542 lines
16 KiB
C++
542 lines
16 KiB
C++
//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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//
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// $Id: G4DiffuseElastic.hh,v 1.13 2007/11/06 17:01:20 grichine Exp $
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// GEANT4 tag $Name: geant4-09-01 $
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//
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//
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// G4 Model: optical elastic scattering with 4-momentum balance
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//
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// Class Description
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// Final state production model for hadron nuclear elastic scattering;
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// Class Description - End
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//
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//
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// 24.05.07 V. Grichine first implementation for hadron (no Coulomb) elastic scattering
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// 04.09.07 V. Grichine implementation for Coulomb elastic scattering
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#ifndef G4DiffuseElastic_h
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#define G4DiffuseElastic_h 1
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#include "globals.hh"
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#include "G4HadronicInteraction.hh"
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#include "G4HadProjectile.hh"
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#include "G4Nucleus.hh"
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using namespace std;
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class G4ParticleDefinition;
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class G4PhysicsTable;
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class G4PhysicsLogVector;
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class G4DiffuseElastic : public G4HadronicInteraction
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{
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public:
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G4DiffuseElastic();
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G4DiffuseElastic(const G4ParticleDefinition* aParticle);
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virtual ~G4DiffuseElastic();
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void Initialise();
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void InitialiseOnFly(G4double Z, G4double A);
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void BuildAngleTable();
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G4HadFinalState * ApplyYourself(const G4HadProjectile & aTrack,
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G4Nucleus & targetNucleus);
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void SetPlabLowLimit(G4double value);
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void SetHEModelLowLimit(G4double value);
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void SetQModelLowLimit(G4double value);
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void SetLowestEnergyLimit(G4double value);
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void SetRecoilKinEnergyLimit(G4double value);
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G4double SampleT(const G4ParticleDefinition* aParticle,
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G4double p, G4double A);
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G4double SampleTableT(const G4ParticleDefinition* aParticle,
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G4double p, G4double Z, G4double A);
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G4double SampleThetaCMS(const G4ParticleDefinition* aParticle, G4double p, G4double A);
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G4double SampleTableThetaCMS(const G4ParticleDefinition* aParticle, G4double p,
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G4double Z, G4double A);
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G4double GetScatteringAngle(G4int iMomentum, G4int iAngle, G4double position);
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G4double SampleThetaLab(const G4HadProjectile* aParticle,
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G4double tmass, G4double A);
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G4double GetDiffuseElasticXsc( const G4ParticleDefinition* particle,
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G4double theta,
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G4double momentum,
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G4double A );
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G4double GetInvElasticXsc( const G4ParticleDefinition* particle,
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G4double theta,
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G4double momentum,
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G4double A, G4double Z );
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G4double GetDiffuseElasticSumXsc( const G4ParticleDefinition* particle,
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G4double theta,
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G4double momentum,
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G4double A, G4double Z );
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G4double GetInvElasticSumXsc( const G4ParticleDefinition* particle,
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G4double tMand,
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G4double momentum,
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G4double A, G4double Z );
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G4double IntegralElasticProb( const G4ParticleDefinition* particle,
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G4double theta,
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G4double momentum,
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G4double A );
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G4double GetCoulombElasticXsc( const G4ParticleDefinition* particle,
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G4double theta,
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G4double momentum,
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G4double Z );
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G4double GetInvCoulombElasticXsc( const G4ParticleDefinition* particle,
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G4double tMand,
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G4double momentum,
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G4double A, G4double Z );
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G4double GetCoulombTotalXsc( const G4ParticleDefinition* particle,
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G4double momentum, G4double Z );
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G4double GetCoulombIntegralXsc( const G4ParticleDefinition* particle,
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G4double momentum, G4double Z,
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G4double theta1, G4double theta2 );
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G4double CalculateParticleBeta( const G4ParticleDefinition* particle,
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G4double momentum );
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G4double CalculateZommerfeld( G4double beta, G4double Z1, G4double Z2 );
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G4double CalculateAm( G4double momentum, G4double n, G4double Z);
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G4double CalculateNuclearRad( G4double A);
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G4double ThetaCMStoThetaLab(const G4DynamicParticle* aParticle,
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G4double tmass, G4double thetaCMS);
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G4double ThetaLabToThetaCMS(const G4DynamicParticle* aParticle,
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G4double tmass, G4double thetaLab);
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G4double BesselJzero(G4double z);
