[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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[961] | 27 | // $Id: G4PAIxSection.hh,v 1.15 2008/05/30 16:04:40 grichine Exp $ |
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[1337] | 28 | // GEANT4 tag $Name: geant4-09-04-beta-01 $ |
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[819] | 29 | // |
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| 30 | // |
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| 31 | // G4PAIxSection.hh -- header file |
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| 32 | // |
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| 33 | // GEANT 4 class header file --- Copyright CERN 1995 |
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| 34 | // CERB Geneva Switzerland |
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| 35 | // |
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| 36 | // for information related to this code, please, contact |
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| 37 | // CERN, CN Division, ASD Group |
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| 38 | // |
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| 39 | // Preparation of ionizing collision cross section according to Photo Absorption |
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| 40 | // Ionization (PAI) model for simulation of ionization energy losses in very thin |
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| 41 | // absorbers. Author: Vladimir.Grichine@cern.ch |
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| 42 | // |
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| 43 | // History: |
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| 44 | // |
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| 45 | // 19.10.03, V. Grichine: Integral dEdx was added for G4PAIModel class |
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| 46 | // |
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| 47 | // 13.05.03, V. Grichine: Numerical instability was fixed in SumOverInterval/Border |
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| 48 | // functions |
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| 49 | // 10.02.02, V. Grichine: New functions and arrays/gets for Cerenkov and |
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| 50 | // plasmon collisions dN/dx |
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| 51 | // 27.10.99, V. Grichine: Bug fixed in constructors, 3rd constructor and |
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| 52 | // GetStepEnergyLoss(step) were added, fDelta = 0.005 |
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| 53 | // 30.11.97, V. Grichine: 2nd version |
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| 54 | // 11.06.97, V. Grichine: 1st version |
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| 55 | |
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| 56 | #ifndef G4PAIXSECTION_HH |
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| 57 | #define G4PAIXSECTION_HH |
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| 58 | |
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| 59 | #include "G4ios.hh" |
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| 60 | #include "globals.hh" |
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| 61 | #include "Randomize.hh" |
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| 62 | |
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| 63 | #include"G4SandiaTable.hh" |
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| 64 | |
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| 65 | class G4MaterialCutsCouple; |
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| 66 | class G4Sandiatable; |
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| 67 | |
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| 68 | |
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| 69 | class G4PAIxSection |
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| 70 | { |
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| 71 | public: |
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| 72 | // Constructors |
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| 73 | G4PAIxSection( G4MaterialCutsCouple* matCC); |
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| 74 | |
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| 75 | G4PAIxSection( G4int materialIndex, |
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[961] | 76 | G4double maxEnergyTransfer ); |
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[819] | 77 | |
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| 78 | G4PAIxSection( G4int materialIndex, // for proton loss table |
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| 79 | G4double maxEnergyTransfer, |
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| 80 | G4double betaGammaSq , |
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[961] | 81 | G4double** photoAbsCof, G4int intNumber ); |
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[819] | 82 | |
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| 83 | G4PAIxSection( G4int materialIndex, // test constructor |
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| 84 | G4double maxEnergyTransfer, |
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[961] | 85 | G4double betaGammaSq ); |
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[819] | 86 | |
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[961] | 87 | // G4PAIxSection(const G4PAIxSection& right); |
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[819] | 88 | |
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| 89 | // Destructor |
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| 90 | |
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[961] | 91 | ~G4PAIxSection(); |
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[819] | 92 | |
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| 93 | // Operators |
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[961] | 94 | // G4PAIxSection& operator=(const G4PAIxSection& right); |
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| 95 | // G4int operator==(const G4PAIxSection& right)const; |
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| 96 | // G4int operator!=(const G4PAIxSection& right)const; |
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[819] | 97 | |
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| 98 | // Methods |
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| 99 | |
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| 100 | // General control functions |
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| 101 | |
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[961] | 102 | void InitPAI(); |
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[819] | 103 | |
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[961] | 104 | void NormShift( G4double betaGammaSq ); |
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[819] | 105 | |
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[961] | 106 | void SplainPAI( G4double betaGammaSq ); |
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[819] | 107 | |
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| 108 | // Physical methods |
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| 109 | |
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| 110 | |
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| 111 | G4double RutherfordIntegral( G4int intervalNumber, |
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| 112 | G4double limitLow, |
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[961] | 113 | G4double limitHigh ); |
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[819] | 114 | |
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| 115 | G4double ImPartDielectricConst( G4int intervalNumber, |
