| 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: G4NuclNuclDiffuseElastic.hh,v 1.8 2009/04/10 13:22:25 grichine Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-03 $
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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 nucleus-nucleus elastic scattering;
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| 35 | // Coulomb amplitude is not considered as correction
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| 36 | // (as in G4DiffuseElastic)
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| 37 | // Class Description - End
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| 38 | //
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| 39 | //
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| 40 | // 17.03.09 V. Grichine implementation for Coulomb elastic scattering
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| 41 |
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| 42 |
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| 43 | #ifndef G4NuclNuclDiffuseElastic_h
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| 44 | #define G4NuclNuclDiffuseElastic_h 1
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| 45 |
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| 46 | #include "globals.hh"
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| 47 | #include <complex>
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| 48 | #include "G4Integrator.hh"
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| 49 |
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| 50 | #include "G4HadronicInteraction.hh"
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| 51 | #include "G4HadProjectile.hh"
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| 52 | #include "G4Nucleus.hh"
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| 53 |
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| 54 | using namespace std;
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| 55 |
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| 56 | class G4ParticleDefinition;
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| 57 | class G4PhysicsTable;
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| 58 | class G4PhysicsLogVector;
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| 59 |
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| 60 | class G4NuclNuclDiffuseElastic : public G4HadronicInteraction
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| 61 | {
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| 62 | public:
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| 63 |
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| 64 | G4NuclNuclDiffuseElastic();
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| 65 |
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| 66 | G4NuclNuclDiffuseElastic(const G4ParticleDefinition* aParticle);
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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 | virtual ~G4NuclNuclDiffuseElastic();
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| 73 |
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| 74 | void Initialise();
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| 75 |
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| 76 | void InitialiseOnFly(G4double Z, G4double A);
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| 77 |
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| 78 | void BuildAngleTable();
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| 79 |
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| 80 |
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| 81 | G4HadFinalState * ApplyYourself(const G4HadProjectile & aTrack,
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| 82 | G4Nucleus & targetNucleus);
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| 83 |
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| 84 |
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| 85 | void SetPlabLowLimit(G4double value);
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| 86 |
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| 87 | void SetHEModelLowLimit(G4double value);
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| 88 |
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| 89 | void SetQModelLowLimit(G4double value);
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| 90 |
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| 91 | void SetLowestEnergyLimit(G4double value);
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| 92 |
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| 93 | void SetRecoilKinEnergyLimit(G4double value);
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| 94 |
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| 95 | G4double SampleT(const G4ParticleDefinition* aParticle,
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| 96 | G4double p, G4double A);
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| 97 |
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| 98 | G4double SampleTableT(const G4ParticleDefinition* aParticle,
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| 99 | G4double p, G4double Z, G4double A);
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| 100 |
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| 101 | G4double SampleThetaCMS(const G4ParticleDefinition* aParticle, G4double p, G4double A);
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| 102 |
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| 103 | G4double SampleTableThetaCMS(const G4ParticleDefinition* aParticle, G4double p,
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| 104 | G4double Z, G4double A);
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| 105 |
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| 106 | G4double GetScatteringAngle(G4int iMomentum, G4int iAngle, G4double position);
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| 107 |
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| 108 | G4double SampleThetaLab(const G4HadProjectile* aParticle,
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| 109 | G4double tmass, G4double A);
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| 110 |
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| 111 | G4double GetDiffuseElasticXsc( const G4ParticleDefinition* particle,
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| 112 | G4double theta,
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| 113 | G4double momentum,
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| 114 | G4double A );
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| 115 |
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| 116 | G4double GetInvElasticXsc( const G4ParticleDefinition* particle,
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| 117 | G4double theta,
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| 118 | G4double momentum,
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| 119 | G4double A, G4double Z );
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| 120 |
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| 121 | G4double GetDiffuseElasticSumXsc( const G4ParticleDefinition* particle,
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| 122 | G4double theta,
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| 123 | G4double momentum,
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| 124 | G4double A, G4double Z );
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| 125 |
