| 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: G4DiffuseElastic.hh,v 1.17 2009/09/22 16:21:46 vnivanch Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 29 | //
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| 30 | //
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| 31 | // G4 Model: optical elastic scattering with 4-momentum balance
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| 32 | //
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| 33 | // Class Description
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| 34 | // Final state production model for hadron nuclear elastic scattering;
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| 35 | // Class Description - End
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| 36 | //
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| 37 | //
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| 38 | // 24.05.07 V. Grichine first implementation for hadron (no Coulomb) elastic scattering
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| 39 | // 04.09.07 V. Grichine implementation for Coulomb elastic scattering
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| 40 |
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| 41 |
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| 42 | #ifndef G4DiffuseElastic_h
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| 43 | #define G4DiffuseElastic_h 1
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| 44 |
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| 45 | #include "globals.hh"
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| 46 | #include "G4HadronicInteraction.hh"
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| 47 | #include "G4HadProjectile.hh"
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| 48 | #include "G4Nucleus.hh"
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| 49 |
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| 50 | using namespace std;
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| 51 |
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| 52 | class G4ParticleDefinition;
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| 53 | class G4PhysicsTable;
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| 54 | class G4PhysicsLogVector;
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| 55 |
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| 56 | class G4DiffuseElastic : public G4HadronicInteraction
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| 57 | {
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| 58 | public:
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| 59 |
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| 60 | G4DiffuseElastic();
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| 61 |
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| 62 | G4DiffuseElastic(const G4ParticleDefinition* aParticle);
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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 | virtual ~G4DiffuseElastic();
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| 69 |
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| 70 | void Initialise();
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| 71 |
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| 72 | void InitialiseOnFly(G4double Z, G4double A);
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| 73 |
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| 74 | void BuildAngleTable();
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| 75 |
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| 76 |
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| 77 | G4HadFinalState * ApplyYourself(const G4HadProjectile & aTrack,
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| 78 | G4Nucleus & targetNucleus);
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| 79 |
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| 80 |
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| 81 | void SetPlabLowLimit(G4double value);
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| 82 |
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| 83 | void SetHEModelLowLimit(G4double value);
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| 84 |
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| 85 | void SetQModelLowLimit(G4double value);
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| 86 |
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| 87 | void SetLowestEnergyLimit(G4double value);
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| 88 |
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| 89 | void SetRecoilKinEnergyLimit(G4double value);
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| 90 |
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| 91 | G4double SampleT(const G4ParticleDefinition* aParticle,
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| 92 | G4double p, G4double A);
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| 93 |
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| 94 | G4double SampleTableT(const G4ParticleDefinition* aParticle,
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| 95 | G4double p, G4double Z, G4double A);
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| 96 |
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| 97 | G4double SampleThetaCMS(const G4ParticleDefinition* aParticle, G4double p, G4double A);
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| 98 |
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| 99 | G4double SampleTableThetaCMS(const G4ParticleDefinition* aParticle, G4double p,
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| 100 | G4double Z, G4double A);
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| 101 |
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| 102 | G4double GetScatteringAngle(G4int iMomentum, G4int iAngle, G4double position);
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| 103 |
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| 104 | G4double SampleThetaLab(const G4HadProjectile* aParticle,
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| 105 | G4double tmass, G4double A);
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| 106 |
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| 107 | G4double GetDiffuseElasticXsc( const G4ParticleDefinition* particle,
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| 108 | G4double theta,
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| 109 | G4double momentum,
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| 110 | G4double A );
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| 111 |
