| 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: G4PolarizedComptonCrossSection.cc,v 1.4 2007/11/01 17:32:34 schaelic Exp $
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| 27 | // GEANT4 tag $Name: $
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| 28 | //
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| 29 | // GEANT4 Class file
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| 30 | //
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| 31 | //
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| 32 | // File name: G4PolarizedComptonCrossSection
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| 33 | //
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| 34 | // Author: Andreas Schaelicke
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| 35 | //
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| 36 | // Creation date: 15.05.2005
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| 37 | //
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| 38 | // Modifications:
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| 39 | //
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| 40 | // Class Description:
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| 41 | // determine the polarization of the final state
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| 42 | // in a Compton scattering process employing the differential
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| 43 | // cross section by F.W.Lipps & H.A.Tolhoek
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| 44 | // ( Physica 20 (1954) 395 )
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| 45 | // recalculated by P.Starovoitov
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| 46 | //
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| 47 | #include "G4PolarizedComptonCrossSection.hh"
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| 48 | #include "Randomize.hh"
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| 49 |
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| 50 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 51 | G4PolarizedComptonCrossSection::G4PolarizedComptonCrossSection()
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| 52 | {
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| 53 | SetYmin(0.);
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| 54 |
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| 55 | // G4cout<<"G4PolarizedComptonCrossSection() init\n";
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| 56 |
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| 57 | re2 = classic_electr_radius * classic_electr_radius * sqr(4*pi/hbarc);
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| 58 | // G4double unit_conversion = hbarc_squared ;
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| 59 | // G4cout<<" (keV)^2* m^2 ="<<unit_conversion<<"\n";
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| 60 | phi0 = 0.; polXS = 0.; unpXS = 0.;
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| 61 | phi2 = G4ThreeVector(0., 0., 0.);
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| 62 | phi3 = G4ThreeVector(0., 0., 0.);
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| 63 | polxx = polyy = polzz = polxz = polzx = polyz = polzy = polxy = polyx = 0.;
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| 64 | diffXSFactor = 1.;
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| 65 | totalXSFactor = 1.;
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| 66 | }
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| 67 |
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| 68 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 69 | G4PolarizedComptonCrossSection::~G4PolarizedComptonCrossSection()
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| 70 | {}
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| 71 |
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| 72 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 73 | void G4PolarizedComptonCrossSection::Initialize(G4double eps, G4double X, G4double , // phi
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| 74 | const G4StokesVector & pol0,
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| 75 | const G4StokesVector & pol1,
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| 76 | G4int flag)
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| 77 | {
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| 78 | G4double cosT = 1. - (1./eps - 1.)/X;
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| 79 | if(cosT > 1.+1.e-8) cosT = 1.;
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| 80 | if(cosT < -1.-1.e-8) cosT = -1.;
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| 81 | G4double cosT2 = cosT*cosT;
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| 82 | G4double cosT3 = cosT2*cosT;
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| 83 | G4double sinT2 = 1. - cosT2;
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| 84 | if(sinT2 > 1. + 1.e-8) sinT2 = 1.;
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| 85 | if(sinT2 < 0.) sinT2 = 0.;
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| 86 | G4double sinT = std::sqrt(sinT2);
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| 87 | G4double cos2T = 2.*cosT2 - 1.;
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| 88 | G4double sin2T = 2.*sinT*cosT;
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| 89 | G4double eps2 = sqr(eps);
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| 90 | DefineCoefficients(pol0,pol1);
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| 91 | diffXSFactor = re2/(4.*X);
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| 92 |
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| 93 | // unpolarized Cross Section
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| 94 | unpXS = (eps2 + 1. - eps*sinT2)/(2.*eps);
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| 95 | // initial polarization dependence
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| 96 | polXS = -sinT2*pol0.x() + (1. - eps)*sinT*polzx + ((eps2 - 1.)/eps)*cosT*polzz;
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| 97 | polXS *= 0.5;
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| 98 |
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| 99 | phi0 = unpXS + polXS;
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| 100 |
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| 101 | if (flag == 2 ){
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| 102 | // polarization of outgoing photon
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| 103 | G4double PHI21 = -sinT2 + 0.5*(cos2T + 3.)*pol0.x() - ((1. - eps)/eps)*sinT*polzx;
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| 104 | PHI21 *= 0.5;
