y = dy < 0.0 ? -dy : dy; |
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| 430 | G4double z = dz < 0.0 ? -dz : dz; |
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| 431 | if (x < y) { |
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| 432 | return x < z ? G4ThreeVector(-dy,dx,0) : G4ThreeVector(0,-dz,dy); |
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| 433 | }else{ |
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| 434 | return y < z ? G4ThreeVector(dz,0,-dx) : G4ThreeVector(-dy,dx,0); |
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| 435 | } |
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| 436 | } |
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| 437 | |
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| 438 | G4ThreeVector G4LowEnergyPolarizedCompton::GetRandomPolarization(G4ThreeVector& direction0) |
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| 439 | { |
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| 440 | G4ThreeVector d0 = direction0.unit(); |
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| 441 | G4ThreeVector a1 = SetPerpendicularVector(d0); //different orthogonal |
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| 442 | G4ThreeVector a0 = a1.unit(); // unit vector |
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| 443 | |
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| 444 | G4double rand1 = G4UniformRand(); |
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| 445 | |
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| 446 | G4double angle = twopi*rand1; // random polar angle |
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| 447 | G4ThreeVector b0 = d0.cross(a0); // cross product |
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| 448 | |
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| 449 | G4ThreeVector c; |
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| 450 | |
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| 451 | c.setX(std::cos(angle)*(a0.x())+std::sin(angle)*b0.x()); |
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| 452 | c.setY(std::cos(angle)*(a0.y())+std::sin(angle)*b0.y()); |
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| 453 | c.setZ(std::cos(angle)*(a0.z())+std::sin(angle)*b0.z()); |
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| 454 | |
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| 455 | G4ThreeVector c0 = c.unit(); |
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| 456 | |
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| 457 | return c0; |
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| 458 | |
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| 459 | } |
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| 460 | |
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| 461 | |
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| 462 | G4ThreeVector G4LowEnergyPolarizedCompton::GetPerpendicularPolarization |
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| 463 | (const G4ThreeVector& gammaDirection, const G4ThreeVector& gammaPolarization) const |
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| 464 | { |
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| 465 | |
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| 466 | // |
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| 467 | // The polarization of a photon is always perpendicular to its momentum direction. |
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| 468 | // Therefore this function removes those vector component of gammaPolarization, which |
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| 469 | // points in direction of gammaDirection |
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| 470 | // |
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| 471 | // Mathematically we search the projection of the vector a on the plane E, where n is the |
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| 472 | // plains normal vector. |
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| 473 | // The basic equation can be found in each geometry book (e.g. Bronstein): |
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| 474 | // p = a - (a o n)/(n o n)*n |
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| 475 | |
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| 476 | return gammaPolarization - gammaPolarization.dot(gammaDirection)/gammaDirection.dot(gammaDirection) * gammaDirection; |
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| 477 | } |
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| 478 | |
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| 479 | |
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| 480 | G4ThreeVector G4LowEnergyPolarizedCompton::SetNewPolarization(G4double epsilon, |
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| 481 | G4double sinSqrTh, |
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| 482 | G4double phi, |
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| 483 | G4double costheta) |
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| 484 | { |
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| 485 | G4double rand1; |
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| 486 | G4double rand2; |
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| 487 | G4double cosPhi = std::cos(phi); |
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| 488 | G4double sinPhi = std::sin(phi); |
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| 489 | G4double sinTheta = std::sqrt(sinSqrTh); |
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| 490 | G4double cosSqrPhi = cosPhi*cosPhi; |
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| 491 | // G4double cossqrth = 1.-sinSqrTh; |
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| 492 | // G4double sinsqrphi = sinPhi*sinPhi; |
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| 493 | G4double normalisation = std::sqrt(1. - cosSqrPhi*sinSqrTh); |
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| 494 | |
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| 495 | |
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| 496 | // Determination of Theta |
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| 497 | |
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| 498 | G4double thetaProbability; |
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| 499 | G4double theta; |
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| 500 | G4double a, b; |
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| 501 | G4double cosTheta; |
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| 502 | |
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| 503 | do |
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| 504 | { |
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| 505 | rand1 = G4UniformRand(); |
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| 506 | rand2 = G4UniformRand(); |
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| 507 | thetaProbability=0.; |
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| 508 | theta = twopi*rand1; |
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| 509 | a = 4*normalisation*normalisation; |
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| 510 | b = (epsilon + 1/epsilon) - 2; |