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[961] | 116 | G4double energy ); |
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[819] | 117 | |
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[961] | 118 | G4double GetPhotonRange( G4double energy ); |
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| 119 | G4double GetElectronRange( G4double energy ); |
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[819] | 120 | |
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[961] | 121 | G4double RePartDielectricConst(G4double energy); |
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| 122 | |
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[819] | 123 | G4double DifPAIxSection( G4int intervalNumber, |
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[961] | 124 | G4double betaGammaSq ); |
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[819] | 125 | |
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| 126 | G4double PAIdNdxCerenkov( G4int intervalNumber, |
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[961] | 127 | G4double betaGammaSq ); |
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| 128 | G4double PAIdNdxMM( G4int intervalNumber, |
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| 129 | G4double betaGammaSq ); |
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[819] | 130 | |
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| 131 | G4double PAIdNdxPlasmon( G4int intervalNumber, |
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[961] | 132 | G4double betaGammaSq ); |
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[819] | 133 | |
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[961] | 134 | G4double PAIdNdxResonance( G4int intervalNumber, |
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| 135 | G4double betaGammaSq ); |
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[819] | 136 | |
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[961] | 137 | void IntegralPAIxSection(); |
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| 138 | void IntegralCerenkov(); |
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| 139 | void IntegralMM(); |
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| 140 | void IntegralPlasmon(); |
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| 141 | void IntegralResonance(); |
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[819] | 142 | |
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[961] | 143 | G4double SumOverInterval(G4int intervalNumber); |
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| 144 | G4double SumOverIntervaldEdx(G4int intervalNumber); |
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| 145 | G4double SumOverInterCerenkov(G4int intervalNumber); |
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| 146 | G4double SumOverInterMM(G4int intervalNumber); |
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| 147 | G4double SumOverInterPlasmon(G4int intervalNumber); |
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| 148 | G4double SumOverInterResonance(G4int intervalNumber); |
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| 149 | |
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[819] | 150 | G4double SumOverBorder( G4int intervalNumber, |
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[961] | 151 | G4double energy ); |
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[819] | 152 | G4double SumOverBorderdEdx( G4int intervalNumber, |
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[961] | 153 | G4double energy ); |
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[819] | 154 | G4double SumOverBordCerenkov( G4int intervalNumber, |
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[961] | 155 | G4double energy ); |
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| 156 | G4double SumOverBordMM( G4int intervalNumber, |
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| 157 | G4double energy ); |
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[819] | 158 | G4double SumOverBordPlasmon( G4int intervalNumber, |
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[961] | 159 | G4double energy ); |
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| 160 | G4double SumOverBordResonance( G4int intervalNumber, |
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| 161 | G4double energy ); |
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[819] | 162 | |
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[961] | 163 | G4double GetStepEnergyLoss( G4double step ); |
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| 164 | G4double GetStepCerenkovLoss( G4double step ); |
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| 165 | G4double GetStepMMLoss( G4double step ); |
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| 166 | G4double GetStepPlasmonLoss( G4double step ); |
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| 167 | G4double GetStepResonanceLoss( G4double step ); |
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[819] | 168 | |
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[961] | 169 | G4double GetEnergyTransfer(); |
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| 170 | G4double GetCerenkovEnergyTransfer(); |
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| 171 | G4double GetMMEnergyTransfer(); |
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| 172 | G4double GetPlasmonEnergyTransfer(); |
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| 173 | G4double GetResonanceEnergyTransfer(); |
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| 174 | G4double GetRutherfordEnergyTransfer(); |
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| 175 | |
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[819] | 176 | // Inline access functions |
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| 177 | |
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[961] | 178 | G4int GetNumberOfGammas() const { return fNumberOfGammas; } |
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[819] | 179 | |
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[961] | 180 | G4int GetSplineSize() const { return fSplineNumber; } |
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[819] | 181 | |
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[961] | 182 | G4int GetIntervalNumber() const { return fIntervalNumber; } |
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[819] | 183 | |
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[961] | 184 | G4double GetEnergyInterval(G4int i){ return fEnergyInterval[i]; } |
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[819] | 185 | |
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[961] | 186 | G4double GetDifPAIxSection(G4int i){ return fDifPAIxSection[i]; } |
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| 187 | G4double GetPAIdNdxCerenkov(G4int i){ return fdNdxCerenkov[i]; } |
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| 188 | G4double GetPAIdNdxMM(G4int i){ return fdNdxMM[i]; } |
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| 189 | G4double GetPAIdNdxPlasmon(G4int i){ return fdNdxPlasmon[i]; } |
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| 190 | G4double GetPAIdNdxResonance(G4int i){ return fdNdxResonance[i]; } |
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[819] | 191 | |
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[961] | 192 | G4double GetMeanEnergyLoss() const {return fIntegralPAIxSection[0]; } |
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| 193 | G4double GetMeanCerenkovLoss() const {return fIntegralCerenkov[0]; } |
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| 194 | G4double GetMeanMMLoss() const {return fIntegralMM[0]; } |