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| 126 | G4double GetInvElasticSumXsc( const G4ParticleDefinition* particle,
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| 127 | G4double tMand,
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| 128 | G4double momentum,
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| 129 | G4double A, G4double Z );
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| 130 |
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| 131 | G4double IntegralElasticProb( const G4ParticleDefinition* particle,
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| 132 | G4double theta,
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| 133 | G4double momentum,
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| 134 | G4double A );
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| 135 |
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| 136 |
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| 137 | G4double GetCoulombElasticXsc( const G4ParticleDefinition* particle,
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| 138 | G4double theta,
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| 139 | G4double momentum,
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| 140 | G4double Z );
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| 141 |
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| 142 | G4double GetInvCoulombElasticXsc( const G4ParticleDefinition* particle,
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| 143 | G4double tMand,
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| 144 | G4double momentum,
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| 145 | G4double A, G4double Z );
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| 146 |
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| 147 | G4double GetCoulombTotalXsc( const G4ParticleDefinition* particle,
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| 148 | G4double momentum, G4double Z );
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| 149 |
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| 150 | G4double GetCoulombIntegralXsc( const G4ParticleDefinition* particle,
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| 151 | G4double momentum, G4double Z,
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| 152 | G4double theta1, G4double theta2 );
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| 153 |
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| 154 |
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| 155 | G4double CalculateParticleBeta( const G4ParticleDefinition* particle,
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| 156 | G4double momentum );
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| 157 |
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| 158 | G4double CalculateZommerfeld( G4double beta, G4double Z1, G4double Z2 );
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| 159 |
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| 160 | G4double CalculateAm( G4double momentum, G4double n, G4double Z);
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| 161 |
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| 162 | G4double CalculateNuclearRad( G4double A);
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| 163 |
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| 164 | G4double ThetaCMStoThetaLab(const G4DynamicParticle* aParticle,
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| 165 | G4double tmass, G4double thetaCMS);
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| 166 |
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| 167 | G4double ThetaLabToThetaCMS(const G4DynamicParticle* aParticle,
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| 168 | G4double tmass, G4double thetaLab);
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| 169 |
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| 170 | void TestAngleTable(const G4ParticleDefinition* theParticle, G4double partMom,
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| 171 | G4double Z, G4double A);
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| 172 |
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| 173 |
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| 174 |
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| 175 | G4double BesselJzero(G4double z);
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| 176 | G4double BesselJone(G4double z);
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| 177 | G4double DampFactor(G4double z);
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| 178 | G4double BesselOneByArg(G4double z);
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| 179 |
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| 180 | G4double GetDiffElasticProb(G4double theta);
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| 181 | G4double GetDiffElasticSumProb(G4double theta);
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| 182 | G4double GetDiffElasticSumProbA(G4double alpha);
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| 183 | G4double GetIntegrandFunction(G4double theta);
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| 184 |
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| 185 | G4double GetNuclearRadius(){return fNuclearRadius;};
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| 186 |
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| 187 |
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| 188 | // Technical math functions for strong Coulomb contribution
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| 189 |
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| 190 | G4complex GammaLogarithm(G4complex xx);
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| 191 |
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| 192 | G4double GetErf(G4double x);
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| 193 |
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| 194 | G4complex GetErfcComp(G4complex z, G4int nMax);
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| 195 | G4complex GetErfcSer(G4complex z, G4int nMax);
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| 196 | G4complex GetErfcInt(G4complex z); // , G4int nMax);
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| 197 |
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| 198 | G4complex GetErfComp(G4complex z, G4int nMax); // AandS algorithm != Ser, Int
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| 199 | G4complex GetErfSer(G4complex z, G4int nMax);
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| 200 |
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| 201 | G4double GetExpCos(G4double x);
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| 202 | G4double GetExpSin(G4double x);
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| 203 | G4complex GetErfInt(G4complex z); // , G4int nMax);
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| 204 |
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| 205 |
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| 206 | G4complex TestErfcComp(G4complex z, G4int nMax);
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| 207 | G4complex TestErfcSer(G4complex z, G4int nMax);
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| 208 | G4complex TestErfcInt(G4complex z); // , G4int nMax);
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| 209 |
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| 210 | G4complex CoulombAmplitude(G4double theta);
