| [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 | //
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| 27 | // $Id: G4TransparentRegXTRadiator.cc,v 1.11 2007/09/29 17:49:34 vnivanch Exp $
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| [1007] | 28 | // GEANT4 tag $Name: geant4-09-02 $
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| [819] | 29 | //
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| 30 |
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| 31 | #include <complex>
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| 32 |
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| 33 | #include "G4TransparentRegXTRadiator.hh"
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| 34 | #include "Randomize.hh"
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| 35 | #include "G4Integrator.hh"
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| 36 | #include "G4Gamma.hh"
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| 37 |
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| 38 | using namespace std;
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| 39 |
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| 40 | ////////////////////////////////////////////////////////////////////////////
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| 41 | //
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| 42 | // Constructor, destructor
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| 43 |
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| 44 | G4TransparentRegXTRadiator::G4TransparentRegXTRadiator(G4LogicalVolume *anEnvelope,
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| 45 | G4Material* foilMat,G4Material* gasMat,
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| 46 | G4double a, G4double b, G4int n,
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| 47 | const G4String& processName) :
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| 48 | G4VXTRenergyLoss(anEnvelope,foilMat,gasMat,a,b,n,processName)
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| 49 | {
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| 50 | if(verboseLevel > 0)
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| 51 | G4cout<<"Regular transparent X-ray TR radiator EM process is called"<<G4endl;
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| 52 |
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| 53 | // Build energy and angular integral spectra of X-ray TR photons from
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| 54 | // a radiator
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| 55 |
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| 56 | fAlphaPlate = 10000;
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| 57 | fAlphaGas = 1000;
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| 58 |
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| 59 | // BuildTable();
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| 60 | }
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| 61 |
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| 62 | ///////////////////////////////////////////////////////////////////////////
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| 63 |
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| 64 | G4TransparentRegXTRadiator::~G4TransparentRegXTRadiator()
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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 | //
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| 72 |
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| 73 | G4double G4TransparentRegXTRadiator::SpectralXTRdEdx(G4double energy)
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| 74 | {
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| 75 | G4double result, sum = 0., tmp, cof1, cof2, cofMin, cofPHC,aMa, bMb, sigma;
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| 76 | G4int k, kMax, kMin;
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| 77 |
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| 78 | aMa = fPlateThick*GetPlateLinearPhotoAbs(energy);
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| 79 | bMb = fGasThick*GetGasLinearPhotoAbs(energy);
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| 80 | sigma = aMa + bMb;
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| 81 |
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| 82 | cofPHC = 4*pi*hbarc;
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| 83 | tmp = (fSigma1 - fSigma2)/cofPHC/energy;
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| 84 | cof1 = fPlateThick*tmp;
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| 85 | cof2 = fGasThick*tmp;
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| 86 |
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| 87 | cofMin = energy*(fPlateThick + fGasThick)/fGamma/fGamma;
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| 88 | cofMin += (fPlateThick*fSigma1 + fGasThick*fSigma2)/energy;
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| 89 | cofMin /= cofPHC;
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| 90 |
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| 91 | // if (fGamma < 1200) kMin = G4int(cofMin); // 1200 ?