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G4double BesselJone(G4double z);
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G4double DampFactor(G4double z);
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G4double BesselOneByArg(G4double z);
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G4double GetDiffElasticProb(G4double theta);
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G4double GetDiffElasticSumProb(G4double theta);
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G4double GetIntegrandFunction(G4double theta);
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G4double GetNuclearRadius(){return fNuclearRadius;};
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private:
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G4ParticleDefinition* theProton;
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G4ParticleDefinition* theNeutron;
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G4ParticleDefinition* theDeuteron;
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G4ParticleDefinition* theAlpha;
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const G4ParticleDefinition* thePionPlus;
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const G4ParticleDefinition* thePionMinus;
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G4double lowEnergyRecoilLimit;
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G4double lowEnergyLimitHE;
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G4double lowEnergyLimitQ;
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G4double lowestEnergyLimit;
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G4double plabLowLimit;
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G4int fEnergyBin;
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G4int fAngleBin;
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G4PhysicsLogVector* fEnergyVector;
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G4PhysicsTable* fAngleTable;
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std::vector<G4PhysicsTable*> fAngleBank;
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std::vector<G4double> fElementNumberVector;
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std::vector<G4String> fElementNameVector;
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const G4ParticleDefinition* fParticle;
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G4double fWaveVector;
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G4double fAtomicWeight;
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G4double fAtomicNumber;
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G4double fNuclearRadius;
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G4double fBeta;
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G4double fZommerfeld;
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G4double fAm;
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G4bool fAddCoulomb;
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};
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inline void G4DiffuseElastic::SetRecoilKinEnergyLimit(G4double value)
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{
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lowEnergyRecoilLimit = value;
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}
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inline void G4DiffuseElastic::SetPlabLowLimit(G4double value)
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{
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plabLowLimit = value;
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}
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inline void G4DiffuseElastic::SetHEModelLowLimit(G4double value)
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{
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lowEnergyLimitHE = value;
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}
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inline void G4DiffuseElastic::SetQModelLowLimit(G4double value)
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{
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lowEnergyLimitQ = value;
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}
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inline void G4DiffuseElastic::SetLowestEnergyLimit(G4double value)
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{
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lowestEnergyLimit = value;
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}
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/////////////////////////////////////////////////////////////
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//
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// Bessel J0 function based on rational approximation from
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// J.F. Hart, Computer Approximations, New York, Willey 1968, p. 141
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inline G4double G4DiffuseElastic::BesselJzero(G4double value)
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{
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G4double modvalue, value2, fact1, fact2, arg, shift, bessel;
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modvalue = fabs(value);
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if ( value < 8.0 && value > -8.0 )
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{
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value2 = value*value;
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fact1 = 57568490574.0 + value2*(-13362590354.0
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+ value2*( 651619640.7
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+ value2*(-11214424.18
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+ value2*( 77392.33017
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+ value2*(-184.9052456 ) ) ) ) );
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fact2 = 57568490411.0 + value2*( 1029532985.0
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+ value2*( 9494680.718
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+ value2*(59272.64853
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+ value2*(267.8532712
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+ value2*1.0 ) ) ) );
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bessel = fact1/fact2;
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}
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else
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{
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arg = 8.0/modvalue;
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value2 = arg*arg;
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shift = modvalue-0.785398164;
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fact1 = 1.0 + value2*(-0.1098628627e-2
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+ value2*(0.2734510407e-4
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+ value2*(-0.2073370639e-5
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+ value2*0.2093887211e-6 ) ) );
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fact2 = -0.1562499995e-1 + value2*(0.1430488765e-3
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+ value2*(-0.6911147651e-5
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+ value2*(0.7621095161e-6
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- value2*0.934945152e-7 ) ) );
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bessel = sqrt(0.636619772/modvalue)*(cos(shift)*fact1 - arg*sin(shift)*fact2 );
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}
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return bessel;
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}
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/////////////////////////////////////////////////////////////
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//
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// Bessel J1 function based on rational approximation from
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// J.F. Hart, Computer Approximations, New York, Willey 1968, p. 141
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inline G4double G4DiffuseElastic::BesselJone(G4double value)
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{
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G4double modvalue, value2, fact1, fact2, arg, shift, bessel;
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modvalue = fabs(value);
