source: trunk/source/processes/electromagnetic/polarisation/src/G4VPolarizedCrossSection.cc@ 1196

Last change on this file since 1196 was 1196, checked in by garnier, 16 years ago

update CVS release candidate geant4.9.3.01

File size: 5.1 KB
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[819]1//
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25//
26// $Id: G4VPolarizedCrossSection.cc,v 1.4 2007/11/01 17:32:34 schaelic Exp $
[1196]27// GEANT4 tag $Name: geant4-09-03-cand-01 $
[819]28// File name: G4VPolarizedCrossSection
29//
30// Author: Andreas Schaelicke
31//
32// Creation date: 15.05.2005
33//
34// Modifications:
35//
36// Class Description:
37// (pure virtual) interface class
38//
39// provides readable but efficient routines to determine
40// polarization for the final state of a given process
41// empoying the differential cross section
42//
43
44#include "G4VPolarizedCrossSection.hh"
45#include "Randomize.hh"
46
47G4VPolarizedCrossSection::G4VPolarizedCrossSection() :
48 fXmin(0), fXmax(1.), fYmin(1.), theA(1), theZ(1), fCoul(0.)
49{
50}
51
52G4VPolarizedCrossSection::~G4VPolarizedCrossSection()
53{
54}
55
56void G4VPolarizedCrossSection::Initialize(G4double, G4double, G4double,
57 const G4StokesVector &,
58 const G4StokesVector &,
59 G4int )
60{
61}
62
63G4StokesVector G4VPolarizedCrossSection::GetPol2()
64{
65 // neglects correlation effects!
66
67 G4double invXsecTotal=1./XSection(G4StokesVector::ZERO,G4StokesVector::ZERO);
68 G4double xsPol1=XSection(G4StokesVector::P1,G4StokesVector::ZERO);
69 G4double xsPol2=XSection(G4StokesVector::P2,G4StokesVector::ZERO);
70 G4double xsPol3=XSection(G4StokesVector::P3,G4StokesVector::ZERO);
71 return G4ThreeVector(invXsecTotal*xsPol1,invXsecTotal*xsPol2,invXsecTotal*xsPol3);
72}
73
74G4StokesVector G4VPolarizedCrossSection::GetPol3()
75{
76 // neglects correlation effects!
77
78 G4double invXsecTotal=1./XSection(G4StokesVector::ZERO,G4StokesVector::ZERO);
79 G4double xsPol1=XSection(G4StokesVector::ZERO,G4StokesVector::P1);
80 G4double xsPol2=XSection(G4StokesVector::ZERO,G4StokesVector::P2);
81 G4double xsPol3=XSection(G4StokesVector::ZERO,G4StokesVector::P3);
82 return G4ThreeVector(invXsecTotal*xsPol1,invXsecTotal*xsPol2,invXsecTotal*xsPol3);
83}
84// minimal energy fraction in TotalXSection
85G4double G4VPolarizedCrossSection::GetXmin(G4double /*y*/)
86{
87 return fXmin;
88}
89
90// maximal energy fraction in TotalXSection
91G4double G4VPolarizedCrossSection::GetXmax(G4double /*y*/)
92{
93 return fXmax;
94}
95
96
97/*
98void G4VPolarizedCrossSection::DicePolarization()
99{
100 // can respect correlation effects, but is limited to
101 // one quantization axis!
102 G4double sigma[4];
103 sigma[0]=XSection(G4StokesVector::P3,G4StokesVector::P3);
104 sigma[1]=XSection(G4StokesVector::P3,G4StokesVector::M3);
105 sigma[2]=XSection(G4StokesVector::M3,G4StokesVector::P3);
106 sigma[3]=XSection(G4StokesVector::M3,G4StokesVector::M3);
107
108 G4double sigma_max = 4. * XSection(G4StokesVector::ZERO,G4StokesVector::ZERO);
109
110 for (G4int i=0;i<4;++i) {
111 G4cout<<"sigma="<<sigma[i]<<" vs."<<(.25*sigma_max)<<G4endl;
112 if (sigma[i]<0 || sigma[i]>sigma_max) {
113 G4cout<<"ERROR G4VPolarizedCrossSection::DicePolarization(["<<i<<"]): "
114 <<sigma[i]<<" vs."<<sigma_max<<G4endl;
115 }
116 if (i>0) sigma[i]+=sigma[i-1];
117 }
118
119 G4int k = 0;
120 G4double disc = sigma[3]*G4UniformRand();
121 while (sigma[k]<disc && k<4) {
122 ++k;
123 }
124
125 if ((k&2)==0) pol2=G4StokesVector::P3;
126 else pol2=G4StokesVector::M3;
127 if ((k&1)==0) pol3=G4StokesVector::P3;
128 else pol3=G4StokesVector::M3;
129
130}
131*/
132
133/*
134G4StokesVector G4VPolarizedCrossSection::DicedPol2()
135{
136 return pol2;
137}
138
139G4StokesVector G4VPolarizedCrossSection::DicedPol3()
140{
141 return pol3;
142}
143*/
144
145G4double G4VPolarizedCrossSection::TotalXSection(const G4double, const G4double, const G4double,
146 const G4StokesVector &,const G4StokesVector &)
147{
148 G4cout << "WARNING virtual function G4VPolarizedCrossSection::TotalXSection() called" << G4endl;
149 return 0.;
150}
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