[807] | 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 | |
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| 28 | #include <complex> |
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| 29 | |
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| 30 | #include "Em10XTRTransparentRegRadModel.hh" |
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| 31 | #include "Randomize.hh" |
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| 32 | #include "G4Integrator.hh" |
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| 33 | #include "G4Gamma.hh" |
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| 34 | |
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| 35 | using namespace std; |
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| 36 | |
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| 37 | //////////////////////////////////////////////////////////////////////////// |
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| 38 | // |
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| 39 | // Constructor, destructor |
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| 40 | |
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| 41 | Em10XTRTransparentRegRadModel::Em10XTRTransparentRegRadModel(G4LogicalVolume *anEnvelope, |
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| 42 | G4Material* foilMat,G4Material* gasMat, |
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| 43 | G4double a, G4double b, G4int n, |
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| 44 | const G4String& processName) : |
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| 45 | G4VXTRenergyLoss(anEnvelope,foilMat,gasMat,a,b,n,processName) |
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| 46 | { |
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| 47 | G4cout<<"Regular transparent X-ray TR radiator EM process is called"<<G4endl; |
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| 48 | |
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| 49 | // Build energy and angular integral spectra of X-ray TR photons from |
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| 50 | // a radiator |
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| 51 | fExitFlux = true; |
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| 52 | fAlphaPlate = 10000; |
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| 53 | fAlphaGas = 1000; |
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| 54 | |
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| 55 | // BuildTable(); |
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| 56 | } |
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| 57 | |
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| 58 | /////////////////////////////////////////////////////////////////////////// |
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| 59 | |
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| 60 | Em10XTRTransparentRegRadModel::~Em10XTRTransparentRegRadModel() |
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| 61 | { |
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| 62 | ; |
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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 | G4double Em10XTRTransparentRegRadModel::SpectralXTRdEdx(G4double energy) |
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| 70 | { |
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| 71 | G4double result, sum = 0., tmp, cof1, cof2, cofMin, cofPHC,aMa, bMb, sigma; |
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| 72 | G4int k, kMax, kMin; |
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| 73 | |
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| 74 | aMa = GetPlateLinearPhotoAbs(energy); |
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| 75 | bMb = GetGasLinearPhotoAbs(energy); |
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| 76 | |
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| 77 | // if(fCompton) |
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| 78 | { |
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| 79 | aMa += GetPlateCompton(energy); |
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| 80 | bMb += GetGasCompton(energy); |
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| 81 | } |
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| 82 | aMa *= fPlateThick; |
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| 83 | bMb *= fGasThick; |
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| 84 | |
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| 85 | sigma = aMa + bMb; |
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| 86 | |
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| 87 | cofPHC = 4*pi*hbarc; |
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| 88 | cofPHC *= 200./197.; |
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| 89 | tmp = (fSigma1 - fSigma2)/cofPHC/energy; |
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| 90 | cof1 = fPlateThick*tmp; |
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| 91 | cof2 = fGasThick*tmp; |
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| 92 | |
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| 93 | cofMin = energy*(fPlateThick + fGasThick)/fGamma/fGamma; |
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| 94 | cofMin += (fPlateThick*fSigma1 + fGasThick*fSigma2)/energy; |
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| 95 | cofMin /= cofPHC; |
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| 96 | |
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| 97 | // if (fGamma < 1200) kMin = G4int(cofMin); // 1200 ? |
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| 98 | // else kMin = 1; |
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| 99 | |
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| 100 | |
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| 101 | kMin = G4int(cofMin); |
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| 102 | if (cofMin > kMin) kMin++; |
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| 103 | |
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| 104 | // tmp = (fPlateThick + fGasThick)*energy*fMaxThetaTR; |
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| 105 | // tmp /= cofPHC; |
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| 106 | // kMax = G4int(tmp); |
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| 107 | // if(kMax < 0) kMax = 0; |
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| 108 | // kMax += kMin; |
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| 109 | |
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| 110 | |
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| 111 | kMax = kMin + 9; // 5; // 9; // kMin + G4int(tmp); |
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| 112 | |
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| 113 | // tmp /= fGamma; |
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| 114 | // if( G4int(tmp) < kMin ) kMin = G4int(tmp); |
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| 115 | // G4cout<<"kMin = "<<kMin<<"; kMax = "<<kMax<<G4endl; |
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| 116 | |
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| 117 | for( k = kMin; k <= kMax; k++ ) |
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| 118 | { |
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| 119 | tmp = pi*fPlateThick*(k + cof2)/(fPlateThick + fGasThick); |
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| 120 | result = (k - cof1)*(k - cof1)*(k + cof2)*(k + cof2); |
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| 121 | |
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| 122 | if( k == kMin && kMin == G4int(cofMin) ) |
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| 123 | { |
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| 124 | sum += 0.5*sin(tmp)*sin(tmp)*std::abs(k-cofMin)/result; |
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| 125 | } |