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| 511 | thetaProbability = (b + a*std::cos(theta)*std::cos(theta))/(a+b); |
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| 512 | cosTheta = std::cos(theta); |
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| 513 | } |
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| 514 | while ( rand2 > thetaProbability ); |
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| 515 | |
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| 516 | G4double cosBeta = cosTheta; |
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| 517 | G4double sinBeta = std::sqrt(1-cosBeta*cosBeta); |
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| 518 | |
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| 519 | G4ThreeVector gammaPolarization1; |
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| 520 | |
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| 521 | G4double xParallel = normalisation*cosBeta; |
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| 522 | G4double yParallel = -(sinSqrTh*cosPhi*sinPhi)*cosBeta/normalisation; |
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| 523 | G4double zParallel = -(costheta*sinTheta*cosPhi)*cosBeta/normalisation; |
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| 524 | G4double xPerpendicular = 0.; |
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| 525 | G4double yPerpendicular = (costheta)*sinBeta/normalisation; |
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| 526 | G4double zPerpendicular = -(sinTheta*sinPhi)*sinBeta/normalisation; |
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| 527 | |
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| 528 | G4double xTotal = (xParallel + xPerpendicular); |
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| 529 | G4double yTotal = (yParallel + yPerpendicular); |
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| 530 | G4double zTotal = (zParallel + zPerpendicular); |
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| 531 | |
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| 532 | gammaPolarization1.setX(xTotal); |
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| 533 | gammaPolarization1.setY(yTotal); |
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| 534 | gammaPolarization1.setZ(zTotal); |
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| 535 | |
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| 536 | return gammaPolarization1; |
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| 537 | |
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| 538 | } |
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| 539 | |
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| 540 | |
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| 541 | void G4LowEnergyPolarizedCompton::SystemOfRefChange(G4ThreeVector& direction0, |
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| 542 | G4ThreeVector& direction1, |
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| 543 | G4ThreeVector& polarization0, |
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| 544 | G4ThreeVector& polarization1) |
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| 545 | { |
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| 546 | // direction0 is the original photon direction ---> z |
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| 547 | // polarization0 is the original photon polarization ---> x |
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| 548 | // need to specify y axis in the real reference frame ---> y |
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| 549 | G4ThreeVector Axis_Z0 = direction0.unit(); |
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| 550 | G4ThreeVector Axis_X0 = polarization0.unit(); |
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| 551 | G4ThreeVector Axis_Y0 = (Axis_Z0.cross(Axis_X0)).unit(); // to be confirmed; |
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| 552 | |
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| 553 | G4double direction_x = direction1.getX(); |
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| 554 | G4double direction_y = direction1.getY(); |
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| 555 | G4double direction_z = direction1.getZ(); |
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| 556 | |
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| 557 | direction1 = (direction_x*Axis_X0 + direction_y*Axis_Y0 + direction_z*Axis_Z0).unit(); |
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| 558 | G4double polarization_x = polarization1.getX(); |
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| 559 | G4double polarization_y = polarization1.getY(); |
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| 560 | G4double polarization_z = polarization1.getZ(); |
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| 561 | |
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| 562 | polarization1 = (polarization_x*Axis_X0 + polarization_y*Axis_Y0 + polarization_z*Axis_Z0).unit(); |
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| 563 | |
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| 564 | } |
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| 565 | |
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| 566 | |
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| 567 | G4bool G4LowEnergyPolarizedCompton::IsApplicable(const G4ParticleDefinition& particle) |
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| 568 | { |
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| 569 | return ( &particle == G4Gamma::Gamma() ); |
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| 570 | } |
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| 571 | |
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| 572 | |
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| 573 | G4double G4LowEnergyPolarizedCompton::GetMeanFreePath(const G4Track& track, |
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| 574 | G4double, |
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| 575 | G4ForceCondition*) |
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| 576 | { |
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| 577 | const G4DynamicParticle* photon = track.GetDynamicParticle(); |
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| 578 | G4double energy = photon->GetKineticEnergy(); |
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| 579 | const G4MaterialCutsCouple* couple = track.GetMaterialCutsCouple(); |
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| 580 | size_t materialIndex = couple->GetIndex(); |
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| 581 | G4double meanFreePath; |
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| 582 | if (energy > highEnergyLimit) meanFreePath = meanFreePathTable->FindValue(highEnergyLimit,materialIndex); |
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| 583 | else if (energy < lowEnergyLimit) meanFreePath = DBL_MAX; |
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| 584 | else meanFreePath = meanFreePathTable->FindValue(energy,materialIndex); |
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| 585 | return meanFreePath; |
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| 586 | } |
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