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| 112 | G4double GetInvElasticXsc( const G4ParticleDefinition* particle,
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| 113 | G4double theta,
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| 114 | G4double momentum,
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| 115 | G4double A, G4double Z );
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| 116 |
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| 117 | G4double GetDiffuseElasticSumXsc( const G4ParticleDefinition* particle,
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| 118 | G4double theta,
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| 119 | G4double momentum,
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| 120 | G4double A, G4double Z );
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| 121 |
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| 122 | G4double GetInvElasticSumXsc( const G4ParticleDefinition* particle,
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| 123 | G4double tMand,
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| 124 | G4double momentum,
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| 125 | G4double A, G4double Z );
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| 126 |
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| 127 | G4double IntegralElasticProb( const G4ParticleDefinition* particle,
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| 128 | G4double theta,
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| 129 | G4double momentum,
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| 130 | G4double A );
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| 131 |
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| 132 |
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| 133 | G4double GetCoulombElasticXsc( const G4ParticleDefinition* particle,
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| 134 | G4double theta,
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| 135 | G4double momentum,
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| 136 | G4double Z );
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| 137 |
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| 138 | G4double GetInvCoulombElasticXsc( const G4ParticleDefinition* particle,
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| 139 | G4double tMand,
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| 140 | G4double momentum,
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| 141 | G4double A, G4double Z );
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| 142 |
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| 143 | G4double GetCoulombTotalXsc( const G4ParticleDefinition* particle,
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| 144 | G4double momentum, G4double Z );
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| 145 |
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| 146 | G4double GetCoulombIntegralXsc( const G4ParticleDefinition* particle,
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| 147 | G4double momentum, G4double Z,
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| 148 | G4double theta1, G4double theta2 );
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| 149 |
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| 150 |
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| 151 | G4double CalculateParticleBeta( const G4ParticleDefinition* particle,
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| 152 | G4double momentum );
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| 153 |
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| 154 | G4double CalculateZommerfeld( G4double beta, G4double Z1, G4double Z2 );
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| 155 |
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| 156 | G4double CalculateAm( G4double momentum, G4double n, G4double Z);
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| 157 |
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| 158 | G4double CalculateNuclearRad( G4double A);
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| 159 |
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| 160 | G4double ThetaCMStoThetaLab(const G4DynamicParticle* aParticle,
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| 161 | G4double tmass, G4double thetaCMS);
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| 162 |
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| 163 | G4double ThetaLabToThetaCMS(const G4DynamicParticle* aParticle,
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| 164 | G4double tmass, G4double thetaLab);
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| 165 |
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| 166 | void TestAngleTable(const G4ParticleDefinition* theParticle, G4double partMom,
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| 167 | G4double Z, G4double A);
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| 168 |
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| 169 |
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| 170 |
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| 171 | G4double BesselJzero(G4double z);
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| 172 | G4double BesselJone(G4double z);
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| 173 | G4double DampFactor(G4double z);
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| 174 | G4double BesselOneByArg(G4double z);
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| 175 |
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| 176 | G4double GetDiffElasticProb(G4double theta);
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| 177 | G4double GetDiffElasticSumProb(G4double theta);
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| 178 | G4double GetDiffElasticSumProbA(G4double alpha);
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| 179 | G4double GetIntegrandFunction(G4double theta);
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| 180 |
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| 181 |
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| 182 | G4double GetNuclearRadius(){return fNuclearRadius;};
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| 183 |
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| 184 | private:
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| 185 |
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| 186 |
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| 187 | G4ParticleDefinition* theProton;
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| 188 | G4ParticleDefinition* theNeutron;
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| 189 | G4ParticleDefinition* theDeuteron;
