// // ******************************************************************** // * 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;} int operator==(const G4RKFieldIntegrator &) const {return 1;} int 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