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| 211 | void CalculateCoulombPhaseZero();
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| 212 | void CalculateRutherfordAnglePar();
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| 213 |
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| 214 | G4double ProfileNear(G4double theta);
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| 215 | G4double ProfileFar(G4double theta);
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| 216 |
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| 217 | G4complex PhaseNear(G4double theta);
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| 218 | G4complex PhaseFar(G4double theta);
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| 219 |
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| 220 | G4complex GammaLess(G4double theta);
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| 221 | G4complex GammaMore(G4double theta);
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| 222 |
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| 223 | G4complex AmplitudeNear(G4double theta);
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| 224 | G4complex AmplitudeFar(G4double theta);
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| 225 | G4complex Amplitude(G4double theta);
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| 226 | G4double AmplitudeMod2(G4double theta);
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| 227 | void InitParameters(const G4ParticleDefinition* theParticle,
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| 228 | G4double partMom, G4double Z, G4double A);
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| 229 |
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| 230 | G4double GetProfileLambda(){return fProfileLambda;};
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| 231 |
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| 232 | void SetProfileLambda(G4double pl) {fProfileLambda = pl;};
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| 233 | void SetProfileDelta(G4double pd) {fProfileDelta = pd;};
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| 234 | void SetProfileAlpha(G4double pa){fProfileAlpha = pa;};
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| 235 |
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| 236 | private:
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| 237 |
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| 238 |
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| 239 | G4ParticleDefinition* theProton;
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| 240 | G4ParticleDefinition* theNeutron;
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| 241 | G4ParticleDefinition* theDeuteron;
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| 242 | G4ParticleDefinition* theAlpha;
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| 243 |
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| 244 | const G4ParticleDefinition* thePionPlus;
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| 245 | const G4ParticleDefinition* thePionMinus;
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| 246 |
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| 247 | G4double lowEnergyRecoilLimit;
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| 248 | G4double lowEnergyLimitHE;
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| 249 | G4double lowEnergyLimitQ;
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| 250 | G4double lowestEnergyLimit;
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| 251 | G4double plabLowLimit;
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| 252 |
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| 253 | G4int fEnergyBin;
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| 254 | G4int fAngleBin;
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| 255 |
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| 256 | G4PhysicsLogVector* fEnergyVector;
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| 257 | G4PhysicsTable* fAngleTable;
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| 258 | std::vector<G4PhysicsTable*> fAngleBank;
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| 259 |
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| 260 | std::vector<G4double> fElementNumberVector;
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| 261 | std::vector<G4String> fElementNameVector;
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| 262 |
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| 263 | const G4ParticleDefinition* fParticle;
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| 264 | G4double fWaveVector;
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| 265 | G4double fAtomicWeight;
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| 266 | G4double fAtomicNumber;
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| 267 |
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| 268 | G4double fNuclearRadius1;
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| 269 | G4double fNuclearRadius2;
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| 270 | G4double fNuclearRadius;
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| 271 |
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| 272 | G4double fBeta;
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| 273 | G4double fZommerfeld;
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| 274 | G4double fAm;
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| 275 | G4bool fAddCoulomb;
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| 276 |
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| 277 | G4double fCoulombPhase0;
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| 278 | G4double fHalfRutThetaTg;
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| 279 | G4double fRutherfordTheta;
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| 280 |
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| 281 | G4double fProfileLambda;
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| 282 | G4double fProfileDelta;
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| 283 | G4double fProfileAlpha;
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| 284 |
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| 285 | G4double fReZ;
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| 286 |
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| 287 | };
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| 288 |
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| 289 |
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| 290 | inline void G4NuclNuclDiffuseElastic::SetRecoilKinEnergyLimit(G4double value)
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| 291 | {
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| 292 | lowEnergyRecoilLimit = value;
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| 293 | }
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| 294 |
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| 295 | inline void G4NuclNuclDiffuseElastic::SetPlabLowLimit(G4double value)
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| 296 | {
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| 297 | plabLowLimit = value;
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| 298 | }
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| 299 |
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| 300 | inline void G4NuclNuclDiffuseElastic::SetHEModelLowLimit(G4double value)