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| 190 | G4ParticleDefinition* theAlpha;
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| 191 |
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| 192 | const G4ParticleDefinition* thePionPlus;
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| 193 | const G4ParticleDefinition* thePionMinus;
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| 194 |
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| 195 | G4double lowEnergyRecoilLimit;
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| 196 | G4double lowEnergyLimitHE;
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| 197 | G4double lowEnergyLimitQ;
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| 198 | G4double lowestEnergyLimit;
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| 199 | G4double plabLowLimit;
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| 200 |
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| 201 | G4int fEnergyBin;
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| 202 | G4int fAngleBin;
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| 203 |
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| 204 | G4PhysicsLogVector* fEnergyVector;
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| 205 | G4PhysicsTable* fAngleTable;
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| 206 | std::vector<G4PhysicsTable*> fAngleBank;
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| 207 |
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| 208 | std::vector<G4double> fElementNumberVector;
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| 209 | std::vector<G4String> fElementNameVector;
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| 210 |
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| 211 | const G4ParticleDefinition* fParticle;
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| 212 | G4double fWaveVector;
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| 213 | G4double fAtomicWeight;
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| 214 | G4double fAtomicNumber;
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| 215 | G4double fNuclearRadius;
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| 216 | G4double fBeta;
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| 217 | G4double fZommerfeld;
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| 218 | G4double fAm;
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| 219 | G4bool fAddCoulomb;
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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 | inline void G4DiffuseElastic::SetRecoilKinEnergyLimit(G4double value)
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| 225 | {
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| 226 | lowEnergyRecoilLimit = value;
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| 227 | }
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| 228 |
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| 229 | inline void G4DiffuseElastic::SetPlabLowLimit(G4double value)
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| 230 | {
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| 231 | plabLowLimit = value;
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| 232 | }
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| 233 |
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| 234 | inline void G4DiffuseElastic::SetHEModelLowLimit(G4double value)
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| 235 | {
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| 236 | lowEnergyLimitHE = value;
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| 237 | }
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| 238 |
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| 239 | inline void G4DiffuseElastic::SetQModelLowLimit(G4double value)
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| 240 | {
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| 241 | lowEnergyLimitQ = value;
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| 242 | }
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| 243 |
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| 244 | inline void G4DiffuseElastic::SetLowestEnergyLimit(G4double value)
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| 245 | {
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| 246 | lowestEnergyLimit = value;
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| 247 | }
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| 248 |
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| 249 |
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| 250 | /////////////////////////////////////////////////////////////
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| 251 | //
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| 252 | // Bessel J0 function based on rational approximation from
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| 253 | // J.F. Hart, Computer Approximations, New York, Willey 1968, p. 141
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| 254 |
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| 255 | inline G4double G4DiffuseElastic::BesselJzero(G4double value)
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| 256 | {
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| 257 | G4double modvalue, value2, fact1, fact2, arg, shift, bessel;
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| 258 |
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| 259 | modvalue = fabs(value);
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| 260 |
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| 261 | if ( value < 8.0 && value > -8.0 )
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| 262 | {
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| 263 | value2 = value*value;
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| 264 |
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| 265 | fact1 = 57568490574.0 + value2*(-13362590354.0
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| 266 | + value2*( 651619640.7
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| 267 | + value2*(-11214424.18
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| 268 | + value2*( 77392.33017
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| 269 | + value2*(-184.9052456 ) ) ) ) );
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| 270 |
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| 271 | fact2 = 57568490411.0 + value2*( 1029532985.0
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| 272 | + value2*( 9494680.718
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| 273 | + value2*(59272.64853