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| 195 | G4double GetMeanPlasmonLoss() const {return fIntegralPlasmon[0]; } |
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| 196 | G4double GetMeanResonanceLoss() const {return fIntegralResonance[0]; } |
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[819] | 197 | |
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[961] | 198 | G4double GetNormalizationCof() const { return fNormalizationCof; } |
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[819] | 199 | |
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[961] | 200 | inline G4double GetPAItable(G4int i,G4int j) const; |
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[819] | 201 | |
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[961] | 202 | inline G4double GetLorentzFactor(G4int i) const; |
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[819] | 203 | |
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[961] | 204 | inline G4double GetSplineEnergy(G4int i) const; |
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[819] | 205 | |
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[961] | 206 | inline G4double GetIntegralPAIxSection(G4int i) const; |
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| 207 | inline G4double GetIntegralPAIdEdx(G4int i) const; |
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| 208 | inline G4double GetIntegralCerenkov(G4int i) const; |
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| 209 | inline G4double GetIntegralMM(G4int i) const; |
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| 210 | inline G4double GetIntegralPlasmon(G4int i) const; |
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| 211 | inline G4double GetIntegralResonance(G4int i) const; |
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[819] | 212 | |
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| 213 | protected : |
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| 214 | |
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| 215 | private : |
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| 216 | |
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| 217 | // Local class constants |
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| 218 | |
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[961] | 219 | static const G4double fDelta; // energy shift from interval border = 0.001 |
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| 220 | static const G4double fError; // error in lin-log approximation = 0.005 |
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[819] | 221 | |
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[961] | 222 | static G4int fNumberOfGammas; // = 111; |
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| 223 | static const G4double fLorentzFactor[112]; // static gamma array |
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[819] | 224 | |
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| 225 | static |
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[961] | 226 | const G4int fRefGammaNumber ; // The number of gamma for creation of spline (15) |
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[819] | 227 | |
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[961] | 228 | G4int fIntervalNumber ; // The number of energy intervals |
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| 229 | G4double fNormalizationCof; // Normalization cof for PhotoAbsorptionXsection |
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[819] | 230 | |
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[961] | 231 | // G4double fBetaGammaSq; // (beta*gamma)^2 |
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[819] | 232 | |
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[961] | 233 | G4int fMaterialIndex; // current material index |
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| 234 | G4double fDensity; // Current density |
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| 235 | G4double fElectronDensity; // Current electron (number) density |
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| 236 | G4int fSplineNumber; // Current size of spline |
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[819] | 237 | |
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| 238 | // Arrays of Sandia coefficients |
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| 239 | |
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| 240 | G4OrderedTable* fMatSandiaMatrix; |
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| 241 | G4SandiaTable* fSandia; |
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| 242 | |
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[961] | 243 | G4double* fEnergyInterval; |
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| 244 | G4double* fA1; |
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| 245 | G4double* fA2; |
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| 246 | G4double* fA3; |
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| 247 | G4double* fA4; |
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[819] | 248 | |
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| 249 | static |
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[961] | 250 | const G4int fMaxSplineSize ; // Max size of output splain arrays = 500 |
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[819] | 251 | |
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| 252 | /* ****************** |
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[961] | 253 | G4double* fSplineEnergy; // energy points of splain |
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| 254 | G4double* fRePartDielectricConst; // Real part of dielectric const |
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| 255 | G4double* fImPartDielectricConst; // Imaginary part of dielectric const |
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| 256 | G4double* fIntegralTerm; // Integral term in PAI cross section |
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| 257 | G4double* fDifPAIxSection; // Differential PAI cross section |
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| 258 | G4double* fIntegralPAIxSection; // Integral PAI cross section ? |
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[819] | 259 | */ /////////////// |
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| 260 | |
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| 261 | |
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[961] | 262 | G4double fSplineEnergy[500]; // energy points of splain |
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| 263 | G4double fRePartDielectricConst[500]; // Real part of dielectric const |
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| 264 | G4double fImPartDielectricConst[500]; // Imaginary part of dielectric const |
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| 265 | G4double fIntegralTerm[500]; // Integral term in PAI cross section |
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| 266 | G4double fDifPAIxSection[500]; // Differential PAI cross section |
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| 267 | G4double fdNdxCerenkov[500]; // dNdx of Cerenkov collisions |
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| 268 | G4double fdNdxMM[500]; // dNdx of MM-Cerenkov collisions |
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| 269 | G4double fdNdxPlasmon[500]; // dNdx of Plasmon collisions |
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| 270 | G4double fdNdxResonance[500]; // dNdx of resonance collisions |
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[819] | 271 | |
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[961] | 272 | G4double fIntegralPAIxSection[500]; // Integral PAI cross section ? |
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| 273 | G4double fIntegralPAIdEdx[500]; // Integral PAI dEdx ? |
