Files
geant4/source/processes/hadronic/models/binary_cascade/include/G4RKFieldIntegrator.hh
T
2019-06-28 11:59:04 +02:00

89 lines
4.1 KiB
C++

//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
// * LICENSE and available at http://cern.ch/geant4/license . These *
// * include a list of copyright holders. *
// * *
// * Neither the authors of this software system, nor their employing *
// * institutes,nor the agencies providing financial support for this *
// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
// * any work based on the software) you agree to acknowledge its *
// * use in resulting scientific publications, and indicate your *
// * acceptance of all terms of the Geant4 Software license. *
// ********************************************************************
//
#ifndef G4RKFieldIntegrator_h
#define G4RKFieldIntegrator_h 1
#include "G4FieldPropagation.hh"
class G4RKFieldIntegrator : public G4FieldPropagation
{
public:
G4RKFieldIntegrator() {}
G4RKFieldIntegrator(const G4RKFieldIntegrator &):G4FieldPropagation() {}
~G4RKFieldIntegrator() {}
//Operators
const G4RKFieldIntegrator & operator=(const G4RKFieldIntegrator &) {return *this;}
G4bool operator==(const G4RKFieldIntegrator &) const {return 1;}
G4bool operator!=(const G4RKFieldIntegrator &) const {return 1;}
// only theActive are propagated, nothing else
// only theSpectators define the field, nothing else
void Transport(G4KineticTrackVector &theActive, const G4KineticTrackVector &theSpectators, G4double theTimeStep);
G4double GetExcitationEnergy(G4int nHitNucleons, const G4KineticTrackVector &theParticles);
// methods for calculating potentials for different types of particles
void Init(G4int z, G4int a) {theZ = z; theA = a;} // prepare potentials' functions
// aPosition is relative to the nucleus center
G4double GetNeutronPotential(G4double radius);
G4double GetNeutronPotential(G4ThreeVector &aPosition) {return GetNeutronPotential(aPosition.mag());}
G4double GetProtonPotential(G4double radius);
G4double GetProtonPotential(G4ThreeVector &aPosition) {return GetProtonPotential(aPosition.mag());}
G4double GetAntiprotonPotential(G4double radius);
G4double GetAntiprotonPotential(G4ThreeVector &aPosition) {return GetAntiprotonPotential(aPosition.mag());};
G4double GetKaonPotential(G4double radius);
G4double GetKaonPotential(G4ThreeVector &aPosition) {return GetKaonPotential(aPosition.mag());}
G4double GetPionPotential(G4double radius);
G4double GetPionPotential(G4ThreeVector &aPosition) {return GetPionPotential(aPosition.mag());}
private:
void Integrate(const G4KineticTrackVector & theActive, G4double theTimeStep);
G4double CalculateTotalEnergy(const G4KineticTrackVector& Barions);
G4double Erf(G4double X);
// parameters to calculate potentials
G4int theA;
G4int theZ;
// Vc(A, Z) = 1.44 * Z /(r0*(1 + std::pow(A, 1/3)))
// = colomb * Z / (1 + std::pow(A, 1/3))
static const G4double coulomb; // coulomb barier constant
static const G4double a_kaon; // kaon's potential constant
static const G4double a_pion; // pion's potential constant
static const G4double a_antiproton; // antiproton's potential constant
};
#endif // G4RKFieldIntegrator_h