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| 301 | {
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| 302 | lowEnergyLimitHE = value;
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| 303 | }
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| 304 |
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| 305 | inline void G4NuclNuclDiffuseElastic::SetQModelLowLimit(G4double value)
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| 306 | {
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| 307 | lowEnergyLimitQ = value;
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| 308 | }
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| 309 |
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| 310 | inline void G4NuclNuclDiffuseElastic::SetLowestEnergyLimit(G4double value)
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| 311 | {
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| 312 | lowestEnergyLimit = value;
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| 313 | }
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| 314 |
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| 315 |
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| 316 | /////////////////////////////////////////////////////////////
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| 317 | //
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| 318 | // Bessel J0 function based on rational approximation from
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| 319 | // J.F. Hart, Computer Approximations, New York, Willey 1968, p. 141
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| 320 |
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| 321 | inline G4double G4NuclNuclDiffuseElastic::BesselJzero(G4double value)
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| 322 | {
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| 323 | G4double modvalue, value2, fact1, fact2, arg, shift, bessel;
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| 324 |
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| 325 | modvalue = fabs(value);
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| 326 |
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| 327 | if ( value < 8.0 && value > -8.0 )
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| 328 | {
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| 329 | value2 = value*value;
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| 330 |
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| 331 | fact1 = 57568490574.0 + value2*(-13362590354.0
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| 332 | + value2*( 651619640.7
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| 333 | + value2*(-11214424.18
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| 334 | + value2*( 77392.33017
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| 335 | + value2*(-184.9052456 ) ) ) ) );
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| 336 |
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| 337 | fact2 = 57568490411.0 + value2*( 1029532985.0
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| 338 | + value2*( 9494680.718
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| 339 | + value2*(59272.64853
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| 340 | + value2*(267.8532712
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| 341 | + value2*1.0 ) ) ) );
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| 342 |
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| 343 | bessel = fact1/fact2;
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| 344 | }
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| 345 | else
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| 346 | {
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| 347 | arg = 8.0/modvalue;
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| 348 |
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| 349 | value2 = arg*arg;
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| 350 |
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| 351 | shift = modvalue-0.785398164;
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| 352 |
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| 353 | fact1 = 1.0 + value2*(-0.1098628627e-2
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| 354 | + value2*(0.2734510407e-4
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| 355 | + value2*(-0.2073370639e-5
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| 356 | + value2*0.2093887211e-6 ) ) );
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| 357 |
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| 358 | fact2 = -0.1562499995e-1 + value2*(0.1430488765e-3
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| 359 | + value2*(-0.6911147651e-5
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| 360 | + value2*(0.7621095161e-6
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| 361 | - value2*0.934945152e-7 ) ) );
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| 362 |
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| 363 | bessel = sqrt(0.636619772/modvalue)*(cos(shift)*fact1 - arg*sin(shift)*fact2 );
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| 364 | }
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| 365 | return bessel;
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| 366 | }
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| 367 |
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| 368 | /////////////////////////////////////////////////////////////
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| 369 | //
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| 370 | // Bessel J1 function based on rational approximation from
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| 371 | // J.F. Hart, Computer Approximations, New York, Willey 1968, p. 141
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| 372 |
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| 373 | inline G4double G4NuclNuclDiffuseElastic::BesselJone(G4double value)
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| 374 | {
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| 375 | G4double modvalue, value2, fact1, fact2, arg, shift, bessel;
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| 376 |
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| 377 | modvalue = fabs(value);
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| 378 |
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| 379 | if ( modvalue < 8.0 )
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| 380 | {
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| 381 | value2 = value*value;
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| 382 |
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| 383 | fact1 = value*(72362614232.0 + value2*(-7895059235.0
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| 384 | + value2*( 242396853.1
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| 385 | + value2*(-2972611.439
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| 386 | + value2*( 15704.48260
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| 387 | + value2*(-30.16036606 ) ) ) ) ) );
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| 388 |
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| 389 | fact2 = 144725228442.0 + value2*(2300535178.0
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| 390 | + value2*(18583304.74