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| 274 | G4double fIntegralCerenkov[500]; // Integral Cerenkov N>omega ? |
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| 275 | G4double fIntegralMM[500]; // Integral MM-Cerenkov N>omega ? |
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| 276 | G4double fIntegralPlasmon[500]; // Integral Plasmon N>omega ? |
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| 277 | G4double fIntegralResonance[500]; // Integral resonance N>omega ? |
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[819] | 278 | |
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[961] | 279 | G4double fPAItable[500][112]; // Output array |
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[819] | 280 | |
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[961] | 281 | }; |
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[819] | 282 | |
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| 283 | //////////////// Inline methods ////////////////////////////////// |
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| 284 | // |
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| 285 | |
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| 286 | |
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| 287 | inline G4double G4PAIxSection::GetPAItable(G4int i, G4int j) const |
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| 288 | { |
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[961] | 289 | return fPAItable[i][j]; |
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[819] | 290 | } |
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| 291 | |
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| 292 | inline G4double G4PAIxSection::GetLorentzFactor(G4int j) const |
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| 293 | { |
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[961] | 294 | return fLorentzFactor[j]; |
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[819] | 295 | } |
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| 296 | |
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| 297 | inline G4double G4PAIxSection::GetSplineEnergy(G4int i) const |
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| 298 | { |
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| 299 | if(i < 1 || i > fSplineNumber) |
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| 300 | { |
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| 301 | G4Exception("Invalid argument in G4PAIxSection::GetSplineEnergy"); |
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| 302 | } |
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[961] | 303 | return fSplineEnergy[i]; |
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[819] | 304 | } |
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| 305 | |
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| 306 | inline G4double G4PAIxSection::GetIntegralPAIxSection(G4int i) const |
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| 307 | { |
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| 308 | if(i < 1 || i > fSplineNumber) |
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| 309 | { |
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| 310 | G4Exception("Invalid argument in G4PAIxSection::GetIntegralPAIxSection"); |
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| 311 | } |
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[961] | 312 | return fIntegralPAIxSection[i]; |
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[819] | 313 | } |
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| 314 | |
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| 315 | inline G4double G4PAIxSection::GetIntegralPAIdEdx(G4int i) const |
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| 316 | { |
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| 317 | if(i < 1 || i > fSplineNumber) |
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| 318 | { |
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| 319 | G4Exception("Invalid argument in G4PAIxSection::GetIntegralPAIxSection"); |
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| 320 | } |
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[961] | 321 | return fIntegralPAIdEdx[i]; |
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[819] | 322 | } |
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| 323 | |
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| 324 | inline G4double G4PAIxSection::GetIntegralCerenkov(G4int i) const |
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| 325 | { |
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| 326 | if(i < 1 || i > fSplineNumber) |
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| 327 | { |
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| 328 | G4Exception("Invalid argument in G4PAIxSection::GetIntegralCerenkov"); |
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| 329 | } |
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[961] | 330 | return fIntegralCerenkov[i]; |
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[819] | 331 | } |
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| 332 | |
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[961] | 333 | inline G4double G4PAIxSection::GetIntegralMM(G4int i) const |
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| 334 | { |
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| 335 | if(i < 1 || i > fSplineNumber) |
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| 336 | { |
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| 337 | G4Exception("Invalid argument in G4PAIxSection::GetIntegralMM"); |
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| 338 | } |
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| 339 | return fIntegralMM[i]; |
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| 340 | } |
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| 341 | |
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[819] | 342 | inline G4double G4PAIxSection::GetIntegralPlasmon(G4int i) const |
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| 343 | { |
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| 344 | if(i < 1 || i > fSplineNumber) |
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| 345 | { |
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| 346 | G4Exception("Invalid argument in G4PAIxSection::GetIntegralPlasmon"); |
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| 347 | } |
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[961] | 348 | return fIntegralPlasmon[i]; |
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[819] | 349 | } |
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| 350 | |
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[961] | 351 | inline G4double G4PAIxSection::GetIntegralResonance(G4int i) const |
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| 352 | { |
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| 353 | if(i < 1 || i > fSplineNumber) |
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| 354 | { |
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| 355 | G4Exception("Invalid argument in G4PAIxSection::GetIntegralResonance"); |
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| 356 | } |
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| 357 | return fIntegralResonance[i]; |
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| 358 | } |
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| 359 | |
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[819] | 360 | #endif |
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| 361 | |
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| 362 | // ----------------- end of G4PAIxSection header file ------------------- |
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