| [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 | // $Id: G4VPolarizedCrossSection.cc,v 1.4 2007/11/01 17:32:34 schaelic Exp $
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| [1337] | 27 | // GEANT4 tag $Name: geant4-09-04-beta-01 $
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| [819] | 28 | // File name: G4VPolarizedCrossSection
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| 29 | //
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| 30 | // Author: Andreas Schaelicke
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| 31 | //
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| 32 | // Creation date: 15.05.2005
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| 33 | //
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| 34 | // Modifications:
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| 35 | //
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| 36 | // Class Description:
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| 37 | // (pure virtual) interface class
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| 38 | //
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| 39 | // provides readable but efficient routines to determine
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| 40 | // polarization for the final state of a given process
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| 41 | // empoying the differential cross section
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| 42 | //
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| 43 |
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| 44 | #include "G4VPolarizedCrossSection.hh"
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| 45 | #include "Randomize.hh"
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| 46 |
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| 47 | G4VPolarizedCrossSection::G4VPolarizedCrossSection() :
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| 48 | fXmin(0), fXmax(1.), fYmin(1.), theA(1), theZ(1), fCoul(0.)
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| 49 | {
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| 50 | }
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| 51 |
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| 52 | G4VPolarizedCrossSection::~G4VPolarizedCrossSection()
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| 53 | {
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| 54 | }
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| 55 |
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| 56 | void G4VPolarizedCrossSection::Initialize(G4double, G4double, G4double,
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| 57 | const G4StokesVector &,
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| 58 | const G4StokesVector &,
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| 59 | G4int )
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| 60 | {
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| 61 | }
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| 62 |
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| 63 | G4StokesVector G4VPolarizedCrossSection::GetPol2()
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| 64 | {
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| 65 | // neglects correlation effects!
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| 66 |
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| 67 | G4double invXsecTotal=1./XSection(G4StokesVector::ZERO,G4StokesVector::ZERO);
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| 68 | G4double xsPol1=XSection(G4StokesVector::P1,G4StokesVector::ZERO);
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| 69 | G4double xsPol2=XSection(G4StokesVector::P2,G4StokesVector::ZERO);
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| 70 | G4double xsPol3=XSection(G4StokesVector::P3,G4StokesVector::ZERO);
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| 71 | return G4ThreeVector(invXsecTotal*xsPol1,invXsecTotal*xsPol2,invXsecTotal*xsPol3);
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| 72 | }
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| 73 |
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| 74 | G4StokesVector G4VPolarizedCrossSection::GetPol3()
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| 75 | {
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| 76 | // neglects correlation effects!
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| 77 |
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| 78 | G4double invXsecTotal=1./XSection(G4StokesVector::ZERO,G4StokesVector::ZERO);
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| 79 | G4double xsPol1=XSection(G4StokesVector::ZERO,G4StokesVector::P1);
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| 80 | G4double xsPol2=XSection(G4StokesVector::ZERO,G4StokesVector::P2);
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| 81 | G4double xsPol3=XSection(G4StokesVector::ZERO,G4StokesVector::P3);
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| 82 | return G4ThreeVector(invXsecTotal*xsPol1,invXsecTotal*xsPol2,invXsecTotal*xsPol3);
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| 83 | }
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| 84 | // minimal energy fraction in TotalXSection
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| 85 | G4double G4VPolarizedCrossSection::GetXmin(G4double /*y*/)
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| 86 | {
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| 87 | return fXmin;
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| 88 | }
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| 89 |
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| 90 | // maximal energy fraction in TotalXSection
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| 91 | G4double G4VPolarizedCrossSection::GetXmax(G4double /*y*/)
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| 92 | {
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| 93 | return fXmax;
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| 94 | }
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| 95 |
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| 96 |
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| 97 | /*
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| 98 | void G4VPolarizedCrossSection::DicePolarization()
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| 99 | {
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| 100 | // can respect correlation effects, but is limited to
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| 101 | // one quantization axis!
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| 102 | G4double sigma[4];
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| 103 | sigma[0]=XSection(G4StokesVector::P3,G4StokesVector::P3);
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| 104 | sigma[1]=XSection(G4StokesVector::P3,G4StokesVector::M3);
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| 105 | sigma[2]=XSection(G4StokesVector::M3,G4StokesVector::P3);
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| 106 | sigma[3]=XSection(G4StokesVector::M3,G4StokesVector::M3);
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| 107 |
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| 108 | G4double sigma_max = 4. * XSection(G4StokesVector::ZERO,G4StokesVector::ZERO);
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| 109 |
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| 110 | for (G4int i=0;i<4;++i) {
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| 111 | G4cout<<"sigma="<<sigma[i]<<" vs."<<(.25*sigma_max)<<G4endl;
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| 112 | if (sigma[i]<0 || sigma[i]>sigma_max) {
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| 113 | G4cout<<"ERROR G4VPolarizedCrossSection::DicePolarization(["<<i<<"]): "
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| 114 | <<sigma[i]<<" vs."<<sigma_max<<G4endl;
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| 115 | }
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| 116 | if (i>0) sigma[i]+=sigma[i-1];
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| 117 | }
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| 118 |
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| 119 | G4int k = 0;
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| 120 | G4double disc = sigma[3]*G4UniformRand();
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| 121 | while (sigma[k]<disc && k<4) {
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| 122 | ++k;
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| 123 | }
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| 124 |
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| 125 | if ((k&2)==0) pol2=G4StokesVector::P3;
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| 126 | else pol2=G4StokesVector::M3;
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| 127 | if ((k&1)==0) pol3=G4StokesVector::P3;
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| 128 | else pol3=G4StokesVector::M3;
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| 129 |
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| 130 | }
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| 131 | */
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| 132 |
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| 133 | /*
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| 134 | G4StokesVector G4VPolarizedCrossSection::DicedPol2()
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| 135 | {
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| 136 | return pol2;
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| 137 | }
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| 138 |
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| 139 | G4StokesVector G4VPolarizedCrossSection::DicedPol3()
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| 140 | {
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| 141 | return pol3;
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| 142 | }
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| 143 | */
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| 144 |
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| 145 | G4double G4VPolarizedCrossSection::TotalXSection(const G4double, const G4double, const G4double,
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| 146 | const G4StokesVector &,const G4StokesVector &)
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| 147 | {
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| 148 | G4cout << "WARNING virtual function G4VPolarizedCrossSection::TotalXSection() called" << G4endl;
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| 149 | return 0.;
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| 150 | }
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