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| 391 | + value2*(99447.43394
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| 392 | + value2*(376.9991397
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| 393 | + value2*1.0 ) ) ) );
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| 394 | bessel = fact1/fact2;
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| 395 | }
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| 396 | else
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| 397 | {
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| 398 | arg = 8.0/modvalue;
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| 399 |
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| 400 | value2 = arg*arg;
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| 401 |
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| 402 | shift = modvalue - 2.356194491;
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| 403 |
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| 404 | fact1 = 1.0 + value2*( 0.183105e-2
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| 405 | + value2*(-0.3516396496e-4
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| 406 | + value2*(0.2457520174e-5
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| 407 | + value2*(-0.240337019e-6 ) ) ) );
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| 408 |
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| 409 | fact2 = 0.04687499995 + value2*(-0.2002690873e-3
|
|---|
| 410 | + value2*( 0.8449199096e-5
|
|---|
| 411 | + value2*(-0.88228987e-6
|
|---|
| 412 | + value2*0.105787412e-6 ) ) );
|
|---|
| 413 |
|
|---|
| 414 | bessel = sqrt( 0.636619772/modvalue)*(cos(shift)*fact1 - arg*sin(shift)*fact2);
|
|---|
| 415 |
|
|---|
| 416 | if (value < 0.0) bessel = -bessel;
|
|---|
| 417 | }
|
|---|
| 418 | return bessel;
|
|---|
| 419 | }
|
|---|
| 420 |
|
|---|
| 421 | ////////////////////////////////////////////////////////////////////
|
|---|
| 422 | //
|
|---|
| 423 | // damp factor in diffraction x/sh(x), x was already *pi
|
|---|
| 424 |
|
|---|
| 425 | inline G4double G4NuclNuclDiffuseElastic::DampFactor(G4double x)
|
|---|
| 426 | {
|
|---|
| 427 | G4double df;
|
|---|
| 428 | G4double f2 = 2., f3 = 6., f4 = 24.; // first factorials
|
|---|
| 429 |
|
|---|
| 430 | // x *= pi;
|
|---|
| 431 |
|
|---|
| 432 | if( std::fabs(x) < 0.01 )
|
|---|
| 433 | {
|
|---|
| 434 | df = 1./(1. + x/f2 + x*x/f3 + x*x*x/f4);
|
|---|
| 435 | }
|
|---|
| 436 | else
|
|---|
| 437 | {
|
|---|
| 438 | df = x/std::sinh(x);
|
|---|
| 439 | }
|
|---|
| 440 | return df;
|
|---|
| 441 | }
|
|---|
| 442 |
|
|---|
| 443 |
|
|---|
| 444 | ////////////////////////////////////////////////////////////////////
|
|---|
| 445 | //
|
|---|
| 446 | // return J1(x)/x with special case for small x
|
|---|
| 447 |
|
|---|
| 448 | inline G4double G4NuclNuclDiffuseElastic::BesselOneByArg(G4double x)
|
|---|
| 449 | {
|
|---|
| 450 | G4double x2, result;
|
|---|
| 451 |
|
|---|
| 452 | if( std::fabs(x) < 0.01 )
|
|---|
| 453 | {
|
|---|
| 454 | x *= 0.5;
|
|---|
| 455 | x2 = x*x;
|
|---|
| 456 | result = 2. - x2 + x2*x2/6.;
|
|---|
| 457 | }
|
|---|
| 458 | else
|
|---|
| 459 | {
|
|---|
| 460 | result = BesselJone(x)/x;
|
|---|
| 461 | }
|
|---|
| 462 | return result;
|
|---|
| 463 | }
|
|---|
| 464 |
|
|---|
| 465 | ////////////////////////////////////////////////////////////////////
|
|---|
| 466 | //
|
|---|
| 467 | // return particle beta
|
|---|
| 468 |
|
|---|
| 469 | inline G4double G4NuclNuclDiffuseElastic::CalculateParticleBeta( const G4ParticleDefinition* particle,
|
|---|
| 470 | G4double momentum )
|
|---|
| 471 | {
|
|---|
| 472 | G4double mass = particle->GetPDGMass();
|
|---|
| 473 | G4double a = momentum/mass;
|
|---|
| 474 | fBeta = a/std::sqrt(1+a*a);
|
|---|
| 475 |
|
|---|
| 476 | return fBeta;
|
|---|
| 477 | }
|
|---|
| 478 |
|
|---|
| 479 | ////////////////////////////////////////////////////////////////////
|
|---|
| 480 | //
|
|---|
| 481 | // return Zommerfeld parameter for Coulomb scattering
|
|---|
| 482 |
|
|---|
| 483 | inline G4double G4NuclNuclDiffuseElastic::CalculateZommerfeld( G4double beta, G4double Z1, G4double Z2 )
|
|---|
| 484 | {
|
|---|
| 485 | fZommerfeld = fine_structure_const*Z1*Z2/beta;
|
|---|
| 486 |
|
|---|
| 487 | return fZommerfeld;
|
|---|
| 488 | }
|
|---|
| 489 |
|
|---|
| 490 | ////////////////////////////////////////////////////////////////////
|
|---|
| 491 | //
|
|---|
| 492 | // return Wentzel correction for Coulomb scattering
|
|---|
| 493 |
|
|---|
| 494 | inline G4double G4NuclNuclDiffuseElastic::CalculateAm( G4double momentum, G4double n, G4double Z)
|
|---|
| 495 | {
|
|---|
| 496 | G4double k = momentum/hbarc;
|
|---|
| 497 | G4double ch = 1.13 + 3.76*n*n;
|
|---|
| 498 | G4double zn = 1.77*k*std::pow(Z,-1./3.)*Bohr_radius;
|
|---|
| 499 | G4double zn2 = zn*zn;
|
|---|
| 500 | fAm = ch/zn2;
|
|---|
| 501 |
|
|---|
| 502 | return fAm;
|
|---|
| 503 | }
|
|---|
| 504 |
|
|---|
| 505 | ////////////////////////////////////////////////////////////////////
|
|---|
| 506 | //
|
|---|
| 507 | // calculate nuclear radius for different atomic weights using different approximations
|
|---|
| 508 |
|
|---|
| 509 | inline G4double G4NuclNuclDiffuseElastic::CalculateNuclearRad( G4double A)
|
|---|
| 510 | {
|
|---|
| 511 | G4double r0, radius;
|
|---|
| 512 |
|
|---|
| 513 | if( A < 50. )
|
|---|
| 514 | {
|
|---|
| 515 | if( A > 10. ) r0 = 1.16*( 1 - std::pow(A, -2./3.) )*fermi; // 1.08*fermi;
|
|---|
| 516 | else r0 = 1.1*fermi;
|
|---|
| 517 |
|
|---|
| 518 | radius = r0*std::pow(A, 1./3.);
|
|---|
| 519 | }
|
|---|
| 520 | else
|
|---|
| 521 | {
|
|---|
| 522 | r0 = 1.7*fermi; // 1.7*fermi;
|
|---|
| 523 |
|
|---|
| 524 | radius = r0*std::pow(A, 0.27); // 0.27);
|
|---|
| 525 | }
|
|---|
| 526 | return radius;
|
|---|
| 527 | }
|
|---|
| 528 |
|
|---|
| 529 | ////////////////////////////////////////////////////////////////////
|
|---|
| 530 | //
|
|---|
| 531 | // return Coulomb scattering differential xsc with Wentzel correction
|
|---|
| 532 |
|
|---|
| 533 | inline G4double G4NuclNuclDiffuseElastic::GetCoulombElasticXsc( const G4ParticleDefinition* particle,
|
|---|
| 534 | G4double theta,
|
|---|
| 535 | G4double momentum,
|
|---|
| 536 | G4double Z )
|
|---|
| 537 | {
|
|---|
| 538 | G4double sinHalfTheta = std::sin(0.5*theta);
|
|---|
| 539 | G4double sinHalfTheta2 = sinHalfTheta*sinHalfTheta;
|
|---|
| 540 | G4double beta = CalculateParticleBeta( particle, momentum);
|
|---|
| 541 | G4double z = particle->GetPDGCharge();
|
|---|
| 542 | G4double n = CalculateZommerfeld( beta, z, Z );
|
|---|
| 543 | G4double am = CalculateAm( momentum, n, Z);
|
|---|
| 544 | G4double k = momentum/hbarc;
|
|---|
| 545 | G4double ch = 0.5*n/k;
|
|---|
| 546 | G4double ch2 = ch*ch;
|
|---|
| 547 | G4double xsc = ch2/(sinHalfTheta2+am)/(sinHalfTheta2+am);
|
|---|
| 548 |
|
|---|
| 549 | return xsc;
|
|---|
| 550 | }
|
|---|
| 551 |
|
|---|
| 552 |
|
|---|
| 553 | ////////////////////////////////////////////////////////////////////
|
|---|
| 554 | //
|
|---|
| 555 | // return Coulomb scattering total xsc with Wentzel correction
|
|---|
| 556 |
|
|---|
| 557 | inline G4double G4NuclNuclDiffuseElastic::GetCoulombTotalXsc( const G4ParticleDefinition* particle,
|
|---|
| 558 | G4double momentum, G4double Z )
|
|---|
| 559 | {
|
|---|
| 560 | G4double beta = CalculateParticleBeta( particle, momentum);
|
|---|
| 561 | G4cout<<"beta = "<<beta<<G4endl;
|
|---|
| 562 | G4double z = particle->GetPDGCharge();
|
|---|
| 563 | G4double n = CalculateZommerfeld( beta, z, Z );