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if ( modvalue < 8.0 )
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{
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value2 = value*value;
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fact1 = value*(72362614232.0 + value2*(-7895059235.0
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+ value2*( 242396853.1
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+ value2*(-2972611.439
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+ value2*( 15704.48260
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+ value2*(-30.16036606 ) ) ) ) ) );
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fact2 = 144725228442.0 + value2*(2300535178.0
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+ value2*(18583304.74
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+ value2*(99447.43394
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+ value2*(376.9991397
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+ value2*1.0 ) ) ) );
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bessel = fact1/fact2;
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}
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else
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{
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arg = 8.0/modvalue;
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value2 = arg*arg;
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shift = modvalue - 2.356194491;
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fact1 = 1.0 + value2*( 0.183105e-2
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+ value2*(-0.3516396496e-4
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+ value2*(0.2457520174e-5
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+ value2*(-0.240337019e-6 ) ) ) );
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fact2 = 0.04687499995 + value2*(-0.2002690873e-3
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+ value2*( 0.8449199096e-5
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+ value2*(-0.88228987e-6
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+ value2*0.105787412e-6 ) ) );
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bessel = sqrt( 0.636619772/modvalue)*(cos(shift)*fact1 - arg*sin(shift)*fact2);
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if (value < 0.0) bessel = -bessel;
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}
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return bessel;
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}
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////////////////////////////////////////////////////////////////////
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//
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// damp factor in diffraction x/sh(x), x was already *pi
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inline G4double G4DiffuseElastic::DampFactor(G4double x)
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{
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G4double df;
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G4double f2 = 2., f3 = 6., f4 = 24.; // first factorials
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// x *= pi;
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if( std::fabs(x) < 0.01 )
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{
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df = 1./(1. + x/f2 + x*x/f3 + x*x*x/f4);
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}
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else
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{
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df = x/std::sinh(x);
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}
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return df;
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}
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////////////////////////////////////////////////////////////////////
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//
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// return J1(x)/x with special case for small x
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inline G4double G4DiffuseElastic::BesselOneByArg(G4double x)
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{
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G4double x2, result;
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if( std::fabs(x) < 0.01 )
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{
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x *= 0.5;
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x2 = x*x;
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result = 2. - x2 + x2*x2/6.;
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}
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else
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{
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result = BesselJone(x)/x;
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}
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return result;
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}
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////////////////////////////////////////////////////////////////////
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//
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// return particle beta
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inline G4double G4DiffuseElastic::CalculateParticleBeta( const G4ParticleDefinition* particle,
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G4double momentum )
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{
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G4double mass = particle->GetPDGMass();
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G4double a = momentum/mass;
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fBeta = a/std::sqrt(1+a*a);
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return fBeta;
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}
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////////////////////////////////////////////////////////////////////
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//
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// return Zommerfeld parameter for Coulomb scattering
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inline G4double G4DiffuseElastic::CalculateZommerfeld( G4double beta, G4double Z1, G4double Z2 )
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{
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fZommerfeld = fine_structure_const*Z1*Z2/beta;
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return fZommerfeld;
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}
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////////////////////////////////////////////////////////////////////
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//
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// return Wentzel correction for Coulomb scattering
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inline G4double G4DiffuseElastic::CalculateAm( G4double momentum, G4double n, G4double Z)
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{
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G4double k = momentum/hbarc;
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G4double ch = 1.13 + 3.76*n*n;
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G4double zn = 1.77*k*std::pow(Z,-1./3.)*Bohr_radius;
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G4double zn2 = zn*zn;
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fAm = ch/zn2;
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return fAm;
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}
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////////////////////////////////////////////////////////////////////
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//
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// calculate nuclear radius for different atomic weights using different approximations
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inline G4double G4DiffuseElastic::CalculateNuclearRad( G4double A)
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{
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G4double r0;
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if(A < 50.)
