Gabriele Cosmo
219 lines
12 KiB
C++
219 lines
12 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. *
|
|
// ********************************************************************
|
|
//
|
|
// INCL++ intra-nuclear cascade model
|
|
// Alain Boudard, CEA-Saclay, France
|
|
// Joseph Cugnon, University of Liege, Belgium
|
|
// Jean-Christophe David, CEA-Saclay, France
|
|
// Pekka Kaitaniemi, CEA-Saclay, France, and Helsinki Institute of Physics, Finland
|
|
// Sylvie Leray, CEA-Saclay, France
|
|
// Davide Mancusi, CEA-Saclay, France
|
|
//
|
|
#define INCLXX_IN_GEANT4_MODE 1
|
|
|
|
#include "globals.hh"
|
|
|
|
/** \file G4INCLICrossSections.hh
|
|
* \brief Abstract interface for the cross-section classes
|
|
*
|
|
* \date 25nd October 2013
|
|
* \author Davide Mancusi
|
|
*/
|
|
|
|
#ifndef G4INCLICROSSSECTIONS_HH
|
|
#define G4INCLICROSSSECTIONS_HH
|
|
|
|
#include "G4INCLParticle.hh"
|
|
|
|
namespace G4INCL {
|
|
/// \brief Abstract interface for the cross-section classes
|
|
class ICrossSections {
|
|
public:
|
|
|
|
ICrossSections() {}
|
|
virtual ~ICrossSections() {}
|
|
|
|
/// \brief Elastic particle-particle cross section
|
|
virtual G4double elastic(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Total (elastic+inelastic) particle-particle cross section
|
|
virtual G4double total(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NDelta->NN
|
|
virtual G4double NDeltaToNN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NN->NDelta
|
|
virtual G4double NNToNDelta(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NN->xpiN
|
|
virtual G4double NNToxPiNN(const G4int xpi, Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for piN->NDelta
|
|
virtual G4double piNToDelta(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for piN->piNpi
|
|
virtual G4double piNToxPiN(const G4int xpi, Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for PiN->EtaN
|
|
virtual G4double piNToEtaN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for PiN->OmegaN
|
|
virtual G4double piNToOmegaN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for PiN->EtaPrimeN
|
|
virtual G4double piNToEtaPrimeN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for EtaN->PiN
|
|
virtual G4double etaNToPiN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for EtaN->PiPiN
|
|
virtual G4double etaNToPiPiN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for EtaN->LK/SK
|
|
virtual G4double etaNToLK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double etaNToSK(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for OmegaN->PiN
|
|
virtual G4double omegaNToPiN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for OmegaN->PiPiN
|
|
virtual G4double omegaNToPiPiN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for OmegaN->LK/SK
|
|
virtual G4double omegaNToLK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double omegaNToSK(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for EtaPrimeN->PiN
|
|
virtual G4double etaPrimeNToPiN(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NN->NNEta (inclusive)
|
|
virtual G4double NNToNNEta(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NN->NNEta (exclusive)
|
|
virtual G4double NNToNNEtaExclu(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NN->NNEtaxPi
|
|
virtual G4double NNToNNEtaxPi(const G4int xpi, Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for N-Delta-Eta production - NNEta Channel
|
|
virtual G4double NNToNDeltaEta(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NN->NNEta (inclusive)
|
|
virtual G4double NNToNNOmega(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NN->NNEta (exclusive)
|
|
virtual G4double NNToNNOmegaExclu(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for NN->NNEtaxPi
|
|
virtual G4double NNToNNOmegaxPi(const G4int xpi, Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Cross section for N-Delta-Eta production - NNEta Channel
|
|
virtual G4double NNToNDeltaOmega(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
|
|
/// \brief elastic scattering for Nucleon-Strange Particles cross sections
|
|
virtual G4double NYelastic(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKbelastic(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKelastic(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Nucleon-Nucleon to Stange particles cross sections
|
|
virtual G4double NNToNLK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NNToNSK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NNToNLKpi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NNToNSKpi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NNToNLK2pi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NNToNSK2pi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NNToNNKKb(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NNToMissingStrangeness(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Nucleon-Delta to Stange particles cross sections
|
|
virtual G4double NDeltaToNLK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NDeltaToNSK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NDeltaToDeltaLK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NDeltaToDeltaSK(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
virtual G4double NDeltaToNNKKb(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Nucleon-Pion to Stange particles cross sections
|
|
virtual G4double NpiToLK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NpiToSK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double p_pimToSzKz(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double p_pimToSmKp(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double p_pizToSzKp(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NpiToLKpi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NpiToSKpi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NpiToLK2pi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NpiToSK2pi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NpiToNKKb(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NpiToMissingStrangeness(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Nucleon-Hyperon cross sections
|
|
virtual G4double NLToNS(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NSToNL(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NSToNS(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Nucleon-Kaon inelastic cross sections
|
|
virtual G4double NKToNK(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKToNKpi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKToNK2pi(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Nucleon-antiKaon inelastic cross sections
|
|
virtual G4double NKbToNKb(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKbToSpi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKbToLpi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKbToS2pi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKbToL2pi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKbToNKbpi(Particle const * const p1, Particle const * const p2) = 0;
|
|
virtual G4double NKbToNKb2pi(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief NNbar Particles cross sections
|
|
/// \brief Nucleon-AntiNucleon to Baryon-AntiBaryon cross sections
|
|
virtual G4double NNbarElastic(Particle const* const p1, Particle const* const p2) = 0;
|
|
virtual G4double NNbarCEX(Particle const* const p1, Particle const* const p2) = 0;
|
|
|
|
virtual G4double NNbarToLLbar(Particle const * const p1, Particle const * const p2) = 0;
|
|
|
|
/// \brief Nucleon-AntiNucleon to Nucleon-AntiNucleon + pions cross sections
|
|
virtual G4double NNbarToNNbarpi(Particle const* const p1, Particle const* const p2) = 0;
|
|
virtual G4double NNbarToNNbar2pi(Particle const* const p1, Particle const* const p2) = 0;
|
|
virtual G4double NNbarToNNbar3pi(Particle const* const p1, Particle const* const p2) = 0;
|
|
|
|
/// \brief Nucleon-AntiNucleon total annihilation cross sections
|
|
virtual G4double NNbarToAnnihilation(Particle const* const p1, Particle const* const p2) = 0;
|
|
|
|
/** \brief Calculate the slope of the NN DDXS.
|
|
*
|
|
* \param energyCM energy in the CM frame, in MeV
|
|
* \param iso total isospin of the system
|
|
*
|
|
* \return the slope of the angular distribution
|
|
*/
|
|
virtual G4double calculateNNAngularSlope(G4double energyCM, G4int iso) = 0;
|
|
|
|
};
|
|
}
|
|
|
|
#endif
|