|
|---|
| 564 | G4cout<<"fZomerfeld = "<<n<<G4endl;
|
|---|
| 565 | G4double am = CalculateAm( momentum, n, Z);
|
|---|
| 566 | G4cout<<"cof Am = "<<am<<G4endl;
|
|---|
| 567 | G4double k = momentum/hbarc;
|
|---|
| 568 | G4cout<<"k = "<<k*fermi<<" 1/fermi"<<G4endl;
|
|---|
| 569 | G4cout<<"k*Bohr_radius = "<<k*Bohr_radius<<G4endl;
|
|---|
| 570 | G4double ch = n/k;
|
|---|
| 571 | G4double ch2 = ch*ch;
|
|---|
| 572 | G4double xsc = ch2*pi/(am +am*am);
|
|---|
| 573 |
|
|---|
| 574 | return xsc;
|
|---|
| 575 | }
|
|---|
| 576 |
|
|---|
| 577 | ////////////////////////////////////////////////////////////////////
|
|---|
| 578 | //
|
|---|
| 579 | // return Coulomb scattering xsc with Wentzel correction integrated between
|
|---|
| 580 | // theta1 and < theta2
|
|---|
| 581 |
|
|---|
| 582 | inline G4double G4NuclNuclDiffuseElastic::GetCoulombIntegralXsc( const G4ParticleDefinition* particle,
|
|---|
| 583 | G4double momentum, G4double Z,
|
|---|
| 584 | G4double theta1, G4double theta2 )
|
|---|
| 585 | {
|
|---|
| 586 | G4double c1 = std::cos(theta1);
|
|---|
| 587 | G4cout<<"c1 = "<<c1<<G4endl;
|
|---|
| 588 | G4double c2 = std::cos(theta2);
|
|---|
| 589 | G4cout<<"c2 = "<<c2<<G4endl;
|
|---|
| 590 | G4double beta = CalculateParticleBeta( particle, momentum);
|
|---|
| 591 | // G4cout<<"beta = "<<beta<<G4endl;
|
|---|
| 592 | G4double z = particle->GetPDGCharge();
|
|---|
| 593 | G4double n = CalculateZommerfeld( beta, z, Z );
|
|---|
| 594 | // G4cout<<"fZomerfeld = "<<n<<G4endl;
|
|---|
| 595 | G4double am = CalculateAm( momentum, n, Z);
|
|---|
| 596 | // G4cout<<"cof Am = "<<am<<G4endl;
|
|---|
| 597 | G4double k = momentum/hbarc;
|
|---|
| 598 | // G4cout<<"k = "<<k*fermi<<" 1/fermi"<<G4endl;
|
|---|
| 599 | // G4cout<<"k*Bohr_radius = "<<k*Bohr_radius<<G4endl;
|
|---|
| 600 | G4double ch = n/k;
|
|---|
| 601 | G4double ch2 = ch*ch;
|
|---|
| 602 | am *= 2.;
|
|---|
| 603 | G4double xsc = ch2*twopi*(c1-c2);
|
|---|
| 604 | xsc /= (1 - c1 + am)*(1 - c2 + am);
|
|---|
| 605 |
|
|---|
| 606 | return xsc;
|
|---|
| 607 | }
|
|---|
| 608 |
|
|---|
| 609 | ///////////////////////////////////////////////////////////////////
|
|---|
| 610 | //
|
|---|
| 611 | // For the calculation of arg Gamma(z) one needs complex extension
|
|---|
| 612 | // of ln(Gamma(z))
|
|---|
| 613 |
|
|---|
| 614 | inline G4complex G4NuclNuclDiffuseElastic::GammaLogarithm(G4complex zz)
|
|---|
| 615 | {
|
|---|
| 616 | static G4double cof[6] = { 76.18009172947146, -86.50532032941677,
|
|---|
| 617 | 24.01409824083091, -1.231739572450155,
|
|---|
| 618 | 0.1208650973866179e-2, -0.5395239384953e-5 } ;
|
|---|
| 619 | register G4int j;
|
|---|
| 620 | G4complex z = zz - 1.0;
|
|---|
| 621 | G4complex tmp = z + 5.5;
|
|---|
| 622 | tmp -= (z + 0.5) * std::log(tmp);
|
|---|
| 623 | G4complex ser = G4complex(1.000000000190015,0.);
|
|---|
| 624 |
|
|---|
| 625 | for ( j = 0; j <= 5; j++ )
|
|---|
| 626 | {
|
|---|
| 627 | z += 1.0;
|
|---|
| 628 | ser += cof[j]/z;
|
|---|
| 629 | }
|
|---|
| 630 | return -tmp + std::log(2.5066282746310005*ser);
|
|---|
| 631 | }
|
|---|
| 632 |
|
|---|
| 633 | /////////////////////////////////////////////////////////////////
|
|---|
| 634 | //
|
|---|
| 635 | //
|
|---|
| 636 |
|
|---|
| 637 | inline G4double G4NuclNuclDiffuseElastic::GetErf(G4double x)
|
|---|
| 638 | {
|
|---|
| 639 | G4double t, z, tmp, result;
|
|---|
| 640 |
|
|---|
| 641 | z = std::fabs(x);
|
|---|
| 642 | t = 1.0/(1.0+0.5*z);
|
|---|
| 643 |
|
|---|
| 644 | tmp = t*exp(-z*z-1.26551223+t*(1.00002368+t*(0.37409196+t*(0.09678418+
|
|---|
| 645 | t*(-0.18628806+t*(0.27886807+t*(-1.13520398+t*(1.48851587+
|
|---|
| 646 | t*(-0.82215223+t*0.17087277)))))))));
|
|---|
| 647 |
|
|---|
| 648 | if( x >= 0.) result = 1. - tmp;
|
|---|
| 649 | else result = 1. + tmp;
|
|---|
| 650 |
|
|---|
| 651 | return result;
|
|---|
| 652 | }
|
|---|
| 653 |
|
|---|
| 654 | /////////////////////////////////////////////////////////////////
|
|---|
| 655 | //
|
|---|
| 656 | //
|
|---|
| 657 |
|
|---|
| 658 | inline G4complex G4NuclNuclDiffuseElastic::GetErfcComp(G4complex z, G4int nMax)
|
|---|
| 659 | {
|
|---|
| 660 | G4complex erfcz = 1. - GetErfComp( z, nMax);
|
|---|
| 661 | return erfcz;
|
|---|
| 662 | }
|
|---|
| 663 |
|
|---|
| 664 | /////////////////////////////////////////////////////////////////
|
|---|
| 665 | //
|
|---|
| 666 | //
|
|---|
| 667 |
|
|---|
| 668 | inline G4complex G4NuclNuclDiffuseElastic::GetErfcSer(G4complex z, G4int nMax)
|
|---|
| 669 | {
|
|---|
| 670 | G4complex erfcz = 1. - GetErfSer( z, nMax);
|
|---|
| 671 | return erfcz;
|
|---|
| 672 | }
|
|---|
| 673 |
|
|---|
| 674 | /////////////////////////////////////////////////////////////////
|
|---|
| 675 | //
|
|---|
| 676 | //
|
|---|
| 677 |
|
|---|
| 678 | inline G4complex G4NuclNuclDiffuseElastic::GetErfcInt(G4complex z) // , G4int nMax)
|
|---|
| 679 | {
|
|---|
| 680 | G4complex erfcz = 1. - GetErfInt( z); // , nMax);
|
|---|
| 681 | return erfcz;
|
|---|
| 682 | }
|
|---|
| 683 |
|
|---|
| 684 | /////////////////////////////////////////////////////////////////
|
|---|
| 685 | //
|
|---|
| 686 | //
|
|---|
| 687 |
|
|---|
| 688 | inline G4complex G4NuclNuclDiffuseElastic::TestErfcComp(G4complex z, G4int nMax)
|
|---|
| 689 | {
|
|---|
| 690 | G4complex miz = G4complex( z.imag(), -z.real() );
|
|---|
| 691 | G4complex erfcz = 1. - GetErfComp( miz, nMax);
|
|---|
| 692 | G4complex w = std::exp(-z*z)*erfcz;
|
|---|
| 693 | return w;
|
|---|
| 694 | }
|
|---|
| 695 |
|
|---|
| 696 | /////////////////////////////////////////////////////////////////
|
|---|
| 697 | //
|
|---|
| 698 | //
|
|---|
| 699 |
|
|---|
| 700 | inline G4complex G4NuclNuclDiffuseElastic::TestErfcSer(G4complex z, G4int nMax)
|
|---|
| 701 | {
|
|---|
| 702 | G4complex miz = G4complex( z.imag(), -z.real() );
|
|---|
| 703 | G4complex erfcz = 1. - GetErfSer( miz, nMax);
|
|---|
| 704 | G4complex w = std::exp(-z*z)*erfcz;
|
|---|
| 705 | return w;
|
|---|
| 706 | }
|
|---|
| 707 |
|
|---|
| 708 | /////////////////////////////////////////////////////////////////
|
|---|
| 709 | //
|
|---|
| 710 | //
|
|---|
| 711 |
|
|---|
| 712 | inline G4complex G4NuclNuclDiffuseElastic::TestErfcInt(G4complex z) // , G4int nMax)
|
|---|
| 713 | {
|
|---|
| 714 | G4complex miz = G4complex( z.imag(), -z.real() );
|
|---|
| 715 | G4complex erfcz = 1. - GetErfInt( miz); // , nMax);
|
|---|
| 716 | G4complex w = std::exp(-z*z)*erfcz;
|
|---|
| 717 | return w;
|
|---|
| 718 | }
|
|---|
| 719 |
|
|---|
| 720 | /////////////////////////////////////////////////////////////////
|
|---|
| 721 | //
|
|---|
| 722 | //
|
|---|
| 723 |
|
|---|
| 724 | inline G4complex G4NuclNuclDiffuseElastic::GetErfComp(G4complex z, G4int nMax)
|
|---|
| 725 | {
|
|---|
| 726 | G4int n;
|
|---|
| 727 | G4double n2, cofn, shny, chny, fn, gn;
|
|---|
| 728 |
|
|---|
| 729 | G4double x = z.real();
|
|---|
| 730 | G4double y = z.imag();
|
|---|
| 731 |
|
|---|
| 732 | G4double outRe = 0., outIm = 0.;
|
|---|
| 733 |
|
|---|
| 734 | G4double twox = 2.*x;
|
|---|
| 735 | G4double twoxy = twox*y;
|
|---|
| 736 | G4double twox2 = twox*twox;
|
|---|
| 737 |
|
|---|
| 738 | G4double cof1 = std::exp(-x*x)/pi;
|
|---|
| 739 |
|
|---|
| 740 | G4double cos2xy = std::cos(twoxy);
|
|---|
| 741 | G4double sin2xy = std::sin(twoxy);
|
|---|
| 742 |
|
|---|
| 743 | G4double twoxcos2xy = twox*cos2xy;
|
|---|
| 744 | G4double twoxsin2xy = twox*sin2xy;
|
|---|
| 745 |
|
|---|
| 746 | for( n = 1; n <= nMax; n++)
|
|---|
| 747 | {
|
|---|
| 748 | n2 = n*n;
|
|---|
| 749 |
|