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| 92 | // else kMin = 1;
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| 93 |
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| 94 |
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| 95 | kMin = G4int(cofMin);
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| 96 | if (cofMin > kMin) kMin++;
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| 97 |
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| 98 | // tmp = (fPlateThick + fGasThick)*energy*fMaxThetaTR;
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| 99 | // tmp /= cofPHC;
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| 100 | // kMax = G4int(tmp);
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| 101 | // if(kMax < 0) kMax = 0;
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| 102 | // kMax += kMin;
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| 103 |
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| 104 |
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| 105 | kMax = kMin + 19; // 9; // kMin + G4int(tmp);
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| 106 |
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| 107 | // tmp /= fGamma;
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| 108 | // if( G4int(tmp) < kMin ) kMin = G4int(tmp);
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| 109 | // G4cout<<"kMin = "<<kMin<<"; kMax = "<<kMax<<G4endl;
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| 110 |
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| 111 | for( k = kMin; k <= kMax; k++ )
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| 112 | {
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| 113 | tmp = pi*fPlateThick*(k + cof2)/(fPlateThick + fGasThick);
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| 114 | result = (k - cof1)*(k - cof1)*(k + cof2)*(k + cof2);
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| 115 | // tmp = sin(tmp)*sin(tmp)*abs(k-cofMin)/result;
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| 116 | if( k == kMin && kMin == G4int(cofMin) )
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| 117 | {
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| 118 | sum += 0.5*sin(tmp)*sin(tmp)*abs(k-cofMin)/result;
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| 119 | }
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| 120 | else
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| 121 | {
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| 122 | sum += sin(tmp)*sin(tmp)*abs(k-cofMin)/result;
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| 123 | }
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| 124 | if(verboseLevel > 2)
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| 125 | {
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| 126 | G4cout<<"k = "<<k<<"; tmp = "<<sin(tmp)*sin(tmp)*abs(k-cofMin)/result
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| 127 | <<"; sum = "<<sum<<G4endl;
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| 128 | }
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| 129 | }
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| 130 | result = 4*( cof1 + cof2 )*( cof1 + cof2 )*sum/energy;
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| 131 | // result *= ( 1 - exp(-0.5*fPlateNumber*sigma) )/( 1 - exp(-0.5*sigma) );
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| 132 | // fPlateNumber;
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| 133 | result *= fPlateNumber; // *exp(-0.5*fPlateNumber*sigma);
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| 134 | // +1-exp(-0.5*fPlateNumber*sigma);
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| 135 | /*
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| 136 | fEnergy = energy;
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| 137 | // G4Integrator<G4VXTRenergyLoss,G4double(G4VXTRenergyLoss::*)(G4double)> integral;
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| 138 | G4Integrator<G4TransparentRegXTRadiator,G4double(G4VXTRenergyLoss::*)(G4double)> integral;
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| 139 |
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| 140 | tmp = integral.Legendre96(this,&G4VXTRenergyLoss::SpectralAngleXTRdEdx,
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| 141 | 0.0,0.3*fMaxThetaTR) +
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| 142 | integral.Legendre96(this,&G4VXTRenergyLoss::SpectralAngleXTRdEdx,
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| 143 | 0.3*fMaxThetaTR,0.6*fMaxThetaTR) +
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| 144 | integral.Legendre96(this,&G4VXTRenergyLoss::SpectralAngleXTRdEdx,
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| 145 | 0.6*fMaxThetaTR,fMaxThetaTR) ;
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| 146 | result += tmp;
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| 147 | */
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| 148 | return result;
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| 149 | }
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| 150 |
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| 151 |
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| 152 | ///////////////////////////////////////////////////////////////////////////
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| 153 | //
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| 154 | // Approximation for radiator interference factor for the case of
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| 155 | // fully Regular radiator. The plate and gas gap thicknesses are fixed .
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| 156 | // The mean values of the plate and gas gap thicknesses
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| 157 | // are supposed to be about XTR formation zones but much less than
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| 158 | // mean absorption length of XTR photons in coresponding material.