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| 274 | + value2*(267.8532712
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| 275 | + value2*1.0 ) ) ) );
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| 276 |
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| 277 | bessel = fact1/fact2;
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| 278 | }
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| 279 | else
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| 280 | {
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| 281 | arg = 8.0/modvalue;
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| 282 |
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| 283 | value2 = arg*arg;
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| 284 |
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| 285 | shift = modvalue-0.785398164;
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| 286 |
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| 287 | fact1 = 1.0 + value2*(-0.1098628627e-2
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| 288 | + value2*(0.2734510407e-4
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| 289 | + value2*(-0.2073370639e-5
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| 290 | + value2*0.2093887211e-6 ) ) );
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| 291 |
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| 292 | fact2 = -0.1562499995e-1 + value2*(0.1430488765e-3
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| 293 | + value2*(-0.6911147651e-5
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| 294 | + value2*(0.7621095161e-6
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| 295 | - value2*0.934945152e-7 ) ) );
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| 296 |
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| 297 | bessel = sqrt(0.636619772/modvalue)*(cos(shift)*fact1 - arg*sin(shift)*fact2 );
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| 298 | }
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| 299 | return bessel;
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| 300 | }
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| 301 |
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| 302 | /////////////////////////////////////////////////////////////
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| 303 | //
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| 304 | // Bessel J1 function based on rational approximation from
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| 305 | // J.F. Hart, Computer Approximations, New York, Willey 1968, p. 141
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| 306 |
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| 307 | inline G4double G4DiffuseElastic::BesselJone(G4double value)
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| 308 | {
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| 309 | G4double modvalue, value2, fact1, fact2, arg, shift, bessel;
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| 310 |
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| 311 | modvalue = fabs(value);
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| 312 |
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| 313 | if ( modvalue < 8.0 )
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| 314 | {
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| 315 | value2 = value*value;
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| 316 |
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| 317 | fact1 = value*(72362614232.0 + value2*(-7895059235.0
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| 318 | + value2*( 242396853.1
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| 319 | + value2*(-2972611.439
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| 320 | + value2*( 15704.48260
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| 321 | + value2*(-30.16036606 ) ) ) ) ) );
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| 322 |
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| 323 | fact2 = 144725228442.0 + value2*(2300535178.0
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| 324 | + value2*(18583304.74
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| 325 | + value2*(99447.43394
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| 326 | + value2*(376.9991397
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| 327 | + value2*1.0 ) ) ) );
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| 328 | bessel = fact1/fact2;
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| 329 | }
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| 330 | else
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| 331 | {
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| 332 | arg = 8.0/modvalue;
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| 333 |
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| 334 | value2 = arg*arg;
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| 335 |
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| 336 | shift = modvalue - 2.356194491;
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| 337 |
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| 338 | fact1 = 1.0 + value2*( 0.183105e-2
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| 339 | + value2*(-0.3516396496e-4
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| 340 | + value2*(0.2457520174e-5
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| 341 | + value2*(-0.240337019e-6 ) ) ) );
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| 342 |
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| 343 | fact2 = 0.04687499995 + value2*(-0.2002690873e-3
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| 344 | + value2*( 0.8449199096e-5
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| 345 | + value2*(-0.88228987e-6
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| 346 | + value2*0.105787412e-6 ) ) );
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| 347 |
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| 348 | bessel = sqrt( 0.636619772/modvalue)*(cos(shift)*fact1 - arg*sin(shift)*fact2);
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| 349 |
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| 350 | if (value < 0.0) bessel = -bessel;
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| 351 | }
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| 352 | return bessel;
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| 353 | }
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| 354 |
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| 355 | ////////////////////////////////////////////////////////////////////