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| 126 | else |
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| 127 | { |
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| 128 | sum += sin(tmp)*sin(tmp)*std::abs(k-cofMin)/result; |
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| 129 | } |
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| 130 | // G4cout<<"k = "<<k<<"; sum = "<<sum<<G4endl; |
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| 131 | } |
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| 132 | result = 4.*( cof1 + cof2 )*( cof1 + cof2 )*sum/energy; |
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| 133 | result *= ( 1. - exp(-fPlateNumber*sigma) )/( 1. - exp(-sigma) ); |
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| 134 | return result; |
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| 135 | } |
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| 136 | |
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| 137 | |
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| 138 | /////////////////////////////////////////////////////////////////////////// |
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| 139 | // |
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| 140 | // Approximation for radiator interference factor for the case of |
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| 141 | // fully Regular radiator. The plate and gas gap thicknesses are fixed . |
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| 142 | // The mean values of the plate and gas gap thicknesses |
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| 143 | // are supposed to be about XTR formation zones but much less than |
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| 144 | // mean absorption length of XTR photons in coresponding material. |
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| 145 | |
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| 146 | G4double |
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| 147 | Em10XTRTransparentRegRadModel::GetStackFactor( G4double energy, |
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| 148 | G4double gamma, G4double varAngle ) |
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| 149 | { |
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| 150 | /* |
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| 151 | G4double result, Za, Zb, Ma, Mb, sigma; |
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| 152 | |
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| 153 | Za = GetPlateFormationZone(energy,gamma,varAngle); |
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| 154 | Zb = GetGasFormationZone(energy,gamma,varAngle); |
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| 155 | Ma = GetPlateLinearPhotoAbs(energy); |
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| 156 | Mb = GetGasLinearPhotoAbs(energy); |
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| 157 | sigma = Ma*fPlateThick + Mb*fGasThick; |
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| 158 | |
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| 159 | G4complex Ca(1.0+0.5*fPlateThick*Ma/fAlphaPlate,fPlateThick/Za/fAlphaPlate); |
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| 160 | G4complex Cb(1.0+0.5*fGasThick*Mb/fAlphaGas,fGasThick/Zb/fAlphaGas); |
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| 161 | |
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| 162 | G4complex Ha = pow(Ca,-fAlphaPlate); |
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| 163 | G4complex Hb = pow(Cb,-fAlphaGas); |
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| 164 | G4complex H = Ha*Hb; |
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| 165 | G4complex F1 = (1.0 - Ha)*(1.0 - Hb )/(1.0 - H) |
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| 166 | * G4double(fPlateNumber) ; |
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| 167 | G4complex F2 = (1.0-Ha)*(1.0-Ha)*Hb/(1.0-H)/(1.0-H) |
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| 168 | * (1.0 - exp(-0.5*fPlateNumber*sigma)) ; |
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| 169 | // *(1.0 - pow(H,fPlateNumber)) ; |
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| 170 | G4complex R = (F1 + F2)*OneInterfaceXTRdEdx(energy,gamma,varAngle); |
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| 171 | // G4complex R = F2*OneInterfaceXTRdEdx(energy,gamma,varAngle); |
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| 172 | result = 2.0*real(R); |
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| 173 | return result; |
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| 174 | */ |
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| 175 | // numerically unstable result |
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| 176 | |
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| 177 | G4double result, Qa, Qb, Q, aZa, bZb, aMa, bMb, D, sigma; |
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| 178 | |
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| 179 | aZa = fPlateThick/GetPlateFormationZone(energy,gamma,varAngle); |
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| 180 | bZb = fGasThick/GetGasFormationZone(energy,gamma,varAngle); |
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| 181 | aMa = fPlateThick*GetPlateLinearPhotoAbs(energy); |
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| 182 | bMb = fGasThick*GetGasLinearPhotoAbs(energy); |
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| 183 | sigma = aMa*fPlateThick + bMb*fGasThick; |
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| 184 | Qa = exp(-0.5*aMa); |
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| 185 | Qb = exp(-0.5*bMb); |
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| 186 | Q = Qa*Qb; |
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| 187 | |
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| 188 | G4complex Ha( Qa*cos(aZa), -Qa*sin(aZa) ); |
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| 189 | G4complex Hb( Qb*cos(bZb), -Qb*sin(bZb) ); |
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| 190 | G4complex H = Ha*Hb; |
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| 191 | G4complex Hs = conj(H); |
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| 192 | D = 1.0 /( (1 - Q)*(1 - Q) + |
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| 193 | 4*Q*sin(0.5*(aZa + bZb))*sin(0.5*(aZa + bZb)) ); |
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| 194 | G4complex F1 = (1.0 - Ha)*(1.0 - Hb)*(1.0 - Hs) |
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| 195 | * G4double(fPlateNumber)*D; |
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| 196 | G4complex F2 = (1.0 - Ha)*(1.0 - Ha)*Hb*(1.0 - Hs)*(1.0 - Hs) |
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| 197 | // * (1.0 - pow(H,fPlateNumber)) * D*D; |
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| 198 | * (1.0 - exp(-0.5*fPlateNumber*sigma)) * D*D; |
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| 199 | G4complex R = (F1 + F2)*OneInterfaceXTRdEdx(energy,gamma,varAngle); |
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| 200 | result = 2.0*real(R); |
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| 201 | return result; |
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| 202 | |
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| 203 | } |
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| 204 | |
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| 205 | |
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| 206 | // |
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| 207 | // |
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| 208 | //////////////////////////////////////////////////////////////////////////// |
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| 209 | |
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| 216 | |
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