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| 105 | G4double PHI22 = cosT*pol0.y() + ((1. - eps)/(2.*eps))*sinT*polzy;
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| 106 | G4double PHI23 = ((eps2 + 1.)/eps)*cosT*pol0.z() - ((1. - eps)/eps)*(eps*cosT2 + 1.)*pol1.z();
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| 107 | PHI23 += 0.5*(1. - eps)*sin2T*pol1.x();
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| 108 | PHI23 += (eps - 1.)*(-sinT2*polxz + sinT*polyy - 0.5*sin2T*polxx);
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| 109 | PHI23 *= 0.5;
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| 110 | phi2 = G4ThreeVector(PHI21, PHI22, PHI23);
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| 111 |
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| 112 | // polarization of outgoing electron
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| 113 | G4double PHI32 = -sinT2*polxy + ((1. - eps)/eps)*sinT*polyz + 0.5*(cos2T + 3.)*pol1.y();
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| 114 | PHI32 *= 0.5;
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| 115 |
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| 116 | G4double PHI31 = 0., PHI31add = 0., PHI33 = 0., PHI33add = 0.;
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| 117 |
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| 118 | if ((1. - eps) > 1.e-12){
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| 119 | G4double helpVar = std::sqrt(eps2 - 2.*cosT*eps + 1.);
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| 120 |
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| 121 | PHI31 = (1. - eps)*(1. + cosT)*sinT*pol0.z();
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| 122 | PHI31 += (-eps*cosT3 + eps*cosT2 + (eps - 2.)*cosT + eps)*pol1.x();
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| 123 | PHI31 += -(eps*cosT2 - eps*cosT + cosT + 1.)*sinT*pol1.z();
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| 124 | PHI31 /= 2.*helpVar;
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| 125 |
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| 126 | PHI31add = -eps*sqr(1. - cosT)*(1. + cosT)*polxx;
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| 127 | PHI31add += (1. - eps)*sinT2*polyy;
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| 128 | PHI31add += -(-eps2 + cosT*(cosT*eps - eps + 1.)*eps + eps - 1.)*sinT*polxz/eps;
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| 129 | PHI31add /= 2.*helpVar;
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| 130 |
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| 131 | PHI33 = ((1. - eps)/eps)*(-eps*cosT2 + eps*(eps + 1.)*cosT - 1.)*pol0.z();
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| 132 | PHI33 += -(eps*cosT2 + (1. - eps)*eps*cosT + 1.)*sinT*pol1.x();
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| 133 | PHI33 += -(-eps2*cosT3 + eps*(eps2 - eps + 1.)*cosT2 - cosT + eps2)*pol1.z()/eps;
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| 134 | PHI33 /= -2.*helpVar;
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| 135 |
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| 136 | PHI33add = (eps*(eps - cosT - 1.)*cosT + 1.)*sinT*polxx;
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| 137 | PHI33add += -(-eps2 + cosT*eps + eps - 1.)*sinT2*polxz;
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| 138 | PHI33add += (eps - 1.)*(cosT - eps)*sinT*polyy;
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| 139 | PHI33add /= -2.*helpVar;
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| 140 | }else{
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| 141 | PHI31 = -pol1.z() - (X - 1.)*std::sqrt(1. - eps)*pol1.x()/std::sqrt(2.*X);
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| 142 | PHI31add = -(-X*X*pol1.z() - 2.*X*(2.*pol0.z() - pol1.z()) - (4.*pol0.x() + 5.)*pol1.z())*(1. - eps)/(4.*X);
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| 143 |
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| 144 | PHI33 = pol1.x() - (X - 1.)*std::sqrt(1. - eps)*pol1.z()/std::sqrt(2.*X);
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| 145 | PHI33add = -(X*X - 2.*X + 4.*pol0.x() + 5.)*(1. - eps)*pol1.x()/(4.*X);
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| 146 | }
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| 147 | phi3 = G4ThreeVector(PHI31 + PHI31add, PHI32, PHI33 + PHI33add);
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| 148 |
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| 149 | }
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| 150 | unpXS *= diffXSFactor;
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| 151 | polXS *= diffXSFactor;
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| 152 | phi0 *= diffXSFactor;
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| 153 | phi2 *= diffXSFactor;
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| 154 | phi3 *= diffXSFactor;
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| 155 |
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| 156 | }
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| 157 |
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| 158 | G4double G4PolarizedComptonCrossSection::XSection(const G4StokesVector & pol2,const G4StokesVector & pol3)
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| 159 | {
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| 160 | gammaPol2 = !(pol2==G4StokesVector::ZERO);
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| 161 | electronPol3 = !(pol3==G4StokesVector::ZERO);
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| 162 |
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| 163 | G4double phi = 0.;
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| 164 | // polarization independent part
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| 165 | phi += phi0;
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| 166 |
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| 167 |
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| 168 | if (gammaPol2) {
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| 169 | // part depending on the polarization of the final photon
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| 170 | phi += phi2*pol2;
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| 171 | }
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| 172 |
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| 173 | if (electronPol3) {
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| 174 | // part depending on the polarization of the final electron
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| 175 | phi += phi3*pol3;
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| 176 | }
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| 177 |
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| 178 | // return cross section.