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| 356 | //
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| 357 | // damp factor in diffraction x/sh(x), x was already *pi
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| 358 |
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| 359 | inline G4double G4DiffuseElastic::DampFactor(G4double x)
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| 360 | {
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| 361 | G4double df;
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| 362 | G4double f2 = 2., f3 = 6., f4 = 24.; // first factorials
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| 363 |
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| 364 | // x *= pi;
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| 365 |
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| 366 | if( std::fabs(x) < 0.01 )
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| 367 | {
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| 368 | df = 1./(1. + x/f2 + x*x/f3 + x*x*x/f4);
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| 369 | }
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| 370 | else
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| 371 | {
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| 372 | df = x/std::sinh(x);
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| 373 | }
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| 374 | return df;
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| 375 | }
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| 376 |
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| 377 |
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| 378 | ////////////////////////////////////////////////////////////////////
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| 379 | //
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| 380 | // return J1(x)/x with special case for small x
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| 381 |
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| 382 | inline G4double G4DiffuseElastic::BesselOneByArg(G4double x)
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| 383 | {
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| 384 | G4double x2, result;
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| 385 |
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| 386 | if( std::fabs(x) < 0.01 )
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| 387 | {
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| 388 | x *= 0.5;
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| 389 | x2 = x*x;
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| 390 | result = 2. - x2 + x2*x2/6.;
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| 391 | }
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| 392 | else
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| 393 | {
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| 394 | result = BesselJone(x)/x;
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| 395 | }
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| 396 | return result;
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| 397 | }
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| 398 |
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| 399 | ////////////////////////////////////////////////////////////////////
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| 400 | //
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| 401 | // return particle beta
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| 402 |
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| 403 | inline G4double G4DiffuseElastic::CalculateParticleBeta( const G4ParticleDefinition* particle,
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| 404 | G4double momentum )
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| 405 | {
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| 406 | G4double mass = particle->GetPDGMass();
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| 407 | G4double a = momentum/mass;
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| 408 | fBeta = a/std::sqrt(1+a*a);
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| 409 |
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| 410 | return fBeta;
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| 411 | }
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| 412 |
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| 413 | ////////////////////////////////////////////////////////////////////
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| 414 | //
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| 415 | // return Zommerfeld parameter for Coulomb scattering
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| 416 |
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| 417 | inline G4double G4DiffuseElastic::CalculateZommerfeld( G4double beta, G4double Z1, G4double Z2 )
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| 418 | {
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| 419 | fZommerfeld = fine_structure_const*Z1*Z2/beta;
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| 420 |
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| 421 | return fZommerfeld;
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| 422 | }
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| 423 |
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| 424 | ////////////////////////////////////////////////////////////////////
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| 425 | //
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| 426 | // return Wentzel correction for Coulomb scattering
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| 427 |
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| 428 | inline G4double G4DiffuseElastic::CalculateAm( G4double momentum, G4double n, G4double Z)
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| 429 | {
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| 430 | G4double k = momentum/hbarc;
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| 431 | G4double ch = 1.13 + 3.76*n*n;
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| 432 | G4double zn = 1.77*k*std::pow(Z,-1./3.)*Bohr_radius;
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| 433 | G4double zn2 = zn*zn;
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| 434 | fAm = ch/zn2;
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| 435 |
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| 436 | return fAm;
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| 437 | }
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| 438 |