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{
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if(A > 10.) r0 = 1.16*( 1 - std::pow(A, -2./3.) )*fermi; // 1.08*fermi;
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else r0 = 1.1*fermi;
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fNuclearRadius = r0*std::pow(A, 1./3.);
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}
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else
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{
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r0 = 1.7*fermi;
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fNuclearRadius = r0*std::pow(A, 0.27);
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}
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return fNuclearRadius;
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}
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////////////////////////////////////////////////////////////////////
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//
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// return Coulomb scattering differential xsc with Wentzel correction
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inline G4double G4DiffuseElastic::GetCoulombElasticXsc( const G4ParticleDefinition* particle,
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G4double theta,
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G4double momentum,
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G4double Z )
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{
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G4double sinHalfTheta = std::sin(0.5*theta);
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G4double sinHalfTheta2 = sinHalfTheta*sinHalfTheta;
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G4double beta = CalculateParticleBeta( particle, momentum);
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G4double z = particle->GetPDGCharge();
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G4double n = CalculateZommerfeld( beta, z, Z );
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G4double am = CalculateAm( momentum, n, Z);
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G4double k = momentum/hbarc;
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G4double ch = 0.5*n/k;
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G4double ch2 = ch*ch;
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G4double xsc = ch2/(sinHalfTheta2+am)/(sinHalfTheta2+am);
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return xsc;
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}
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////////////////////////////////////////////////////////////////////
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//
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// return Coulomb scattering total xsc with Wentzel correction
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inline G4double G4DiffuseElastic::GetCoulombTotalXsc( const G4ParticleDefinition* particle,
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G4double momentum, G4double Z )
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{
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G4double beta = CalculateParticleBeta( particle, momentum);
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G4cout<<"beta = "<<beta<<G4endl;
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G4double z = particle->GetPDGCharge();
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G4double n = CalculateZommerfeld( beta, z, Z );
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G4cout<<"fZomerfeld = "<<n<<G4endl;
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G4double am = CalculateAm( momentum, n, Z);
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G4cout<<"cof Am = "<<am<<G4endl;
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G4double k = momentum/hbarc;
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G4cout<<"k = "<<k*fermi<<" 1/fermi"<<G4endl;
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G4cout<<"k*Bohr_radius = "<<k*Bohr_radius<<G4endl;
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G4double ch = n/k;
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G4double ch2 = ch*ch;
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G4double xsc = ch2*pi/(am +am*am);
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return xsc;
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}
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////////////////////////////////////////////////////////////////////
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//
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// return Coulomb scattering xsc with Wentzel correction integrated between
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// theta1 and < theta2
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inline G4double G4DiffuseElastic::GetCoulombIntegralXsc( const G4ParticleDefinition* particle,
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G4double momentum, G4double Z,
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G4double theta1, G4double theta2 )
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{
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G4double c1 = std::cos(theta1);
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G4cout<<"c1 = "<<c1<<G4endl;
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G4double c2 = std::cos(theta2);
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G4cout<<"c2 = "<<c2<<G4endl;
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G4double beta = CalculateParticleBeta( particle, momentum);
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// G4cout<<"beta = "<<beta<<G4endl;
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G4double z = particle->GetPDGCharge();
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G4double n = CalculateZommerfeld( beta, z, Z );
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// G4cout<<"fZomerfeld = "<<n<<G4endl;
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G4double am = CalculateAm( momentum, n, Z);
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// G4cout<<"cof Am = "<<am<<G4endl;
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G4double k = momentum/hbarc;
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// G4cout<<"k = "<<k*fermi<<" 1/fermi"<<G4endl;
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// G4cout<<"k*Bohr_radius = "<<k*Bohr_radius<<G4endl;
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G4double ch = n/k;
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G4double ch2 = ch*ch;
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am *= 2.;
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G4double xsc = ch2*twopi*(c1-c2);
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xsc /= (1 - c1 + am)*(1 - c2 + am);
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return xsc;
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}
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#endif
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