|---|
| 750 | cofn = std::exp(-0.5*n2)/(n2+twox2); // /(n2+0.5*twox2);
|
|---|
| 751 |
|
|---|
| 752 | chny = std::cosh(n*y);
|
|---|
| 753 | shny = std::sinh(n*y);
|
|---|
| 754 |
|
|---|
| 755 | fn = twox - twoxcos2xy*chny + n*sin2xy*shny;
|
|---|
| 756 | gn = twoxsin2xy*chny + n*cos2xy*shny;
|
|---|
| 757 |
|
|---|
| 758 | fn *= cofn;
|
|---|
| 759 | gn *= cofn;
|
|---|
| 760 |
|
|---|
| 761 | outRe += fn;
|
|---|
| 762 | outIm += gn;
|
|---|
| 763 | }
|
|---|
| 764 | outRe *= 2*cof1;
|
|---|
| 765 | outIm *= 2*cof1;
|
|---|
| 766 |
|
|---|
| 767 | if(std::abs(x) < 0.0001)
|
|---|
| 768 | {
|
|---|
| 769 | outRe += GetErf(x);
|
|---|
| 770 | outIm += cof1*y;
|
|---|
| 771 | }
|
|---|
| 772 | else
|
|---|
| 773 | {
|
|---|
| 774 | outRe += GetErf(x) + cof1*(1-cos2xy)/twox;
|
|---|
| 775 | outIm += cof1*sin2xy/twox;
|
|---|
| 776 | }
|
|---|
| 777 | return G4complex(outRe, outIm);
|
|---|
| 778 | }
|
|---|
| 779 |
|
|---|
| 780 | /////////////////////////////////////////////////////////////////
|
|---|
| 781 | //
|
|---|
| 782 | //
|
|---|
| 783 |
|
|---|
| 784 | inline G4complex G4NuclNuclDiffuseElastic::GetErfSer(G4complex z, G4int nMax)
|
|---|
| 785 | {
|
|---|
| 786 | G4int n;
|
|---|
| 787 | G4double a =1., b = 1., tmp;
|
|---|
| 788 | G4complex sum = z, d = z;
|
|---|
| 789 |
|
|---|
| 790 | for( n = 1; n <= nMax; n++)
|
|---|
| 791 | {
|
|---|
| 792 | a *= 2.;
|
|---|
| 793 | b *= 2.*n +1.;
|
|---|
| 794 | d *= z*z;
|
|---|
| 795 |
|
|---|
| 796 | tmp = a/b;
|
|---|
| 797 |
|
|---|
| 798 | sum += tmp*d;
|
|---|
| 799 | }
|
|---|
| 800 | sum *= 2.*std::exp(-z*z)/std::sqrt(pi);
|
|---|
| 801 |
|
|---|
| 802 | return sum;
|
|---|
| 803 | }
|
|---|
| 804 |
|
|---|
| 805 | /////////////////////////////////////////////////////////////////////
|
|---|
| 806 |
|
|---|
| 807 | inline G4double G4NuclNuclDiffuseElastic::GetExpCos(G4double x)
|
|---|
| 808 | {
|
|---|
| 809 | G4double result;
|
|---|
| 810 |
|
|---|
| 811 | result = std::exp(x*x-fReZ*fReZ);
|
|---|
| 812 | result *= std::cos(2.*x*fReZ);
|
|---|
| 813 | return result;
|
|---|
| 814 | }
|
|---|
| 815 |
|
|---|
| 816 | /////////////////////////////////////////////////////////////////////
|
|---|
| 817 |
|
|---|
| 818 | inline G4double G4NuclNuclDiffuseElastic::GetExpSin(G4double x)
|
|---|
| 819 | {
|
|---|
| 820 | G4double result;
|
|---|
| 821 |
|
|---|
| 822 | result = std::exp(x*x-fReZ*fReZ);
|
|---|
| 823 | result *= std::sin(2.*x*fReZ);
|
|---|
| 824 | return result;
|
|---|
| 825 | }
|
|---|
| 826 |
|
|---|
| 827 |
|
|---|
| 828 |
|
|---|
| 829 | /////////////////////////////////////////////////////////////////
|
|---|
| 830 | //
|
|---|
| 831 | //
|
|---|
| 832 |
|
|---|
| 833 | inline G4complex G4NuclNuclDiffuseElastic::GetErfInt(G4complex z) // , G4int nMax)
|
|---|
| 834 | {
|
|---|
| 835 | G4double outRe, outIm;
|
|---|
| 836 |
|
|---|
| 837 | G4double x = z.real();
|
|---|
| 838 | G4double y = z.imag();
|
|---|
| 839 | fReZ = x;
|
|---|
| 840 |
|
|---|
| 841 | G4Integrator<G4NuclNuclDiffuseElastic,G4double(G4NuclNuclDiffuseElastic::*)(G4double)> integral;
|
|---|
| 842 |
|
|---|
| 843 | outRe = integral.Legendre96(this,&G4NuclNuclDiffuseElastic::GetExpSin, 0., y );
|
|---|
| 844 | outIm = integral.Legendre96(this,&G4NuclNuclDiffuseElastic::GetExpCos, 0., y );
|
|---|
| 845 |
|
|---|
| 846 | outRe *= 2./sqrt(pi);
|
|---|
| 847 | outIm *= 2./sqrt(pi);
|
|---|
| 848 |
|
|---|
| 849 | outRe += GetErf(x);
|
|---|
| 850 |
|
|---|
| 851 | return G4complex(outRe, outIm);
|
|---|
| 852 | }
|
|---|
| 853 |
|
|---|
| 854 |
|
|---|
| 855 | /////////////////////////////////////////////////////////////////
|
|---|
| 856 | //
|
|---|
| 857 | //
|
|---|
| 858 |
|
|---|
| 859 | inline G4complex G4NuclNuclDiffuseElastic::CoulombAmplitude(G4double theta)
|
|---|
| 860 | {
|
|---|
| 861 | G4complex ca;
|
|---|
| 862 |
|
|---|
| 863 | G4double sinHalfTheta = std::sin(0.5*theta);
|
|---|
| 864 | G4double sinHalfTheta2 = sinHalfTheta*sinHalfTheta;
|
|---|
| 865 | sinHalfTheta2 += fAm;
|
|---|
| 866 | G4double order = 2.*fCoulombPhase0 - fZommerfeld*std::log(sinHalfTheta2);
|
|---|
| 867 | G4complex z = G4complex(0., order);
|
|---|
| 868 | ca = std::exp(z);
|
|---|
| 869 | ca *= -fZommerfeld/(2.*fWaveVector*sinHalfTheta2);
|
|---|
| 870 |
|
|---|
| 871 | return ca;
|
|---|
| 872 | }
|
|---|
| 873 |
|
|---|
| 874 | /////////////////////////////////////////////////////////////////
|
|---|
| 875 | //
|
|---|
| 876 | //
|
|---|
| 877 |
|
|---|
| 878 |
|
|---|
| 879 | inline void G4NuclNuclDiffuseElastic::CalculateCoulombPhaseZero()
|
|---|
| 880 | {
|
|---|
| 881 | G4complex z = G4complex(1,fZommerfeld);
|
|---|
| 882 | G4complex gammalog = GammaLogarithm(z);
|
|---|
| 883 | fCoulombPhase0 = gammalog.imag();
|
|---|
| 884 | }
|
|---|
| 885 |
|
|---|
| 886 |
|
|---|
| 887 | /////////////////////////////////////////////////////////////////
|
|---|
| 888 | //
|
|---|
| 889 | //
|
|---|
| 890 |
|
|---|
| 891 |
|
|---|
| 892 | inline void G4NuclNuclDiffuseElastic::CalculateRutherfordAnglePar()
|
|---|
| 893 | {
|
|---|
| 894 | fHalfRutThetaTg = fZommerfeld/(fWaveVector*fNuclearRadius);
|
|---|
| 895 | fRutherfordTheta = 2.*std::atan(fHalfRutThetaTg);
|
|---|
| 896 | G4cout<<"fRutherfordTheta = "<<fRutherfordTheta/degree<<" degree"<<G4endl;
|
|---|
| 897 |
|
|---|
| 898 | }
|
|---|
| 899 |
|
|---|
| 900 | /////////////////////////////////////////////////////////////////
|
|---|
| 901 | //
|
|---|
| 902 | //
|
|---|
| 903 |
|
|---|
| 904 | inline G4double G4NuclNuclDiffuseElastic::ProfileNear(G4double theta)
|
|---|
| 905 | {
|
|---|
| 906 | G4double dTheta = fRutherfordTheta - theta;
|
|---|
| 907 | G4double result = 0., argument = 0.;
|
|---|
| 908 |
|
|---|
| 909 | if(std::abs(dTheta) < 0.001) result = fProfileAlpha*fProfileDelta;
|
|---|
| 910 | else
|
|---|
| 911 | {
|
|---|
| 912 | argument = fProfileDelta*dTheta;
|
|---|
| 913 | result = pi*argument*std::exp(fProfileAlpha*argument);
|
|---|
| 914 | result /= std::sinh(pi*argument);
|
|---|
| 915 | result -= 1.;
|
|---|
| 916 | result /= dTheta;
|
|---|
| 917 | }
|
|---|
| 918 | return result;
|
|---|
| 919 | }
|
|---|
| 920 |
|
|---|
| 921 | /////////////////////////////////////////////////////////////////
|
|---|
| 922 | //
|
|---|
| 923 | //
|
|---|
| 924 |
|
|---|
| 925 | inline G4double G4NuclNuclDiffuseElastic::ProfileFar(G4double theta)
|
|---|
| 926 | {
|
|---|
| 927 | G4double dTheta = fRutherfordTheta + theta;
|
|---|
| 928 | G4double argument = fProfileDelta*dTheta;
|
|---|
| 929 |
|
|---|
| 930 | G4double result = pi*argument*std::exp(fProfileAlpha*argument);
|
|---|
| 931 | result /= std::sinh(pi*argument);
|
|---|
| 932 | result /= dTheta;
|
|---|
| 933 |
|
|---|
| 934 | return result;
|
|---|
| 935 | }
|
|---|
| 936 |
|
|---|
| 937 | /////////////////////////////////////////////////////////////////
|
|---|
| 938 | //
|
|---|
| 939 | //
|
|---|
| 940 |
|
|---|
| 941 | inline G4complex G4NuclNuclDiffuseElastic::PhaseNear(G4double theta)
|
|---|
| 942 | {
|
|---|
| 943 | G4double twosigma = 2.*fCoulombPhase0;
|
|---|
| 944 | twosigma -= fZommerfeld*std::log(fHalfRutThetaTg/(1.+fHalfRutThetaTg*fHalfRutThetaTg));
|
|---|
| 945 | twosigma += fRutherfordTheta*fZommerfeld/fHalfRutThetaTg - halfpi;
|
|---|
| 946 | twosigma -= fProfileLambda*theta - 0.25*pi;
|
|---|
| 947 |
|
|---|
| 948 | G4complex z = G4complex(0., twosigma);
|
|---|
| 949 |
|
|---|
| 950 | return std::exp(z);
|
|---|
| 951 | }
|
|---|
| 952 |
|
|---|
| 953 | /////////////////////////////////////////////////////////////////
|
|---|
| 954 | //
|
|---|
