// // ******************************************************************** // * 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 // Pekka Kaitaniemi, CEA and Helsinki Institute of Physics // Davide Mancusi, CEA // Alain Boudard, CEA // Sylvie Leray, CEA // Joseph Cugnon, University of Liege // #define INCLXX_IN_GEANT4_MODE 1 #include "globals.hh" #ifndef G4INCLCrossSections_hh #define G4INCLCrossSections_hh 1 #include "G4INCLParticle.hh" #include "G4INCLIAvatar.hh" #include "G4INCLIChannel.hh" namespace G4INCL { class CrossSections { public: static G4double elastic(Particle const * const p1, Particle const * const p2); static G4double total(Particle const * const p1, Particle const * const p2); static G4double pionNucleon(Particle const * const p1, Particle const * const p2); static G4double recombination(Particle const * const p1, Particle const * const p2); static G4double deltaProduction(Particle const * const p1, Particle const * const p2); /** \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 */ static G4double calculateNNDiffCrossSection(G4double energyCM, G4int iso); /** \brief Compute the "interaction distance". * * Defined on the basis of the average value of the N-N cross sections at * the given kinetic energy. * * \return the interaction distance */ static G4double interactionDistanceNN(const G4double projectileKineticEnergy); /** \brief Compute the "interaction distance". * * Defined on the basis of the average value of the pi-N cross sections at * the given kinetic energy. * * \return the interaction distance */ static G4double interactionDistancePiN(const G4double projectileKineticEnergy); /** \brief The interaction distance for nucleons at 1 GeV. * * Used to determine the universe radius at any energy. */ static G4double interactionDistanceNN1GeV() { static G4double answer = CrossSections::interactionDistanceNN(1000.); return answer; } /** \brief The interaction distance for pions at 1 GeV. * * Used to determine the universe radius at any energy. */ static G4double interactionDistancePiN1GeV() { static G4double answer = CrossSections::interactionDistancePiN(1000.); return answer; } private: static G4double elasticNNHighEnergy(const G4double momentum); static G4double elasticProtonNeutron(const G4double momentum); static G4double elasticProtonProtonOrNeutronNeutron(const G4double momentum); static G4double elasticNN(Particle const * const p1, Particle const * const p2); static G4double elasticNNLegacy(Particle const * const p1, Particle const * const p2); static G4double deltaProduction(const G4int isospin, const G4double pCM); static G4double spnPiPlusPHE(const G4double x); static G4double spnPiMinusPHE(const G4double x); protected: CrossSections() {}; ~CrossSections() {}; }; } #endif