source: trunk/source/processes/electromagnetic/xrays/src/G4XTRRegularRadModel.cc@ 1016

Last change on this file since 1016 was 819, checked in by garnier, 17 years ago

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[819]1//
2// ********************************************************************
3// * License and Disclaimer *
4// * *
5// * The Geant4 software is copyright of the Copyright Holders of *
6// * the Geant4 Collaboration. It is provided under the terms and *
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14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
16// * for the full disclaimer and the limitation of liability. *
17// * *
18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
20// * By using, copying, modifying or distributing the software (or *
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24// ********************************************************************
25//
26//
27
28#include <complex>
29
30#include "G4XTRRegularRadModel.hh"
31#include "Randomize.hh"
32
33#include "G4Gamma.hh"
34using namespace std;
35
36////////////////////////////////////////////////////////////////////////////
37//
38// Constructor, destructor
39
40G4XTRRegularRadModel::G4XTRRegularRadModel(G4LogicalVolume *anEnvelope,
41 G4Material* foilMat,G4Material* gasMat,
42 G4double a, G4double b, G4int n,
43 const G4String& processName) :
44 G4VXTRenergyLoss(anEnvelope,foilMat,gasMat,a,b,n,processName)
45{
46 G4cout<<" XTR Regular discrete radiator model is called"<<G4endl ;
47
48 fExitFlux = true;
49
50 // Build energy and angular integral spectra of X-ray TR photons from
51 // a radiator
52
53 // BuildTable() ;
54}
55
56///////////////////////////////////////////////////////////////////////////
57
58G4XTRRegularRadModel::~G4XTRRegularRadModel()
59{
60 ;
61}
62
63
64
65///////////////////////////////////////////////////////////////////////////
66//
67// Approximation for radiator interference factor for the case of
68// fully Regular radiator. The plate and gas gap thicknesses are fixed .
69// The mean values of the plate and gas gap thicknesses
70// are supposed to be about XTR formation zones but much less than
71// mean absorption length of XTR photons in coresponding material.
72
73G4double
74G4XTRRegularRadModel::GetStackFactor( G4double energy,
75 G4double gamma, G4double varAngle )
76{
77 G4double result, Qa, Qb, Q, aZa, bZb, aMa, bMb, I2 ;
78
79 aZa = fPlateThick/GetPlateFormationZone(energy,gamma,varAngle) ;
80 bZb = fGasThick/GetGasFormationZone(energy,gamma,varAngle) ;
81
82 aMa = fPlateThick*GetPlateLinearPhotoAbs(energy) ;
83 bMb = fGasThick*GetGasLinearPhotoAbs(energy) ;
84
85 Qa = std::exp(-aMa) ;
86 Qb = std::exp(-bMb) ;
87 Q = Qa*Qb ;
88
89 // G4complex Ca(1.0+0.5*fPlateThick*Ma,fPlateThick/Za) ;
90 // G4complex Cb(1.0+0.5*fGasThick*Mb,fGasThick/Zb) ;
91
92 G4complex Ha( std::exp(-0.5*aMa)*std::cos(aZa),
93 -std::exp(-0.5*aMa)*std::sin(aZa) ) ;
94
95 G4complex Hb( std::exp(-0.5*bMb)*std::cos(bZb),
96 -std::exp(-0.5*bMb)*std::sin(bZb) ) ;
97
98 G4complex H = Ha*Hb ;
99
100 G4complex Hs = std::conj(H) ;
101
102 // G4complex F1 = ( 0.5*(1+Qa)*(1+H) - Ha - Qa*Hb )/(1-H) ;
103
104 G4complex F2 = (1.0-Ha)*(Qa-Ha)*Hb*(1.0-Hs)*(Q-Hs) ;
105
106 F2 *= std::pow(Q,G4double(fPlateNumber)) - std::pow(H,fPlateNumber) ;
107
108 result = ( 1 - std::pow(Q,G4double(fPlateNumber)) )/( 1 - Q ) ;
109
110 result *= (1 - Qa)*(1 + Qa - 2*std::sqrt(Qa)*std::cos(aZa)) ;
111
112 result /= (1 - std::sqrt(Q))*(1 - std::sqrt(Q)) +
113 4*std::sqrt(Q)*std::sin(0.5*(aZa+bZb))*std::sin(0.5*(aZa+bZb)) ;
114
115 I2 = 1.; // 2.0*std::real(F2) ;
116
117 I2 /= (1 - std::sqrt(Q))*(1 - std::sqrt(Q)) +
118 4*std::sqrt(Q)*std::sin(0.5*(aZa+bZb))*std::sin(0.5*(aZa+bZb)) ;
119
120 I2 /= Q*( (std::sqrt(Q)-std::cos(aZa+bZb))*(std::sqrt(Q)-std::cos(aZa+bZb)) +
121 std::sin(aZa+bZb)*std::sin(aZa+bZb) ) ;
122
123 G4complex stack = 2.*I2*F2;
124 stack += result;
125 stack *= OneInterfaceXTRdEdx(energy,gamma,varAngle);
126
127 // result += I2 ;
128 result = std::real(stack);
129
130 return result ;
131}
132
133
134//
135//
136////////////////////////////////////////////////////////////////////////////
137
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144
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