| 955 | //
|
|---|
| 956 |
|
|---|
| 957 | inline G4complex G4NuclNuclDiffuseElastic::PhaseFar(G4double theta)
|
|---|
| 958 | {
|
|---|
| 959 | G4double twosigma = 2.*fCoulombPhase0;
|
|---|
| 960 | twosigma -= fZommerfeld*std::log(fHalfRutThetaTg/(1.+fHalfRutThetaTg*fHalfRutThetaTg));
|
|---|
| 961 | twosigma += fRutherfordTheta*fZommerfeld/fHalfRutThetaTg - halfpi;
|
|---|
| 962 | twosigma += fProfileLambda*theta - 0.25*pi;
|
|---|
| 963 |
|
|---|
| 964 | G4complex z = G4complex(0., twosigma);
|
|---|
| 965 |
|
|---|
| 966 | return std::exp(z);
|
|---|
| 967 | }
|
|---|
| 968 |
|
|---|
| 969 | /////////////////////////////////////////////////////////////////
|
|---|
| 970 | //
|
|---|
| 971 | //
|
|---|
| 972 |
|
|---|
| 973 |
|
|---|
| 974 | inline G4complex G4NuclNuclDiffuseElastic::GammaLess(G4double theta)
|
|---|
| 975 | {
|
|---|
| 976 | G4double sinThetaR = 2.*fHalfRutThetaTg/(1. + fHalfRutThetaTg*fHalfRutThetaTg);
|
|---|
| 977 | G4double cosHalfThetaR2 = 1./(1. + fHalfRutThetaTg*fHalfRutThetaTg);
|
|---|
| 978 |
|
|---|
| 979 | G4double u = std::sqrt(0.5*fProfileLambda/sinThetaR);
|
|---|
| 980 | G4double kappa = u/std::sqrt(pi);
|
|---|
| 981 | G4double dTheta = theta - fRutherfordTheta;
|
|---|
| 982 | u *= dTheta;
|
|---|
| 983 | G4double u2 = u*u;
|
|---|
| 984 | G4double u2m2p3 = u2*2./3.;
|
|---|
| 985 |
|
|---|
| 986 | G4complex im = G4complex(0.,1.);
|
|---|
| 987 | G4complex order = G4complex(u,u);
|
|---|
| 988 | order /= std::sqrt(2.);
|
|---|
| 989 | G4complex gamma = pi*kappa*GetErfcInt(-order)*std::exp(im*(u*u+0.25*pi));
|
|---|
| 990 | G4complex a0 = 0.5*(1. + 4.*(1.+im*u2)*cosHalfThetaR2/3.)/sinThetaR;
|
|---|
| 991 | G4complex a1 = 0.5*(1. + 2.*(1.+im*u2m2p3)*cosHalfThetaR2)/sinThetaR;
|
|---|
| 992 | G4complex out = gamma*(1. - a1*dTheta) - a0;
|
|---|
| 993 | return out;
|
|---|
| 994 | }
|
|---|
| 995 |
|
|---|
| 996 | /////////////////////////////////////////////////////////////////
|
|---|
| 997 | //
|
|---|
| 998 | //
|
|---|
| 999 |
|
|---|
| 1000 | inline G4complex G4NuclNuclDiffuseElastic::GammaMore(G4double theta)
|
|---|
| 1001 | {
|
|---|
| 1002 | G4double sinThetaR = 2.*fHalfRutThetaTg/(1. + fHalfRutThetaTg*fHalfRutThetaTg);
|
|---|
| 1003 | G4double cosHalfThetaR2 = 1./(1. + fHalfRutThetaTg*fHalfRutThetaTg);
|
|---|
| 1004 |
|
|---|
| 1005 | G4double u = std::sqrt(0.5*fProfileLambda/sinThetaR);
|
|---|
| 1006 | G4double kappa = u/std::sqrt(pi);
|
|---|
| 1007 | G4double dTheta = theta - fRutherfordTheta;
|
|---|
| 1008 | u *= dTheta;
|
|---|
| 1009 | G4double u2 = u*u;
|
|---|
| 1010 | G4double u2m2p3 = u2*2./3.;
|
|---|
| 1011 |
|
|---|
| 1012 | G4complex im = G4complex(0.,1.);
|
|---|
| 1013 | G4complex order = G4complex(u,u);
|
|---|
| 1014 | order /= std::sqrt(2.);
|
|---|
| 1015 | G4complex gamma = pi*kappa*GetErfcInt(order)*std::exp(im*(u*u+0.25*pi));
|
|---|
| 1016 | G4complex a0 = 0.5*(1. + 3.*(1.+im*u2)*cosHalfThetaR2/3.)/sinThetaR;
|
|---|
| 1017 | G4complex a1 = 0.5*(1. + 2.*(1.+im*u2m2p3)*cosHalfThetaR2)/sinThetaR;
|
|---|
| 1018 | G4complex out = -gamma*(1. - a1*dTheta) - a0;
|
|---|
| 1019 | return out;
|
|---|
| 1020 | }
|
|---|
| 1021 |
|
|---|
| 1022 | /////////////////////////////////////////////////////////////////
|
|---|
| 1023 | //
|
|---|
| 1024 | //
|
|---|
| 1025 |
|
|---|
| 1026 | inline G4complex G4NuclNuclDiffuseElastic::AmplitudeNear(G4double theta)
|
|---|
| 1027 | {
|
|---|
| 1028 | G4double kappa = std::sqrt(0.5*fProfileLambda/std::sin(theta)/pi);
|
|---|
| 1029 | G4complex out = G4complex(kappa/fWaveVector,0.);
|
|---|
| 1030 | out *= PhaseNear(theta);
|
|---|
| 1031 |
|
|---|
| 1032 | if(theta <= fRutherfordTheta)
|
|---|
| 1033 | {
|
|---|
| 1034 | out *= GammaLess(theta) + ProfileNear(theta);
|
|---|
| 1035 | out += CoulombAmplitude(theta);
|
|---|
| 1036 | }
|
|---|
| 1037 | else
|
|---|
| 1038 | {
|
|---|
| 1039 | out *= GammaMore(theta) + ProfileNear(theta);
|
|---|
| 1040 | }
|
|---|
| 1041 | return out;
|
|---|
| 1042 | }
|
|---|
| 1043 |
|
|---|
| 1044 | /////////////////////////////////////////////////////////////////
|
|---|
| 1045 | //
|
|---|
| 1046 | //
|
|---|
| 1047 |
|
|---|
| 1048 | inline G4complex G4NuclNuclDiffuseElastic::AmplitudeFar(G4double theta)
|
|---|
| 1049 | {
|
|---|
| 1050 | G4double kappa = std::sqrt(0.5*fProfileLambda/std::sin(theta)/pi);
|
|---|
| 1051 | G4complex out = G4complex(kappa/fWaveVector,0.);
|
|---|
| 1052 | out *= ProfileFar(theta)*PhaseFar(theta);
|
|---|
| 1053 | return out;
|
|---|
| 1054 | }
|
|---|
| 1055 |
|
|---|
| 1056 |
|
|---|
| 1057 | /////////////////////////////////////////////////////////////////
|
|---|
| 1058 | //
|
|---|
| 1059 | //
|
|---|
| 1060 |
|
|---|
| 1061 | inline G4complex G4NuclNuclDiffuseElastic::Amplitude(G4double theta)
|
|---|
| 1062 | {
|
|---|
| 1063 |
|
|---|
| 1064 | G4complex out = AmplitudeNear(theta) + AmplitudeFar(theta);
|
|---|
| 1065 | return out;
|
|---|
| 1066 | }
|
|---|
| 1067 |
|
|---|
| 1068 | /////////////////////////////////////////////////////////////////
|
|---|
| 1069 | //
|
|---|
| 1070 | //
|
|---|
| 1071 |
|
|---|
| 1072 | inline G4double G4NuclNuclDiffuseElastic::AmplitudeMod2(G4double theta)
|
|---|
| 1073 | {
|
|---|
| 1074 | G4complex out = Amplitude(theta);
|
|---|
| 1075 | G4double mod2 = out.real()*out.real() + out.imag()*out.imag();
|
|---|
| 1076 | return mod2;
|
|---|
| 1077 | }
|
|---|
| 1078 |
|
|---|
| 1079 |
|
|---|
| 1080 | ///////////////////////////////////////////////////////////////////////////////
|
|---|
| 1081 | //
|
|---|
| 1082 | // Test for given particle and element table of momentum, angle probability.
|
|---|
| 1083 | // For the moment in lab system.
|
|---|
| 1084 |
|
|---|
| 1085 | inline void G4NuclNuclDiffuseElastic::InitParameters(const G4ParticleDefinition* theParticle,
|
|---|
| 1086 | G4double partMom, G4double Z, G4double A)
|
|---|
| 1087 | {
|
|---|
| 1088 | fAtomicNumber = Z; // atomic number
|
|---|
| 1089 | fAtomicWeight = A; // number of nucleons
|
|---|
| 1090 |
|
|---|
| 1091 | fNuclearRadius2 = CalculateNuclearRad(fAtomicWeight);
|
|---|
| 1092 | G4double A1 = G4double( theParticle->GetBaryonNumber() );
|
|---|
| 1093 | fNuclearRadius1 = CalculateNuclearRad(A1);
|
|---|
| 1094 | // fNuclearRadius = std::sqrt(fNuclearRadius1*fNuclearRadius1+fNuclearRadius2*fNuclearRadius2);
|
|---|
| 1095 | fNuclearRadius = fNuclearRadius1 + fNuclearRadius2;
|
|---|
| 1096 |
|
|---|
| 1097 | G4double a = 0.;
|
|---|
| 1098 | G4double z = theParticle->GetPDGCharge();
|
|---|
| 1099 | G4double m1 = theParticle->GetPDGMass();
|
|---|
| 1100 |
|
|---|
| 1101 | fWaveVector = partMom/hbarc;
|
|---|
| 1102 |
|
|---|
| 1103 | G4double lambda = fWaveVector*fNuclearRadius;
|
|---|
| 1104 |
|
|---|
| 1105 | if( z )
|
|---|
| 1106 | {
|
|---|
| 1107 | a = partMom/m1; // beta*gamma for m1
|
|---|
| 1108 | fBeta = a/std::sqrt(1+a*a);
|
|---|
| 1109 | fZommerfeld = CalculateZommerfeld( fBeta, z, fAtomicNumber);
|
|---|
| 1110 | fAm = CalculateAm( partMom, fZommerfeld, fAtomicNumber);
|
|---|
| 1111 | }
|
|---|
| 1112 | fProfileLambda = lambda*std::sqrt(1.-2*fZommerfeld/lambda);
|
|---|
| 1113 | G4cout<<"fProfileLambda = "<<fProfileLambda<<G4endl;
|
|---|
| 1114 | fProfileDelta = 0.1*fProfileLambda;
|
|---|
| 1115 | fProfileAlpha = 0.05*fProfileLambda;
|
|---|
| 1116 |
|
|---|
| 1117 | CalculateCoulombPhaseZero();
|
|---|
| 1118 | CalculateRutherfordAnglePar();
|
|---|
| 1119 |
|
|---|
| 1120 | return;
|
|---|
| 1121 | }
|
|---|
| 1122 |
|
|---|
| 1123 |
|
|---|
| 1124 |
|
|---|
| 1125 |
|
|---|
| 1126 |
|
|---|
| 1127 | #endif
|
|---|