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| 179 | return phi;
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| 180 | }
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| 181 |
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| 182 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 183 |
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| 184 |
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| 185 | G4double G4PolarizedComptonCrossSection::TotalXSection(G4double /*xmin*/, G4double /*xmax*/, G4double k0,
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| 186 | const G4StokesVector & pol0,
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| 187 | const G4StokesVector & pol1)
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| 188 | {
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| 189 |
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| 190 | // G4double k0 = gammaEnergy / electron_mass_c2 ;
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| 191 | G4double k1 = 1 + 2*k0 ;
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| 192 |
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| 193 | // // pi*re^2
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| 194 | // G4double re=2.81794e-15; //m
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| 195 | // G4double barn=1.e-28; //m^2
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| 196 | G4double Z=theZ;
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| 197 |
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| 198 | G4double unit = Z*pi*classic_electr_radius
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| 199 | * classic_electr_radius ; // *1./barn;
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| 200 |
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| 201 | G4double pre = unit/(sqr(k0)*sqr(1.+2.*k0));
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| 202 |
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| 203 | G4double xs_0 = ((k0 - 2.)*k0 -2.)*sqr(k1)*std::log(k1) + 2.*k0*(k0*(k0 + 1.)*(k0 + 8.) + 2.);
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| 204 | G4double xs_pol = (k0 + 1.)*sqr(k1)*std::log(k1) - 2.*k0*(5.*sqr(k0) + 4.*k0 + 1.);
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| 205 |
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| 206 | return pre*(xs_0/k0 + pol0.p3()*pol1.z()*xs_pol);
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| 207 | }
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| 208 |
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| 209 |
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| 210 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 211 |
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| 212 |
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| 213 | G4StokesVector G4PolarizedComptonCrossSection::GetPol2()
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| 214 | {
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| 215 | // Note, mean polarization can not contain correlation
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| 216 | // effects.
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| 217 | return 1./phi0 * phi2;
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| 218 | }
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| 219 |
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| 220 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 221 |
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| 222 | G4StokesVector G4PolarizedComptonCrossSection::GetPol3()
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| 223 | {
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| 224 | // Note, mean polarization can not contain correlation
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| 225 | // effects.
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| 226 | return 1./phi0 * phi3;
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| 227 | }
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| 228 |
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| 229 |
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| 230 |
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| 231 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 232 | void G4PolarizedComptonCrossSection::DefineCoefficients(const G4StokesVector & pol0,
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| 233 | const G4StokesVector & pol1)
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| 234 | {
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| 235 | polxx=pol0.x()*pol1.x();
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| 236 | polyy=pol0.y()*pol1.y();
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| 237 | polzz=pol0.z()*pol1.z();
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| 238 |
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| 239 | polxz=pol0.x()*pol1.z();
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| 240 | polzx=pol0.z()*pol1.x();
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| 241 |
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| 242 | polyz=pol0.y()*pol1.z();
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| 243 | polzy=pol0.z()*pol1.y();
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| 244 |
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| 245 | polxy=pol0.x()*pol1.y();
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| 246 | polyx=pol0.y()*pol1.x();
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| 247 | }
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| 248 |
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| 249 |
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| 250 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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