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| 159 |
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| 160 | G4double
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| 161 | G4TransparentRegXTRadiator::GetStackFactor( G4double energy,
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| 162 | G4double gamma, G4double varAngle )
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| 163 | {
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| 164 | /*
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| 165 | G4double result, Za, Zb, Ma, Mb, sigma;
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| 166 |
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| 167 | Za = GetPlateFormationZone(energy,gamma,varAngle);
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| 168 | Zb = GetGasFormationZone(energy,gamma,varAngle);
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| 169 | Ma = GetPlateLinearPhotoAbs(energy);
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| 170 | Mb = GetGasLinearPhotoAbs(energy);
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| 171 | sigma = Ma*fPlateThick + Mb*fGasThick;
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| 172 |
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| 173 | G4complex Ca(1.0+0.5*fPlateThick*Ma/fAlphaPlate,fPlateThick/Za/fAlphaPlate);
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| 174 | G4complex Cb(1.0+0.5*fGasThick*Mb/fAlphaGas,fGasThick/Zb/fAlphaGas);
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| 175 |
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| 176 | G4complex Ha = pow(Ca,-fAlphaPlate);
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| 177 | G4complex Hb = pow(Cb,-fAlphaGas);
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| 178 | G4complex H = Ha*Hb;
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| 179 | G4complex F1 = (1.0 - Ha)*(1.0 - Hb )/(1.0 - H)
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| 180 | * G4double(fPlateNumber) ;
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| 181 | G4complex F2 = (1.0-Ha)*(1.0-Ha)*Hb/(1.0-H)/(1.0-H)
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| 182 | * (1.0 - exp(-0.5*fPlateNumber*sigma)) ;
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| 183 | // *(1.0 - pow(H,fPlateNumber)) ;
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| 184 | G4complex R = (F1 + F2)*OneInterfaceXTRdEdx(energy,gamma,varAngle);
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| 185 | // G4complex R = F2*OneInterfaceXTRdEdx(energy,gamma,varAngle);
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| 186 | result = 2.0*real(R);
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| 187 | return result;
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| 188 | */
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| 189 | // numerically unstable result
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| 190 |
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| 191 | G4double result, Qa, Qb, Q, aZa, bZb, aMa, bMb, D, sigma;
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| 192 |
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| 193 | aZa = fPlateThick/GetPlateFormationZone(energy,gamma,varAngle);
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| 194 | bZb = fGasThick/GetGasFormationZone(energy,gamma,varAngle);
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| 195 | aMa = fPlateThick*GetPlateLinearPhotoAbs(energy);
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| 196 | bMb = fGasThick*GetGasLinearPhotoAbs(energy);
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| 197 | sigma = aMa*fPlateThick + bMb*fGasThick;
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| 198 | Qa = exp(-0.5*aMa);
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| 199 | Qb = exp(-0.5*bMb);
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| 200 | Q = Qa*Qb;
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| 201 |
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| 202 | G4complex Ha( Qa*cos(aZa), -Qa*sin(aZa) );
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| 203 | G4complex Hb( Qb*cos(bZb), -Qb*sin(bZb) );
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| 204 | G4complex H = Ha*Hb;
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| 205 | G4complex Hs = conj(H);
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| 206 | D = 1.0 /( (1 - Q)*(1 - Q) +
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| 207 | 4*Q*sin(0.5*(aZa + bZb))*sin(0.5*(aZa + bZb)) );
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| 208 | G4complex F1 = (1.0 - Ha)*(1.0 - Hb)*(1.0 - Hs)
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| 209 | * G4double(fPlateNumber)*D;
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| 210 | G4complex F2 = (1.0 - Ha)*(1.0 - Ha)*Hb*(1.0 - Hs)*(1.0 - Hs)
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| 211 | // * (1.0 - pow(H,fPlateNumber)) * D*D;
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| 212 | * (1.0 - exp(-0.5*fPlateNumber*sigma)) * D*D;
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| 213 | G4complex R = (F1 + F2)*OneInterfaceXTRdEdx(energy,gamma,varAngle);
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| 214 | result = 2.0*real(R);
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| 215 | return result;
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| 216 |
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| 217 | }
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| 218 |
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| 219 |
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| 220 | //
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| 221 | //
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| 222 | ////////////////////////////////////////////////////////////////////////////
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| 223 |
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| 224 |
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| 225 |
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| 226 |
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| 227 |
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| 228 |
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| 229 |
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| 230 |
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