| 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: G4RegularXTRadiator.cc,v 1.10 2010/06/16 15:34:15 gcosmo Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-04-beta-01 $
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| 29 | //
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| 30 |
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| 31 | #include <complex>
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| 32 |
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| 33 | #include "G4RegularXTRadiator.hh"
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| 34 | #include "Randomize.hh"
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| 35 |
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| 36 | #include "G4Gamma.hh"
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| 37 |
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| 38 | ////////////////////////////////////////////////////////////////////////////
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| 39 | //
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| 40 | // Constructor, destructor
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| 41 |
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| 42 | G4RegularXTRadiator::G4RegularXTRadiator(G4LogicalVolume *anEnvelope,
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| 43 | G4Material* foilMat,G4Material* gasMat,
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| 44 | G4double a, G4double b, G4int n,
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| 45 | const G4String& processName) :
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| 46 | G4VXTRenergyLoss(anEnvelope,foilMat,gasMat,a,b,n,processName)
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| 47 | {
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| 48 | G4cout<<"Regular X-ray TR radiator EM process is called"<<G4endl ;
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| 49 |
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| 50 | // Build energy and angular integral spectra of X-ray TR photons from
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| 51 | // a radiator
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| 52 |
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| 53 | fAlphaPlate = 10000;
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| 54 | fAlphaGas = 1000;
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| 55 | G4cout<<"fAlphaPlate = "<<fAlphaPlate<<" ; fAlphaGas = "<<fAlphaGas<<G4endl ;
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| 56 |
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| 57 | // BuildTable() ;
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| 58 | }
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| 59 |
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| 60 | ///////////////////////////////////////////////////////////////////////////
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| 61 |
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| 62 | G4RegularXTRadiator::~G4RegularXTRadiator()
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| 63 | {
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| 64 | ;
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| 65 | }
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| 66 |
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| 67 |
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| 68 |
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| 69 | ///////////////////////////////////////////////////////////////////////////
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| 70 | //
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| 71 | // Approximation for radiator interference factor for the case of
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| 72 | // fully Regular radiator. The plate and gas gap thicknesses are fixed .
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| 73 | // The mean values of the plate and gas gap thicknesses
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| 74 | // are supposed to be about XTR formation zones but much less than
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| 75 | // mean absorption length of XTR photons in coresponding material.
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| 76 |
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| 77 | G4double
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| 78 | G4RegularXTRadiator::GetStackFactor( G4double energy,
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| 79 | G4double gamma, G4double varAngle )
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| 80 | {
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| 81 |
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| 82 | // some gamma (10000/1000) like algorithm
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| 83 |
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| 84 | G4double result, Za, Zb, Ma, Mb;
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| 85 |
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| 86 | Za = GetPlateFormationZone(energy,gamma,varAngle);
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| 87 | Zb = GetGasFormationZone(energy,gamma,varAngle);
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| 88 |
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| 89 | Ma = GetPlateLinearPhotoAbs(energy);
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| 90 | Mb = GetGasLinearPhotoAbs(energy);
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| 91 |
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| 92 |
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| 93 | G4complex Ca(1.0+0.5*fPlateThick*Ma/fAlphaPlate,fPlateThick/Za/fAlphaPlate);
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| 94 | G4complex Cb(1.0+0.5*fGasThick*Mb/fAlphaGas,fGasThick/Zb/fAlphaGas);
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| 95 |
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| 96 | G4complex Ha = std::pow(Ca,-fAlphaPlate);
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| 97 | G4complex Hb = std::pow(Cb,-fAlphaGas);
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| 98 | G4complex H = Ha*Hb;
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| 99 |
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| 100 | G4complex F1 = (1.0 - Ha)*(1.0 - Hb )/(1.0 - H)
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| 101 | * G4double(fPlateNumber);
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| 102 |
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| 103 | G4complex F2 = (1.0-Ha)*(1.0-Ha)*Hb/(1.0-H)/(1.0-H)
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| 104 | * (1.0 - std::pow(H,fPlateNumber));
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| 105 |
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| 106 | G4complex R = (F1 + F2)*OneInterfaceXTRdEdx(energy,gamma,varAngle);
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| 107 |
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| 108 | result = 2.0*std::real(R);
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| 109 |
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| 110 | return result;
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| 111 |
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| 112 | /*
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| 113 | // numerically stable but slow algorithm
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| 114 |
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| 115 | G4double result, Qa, Qb, Q, aZa, bZb, aMa, bMb; // , D;
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| 116 |
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| 117 | aZa = fPlateThick/GetPlateFormationZone(energy,gamma,varAngle);
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| 118 | bZb = fGasThick/GetGasFormationZone(energy,gamma,varAngle);
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| 119 | aMa = fPlateThick*GetPlateLinearPhotoAbs(energy);
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| 120 | bMb = fGasThick*GetGasLinearPhotoAbs(energy);
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| 121 | Qa = std::exp(-aMa);
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| 122 | Qb = std::exp(-bMb);
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| 123 | Q = Qa*Qb;
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| 124 | G4complex Ha( std::exp(-0.5*aMa)*std::cos(aZa),
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| 125 | -std::exp(-0.5*aMa)*std::sin(aZa) );
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| 126 | G4complex Hb( std::exp(-0.5*bMb)*std::cos(bZb),
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| 127 | -std::exp(-0.5*bMb)*std::sin(bZb) );
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| 128 | G4complex H = Ha*Hb;
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| 129 |
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| 130 | G4complex Hs = conj(H);
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| 131 | D = 1.0 /( (1 - std::sqrt(Q))*(1 - std::sqrt(Q)) +
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| 132 | 4*std::sqrt(Q)*std::sin(0.5*(aZa+bZb))*std::sin(0.5*(aZa+bZb)) );
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| 133 | G4complex F1 = (1.0 - Ha)*(1.0 - Hb)*(1.0 - Hs)
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| 134 | * G4double(fPlateNumber)*D;
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| 135 | G4complex F2 = (1.0-Ha)*(1.0-Ha)*Hb*(1.0-Hs)*(1.0-Hs)
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| 136 | * (1.0 - std::pow(H,fPlateNumber)) * D*D;
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| 137 | G4complex R = (F1 + F2)*OneInterfaceXTRdEdx(energy,gamma,varAngle);
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| 138 |
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| 139 |
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| 140 | G4complex S(0.,0.), c(1.,0.);
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| 141 | G4int k;
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| 142 | for(k = 1; k < fPlateNumber; k++)
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| 143 | {
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| 144 | c *= H;
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| 145 | S += ( G4double(fPlateNumber) - G4double(k) )*c;
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| 146 | }
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| 147 | G4complex R = (2.- Ha - 1./Ha)*S + (1. - Ha)*G4double(fPlateNumber);
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| 148 | R *= OneInterfaceXTRdEdx(energy,gamma,varAngle);
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| 149 | result = 2.0*std::real(R);
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| 150 | return result;
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| 151 | */
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| 152 | }
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| 153 |
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| 154 |
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| 155 | //
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| 156 | //
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| 157 | ////////////////////////////////////////////////////////////////////////////
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| 158 |
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| 159 |
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| 160 |
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| 161 |
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| 162 |
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| 163 |
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| 164 |
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| 165 |
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