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| 439 | ////////////////////////////////////////////////////////////////////
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| 440 | //
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| 441 | // calculate nuclear radius for different atomic weights using different approximations
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| 442 |
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| 443 | inline G4double G4DiffuseElastic::CalculateNuclearRad( G4double A)
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| 444 | {
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| 445 | G4double r0;
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| 446 |
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| 447 | if( A < 50. )
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| 448 | {
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| 449 | if( A > 10. ) r0 = 1.16*( 1 - std::pow(A, -2./3.) )*fermi; // 1.08*fermi;
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| 450 | else r0 = 1.1*fermi;
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| 451 |
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| 452 | fNuclearRadius = r0*std::pow(A, 1./3.);
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| 453 | }
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| 454 | else
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| 455 | {
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| 456 | r0 = 1.7*fermi; // 1.7*fermi;
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| 457 |
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| 458 | fNuclearRadius = r0*std::pow(A, 0.27); // 0.27);
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| 459 | }
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| 460 | return fNuclearRadius;
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| 461 | }
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| 462 |
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| 463 | ////////////////////////////////////////////////////////////////////
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| 464 | //
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| 465 | // return Coulomb scattering differential xsc with Wentzel correction
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| 466 |
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| 467 | inline G4double G4DiffuseElastic::GetCoulombElasticXsc( const G4ParticleDefinition* particle,
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| 468 | G4double theta,
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| 469 | G4double momentum,
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| 470 | G4double Z )
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|---|
| 471 | {
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|---|
| 472 | G4double sinHalfTheta = std::sin(0.5*theta);
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| 473 | G4double sinHalfTheta2 = sinHalfTheta*sinHalfTheta;
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| 474 | G4double beta = CalculateParticleBeta( particle, momentum);
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| 475 | G4double z = particle->GetPDGCharge();
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|---|
| 476 | G4double n = CalculateZommerfeld( beta, z, Z );
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|---|
| 477 | G4double am = CalculateAm( momentum, n, Z);
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|---|
| 478 | G4double k = momentum/hbarc;
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|---|
| 479 | G4double ch = 0.5*n/k;
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|---|
| 480 | G4double ch2 = ch*ch;
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|---|
| 481 | G4double xsc = ch2/(sinHalfTheta2+am)/(sinHalfTheta2+am);
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|---|
| 482 |
|
|---|
| 483 | return xsc;
|
|---|
| 484 | }
|
|---|
| 485 |
|
|---|
| 486 |
|
|---|
| 487 | ////////////////////////////////////////////////////////////////////
|
|---|
| 488 | //
|
|---|
| 489 | // return Coulomb scattering total xsc with Wentzel correction
|
|---|
| 490 |
|
|---|
| 491 | inline G4double G4DiffuseElastic::GetCoulombTotalXsc( const G4ParticleDefinition* particle,
|
|---|
| 492 | G4double momentum, G4double Z )
|
|---|
| 493 | {
|
|---|
| 494 | G4double beta = CalculateParticleBeta( particle, momentum);
|
|---|
| 495 | G4cout<<"beta = "<<beta<<G4endl;
|
|---|
| 496 | G4double z = particle->GetPDGCharge();
|
|---|
| 497 | G4double n = CalculateZommerfeld( beta, z, Z );
|
|---|
| 498 | G4cout<<"fZomerfeld = "<<n<<G4endl;
|
|---|
| 499 | G4double am = CalculateAm( momentum, n, Z);
|
|---|
| 500 | G4cout<<"cof Am = "<<am<<G4endl;
|
|---|
| 501 | G4double k = momentum/hbarc;
|
|---|
| 502 | G4cout<<"k = "<<k*fermi<<" 1/fermi"<<G4endl;
|
|---|
| 503 | G4cout<<"k*Bohr_radius = "<<k*Bohr_radius<<G4endl;
|
|---|
| 504 | G4double ch = n/k;
|
|---|
| 505 | G4double ch2 = ch*ch;
|
|---|
| 506 | G4double xsc = ch2*pi/(am +am*am);
|
|---|
| 507 |
|
|---|
| 508 | return xsc;
|
|---|
| 509 | }
|
|---|
| 510 |
|
|---|
| 511 | ////////////////////////////////////////////////////////////////////
|
|---|
| 512 | //
|
|---|
| 513 | // return Coulomb scattering xsc with Wentzel correction integrated between
|
|---|
| 514 | // theta1 and < theta2
|
|---|
| 515 |
|
|---|
| 516 | inline G4double G4DiffuseElastic::GetCoulombIntegralXsc( const G4ParticleDefinition* particle,
|
|---|
| 517 | G4double momentum, G4double Z,
|
|---|
| 518 | G4double theta1, G4double theta2 )
|
|---|
| 519 | {
|
|---|
| 520 | G4double c1 = std::cos(theta1);
|
|---|
| 521 | G4cout<<"c1 = "<<c1<<G4endl;
|
|---|
| 522 | G4double c2 = std::cos(theta2);
|
|---|
| 523 | G4cout<<"c2 = "<<c2<<G4endl;
|
|---|
| 524 | G4double beta = CalculateParticleBeta( particle, momentum);
|
|---|
| 525 | // G4cout<<"beta = "<<beta<<G4endl;
|
|---|
| 526 | G4double z = particle->GetPDGCharge();
|
|---|
| 527 | G4double n = CalculateZommerfeld( beta, z, Z );
|
|---|
| 528 | // G4cout<<"fZomerfeld = "<<n<<G4endl;
|
|---|
| 529 | G4double am = CalculateAm( momentum, n, Z);
|
|---|
| 530 | // G4cout<<"cof Am = "<<am<<G4endl;
|
|---|
| 531 | G4double k = momentum/hbarc;
|
|---|
| 532 | // G4cout<<"k = "<<k*fermi<<" 1/fermi"<<G4endl;
|
|---|
| 533 | // G4cout<<"k*Bohr_radius = "<<k*Bohr_radius<<G4endl;
|
|---|
| 534 | G4double ch = n/k;
|
|---|
| 535 | G4double ch2 = ch*ch;
|
|---|
| 536 | am *= 2.;
|
|---|
| 537 | G4double xsc = ch2*twopi*(c1-c2);
|
|---|
| 538 | xsc /= (1 - c1 + am)*(1 - c2 + am);
|
|---|
| 539 |
|
|---|
| 540 | return xsc;
|
|---|
| 541 | }
|
|---|
| 542 |
|
|---|
| 543 | #endif
|
|---|