Geant4 Cross Reference |
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Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitatio 16 // * for the full disclaimer and the limitation of liability. * 17 // * 17 // * * 18 // * This code implementation is the result 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboratio 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distri 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you ag 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publicati 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Sof 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************* 24 // ******************************************************************** 25 // 25 // 26 /// \file hadronic/Hadr02/include/CRMC_FTFP_BE 26 /// \file hadronic/Hadr02/include/CRMC_FTFP_BERT.hh 27 /// \brief Definition of the CRMC_FTFP_BERT cl 27 /// \brief Definition of the CRMC_FTFP_BERT class 28 // 28 // 29 // 29 // 30 //-------------------------------------------- 30 //--------------------------------------------------------------------------- 31 // 31 // 32 // ClassName: CRMC_FTFP_BERT << 32 // ClassName: CRMC_FTFP_BERT 33 // 33 // 34 // Author: 2018 Alberto Ribon 34 // Author: 2018 Alberto Ribon 35 // 35 // 36 // This is a variant of the FTFP_BERT physics << 36 // This is a variant of the FTFP_BERT physics list, whereby CRMC is used 37 // for modeling final-state pion- , kaon- , pr << 37 // for modeling final-state pion- , kaon- , proton- , neutron- and 38 // ion-nuclear inelastic interactions at very 38 // ion-nuclear inelastic interactions at very high energies (above a 39 // threshold defined in HadronPhysicsCRMC_FTFP 39 // threshold defined in HadronPhysicsCRMC_FTFP_BERT and IonCRMCPhysics). 40 // For the remaining inelastic interactions (i 40 // For the remaining inelastic interactions (i.e. hyperon- , antihyperon- , 41 // antinucleon- and light anti-ion-nuclear int 41 // antinucleon- and light anti-ion-nuclear interactions, as well as 42 // for all elastic final-state interactions, a 42 // for all elastic final-state interactions, and for all elastic and 43 // inelastic hadronic cross sections), the usu 43 // inelastic hadronic cross sections), the usual Geant4 approach, as in 44 // FTFP_BERT is used. 44 // FTFP_BERT is used. 45 // 45 // 46 // Modified: 46 // Modified: 47 // - 18-May-2021 Alberto Ribon : Migrated to 47 // - 18-May-2021 Alberto Ribon : Migrated to non-templated physics list. 48 // 48 // 49 //-------------------------------------------- 49 //---------------------------------------------------------------------------- 50 // 50 // 51 #ifndef CRMC_FTFP_BERT_h 51 #ifndef CRMC_FTFP_BERT_h 52 #define CRMC_FTFP_BERT_h 1 52 #define CRMC_FTFP_BERT_h 1 53 53 54 #include "G4VModularPhysicsList.hh" << 55 #include "globals.hh" 54 #include "globals.hh" >> 55 #include "G4VModularPhysicsList.hh" >> 56 56 57 57 class CRMC_FTFP_BERT : public G4VModularPhysic << 58 class CRMC_FTFP_BERT : public G4VModularPhysicsList { 58 { << 59 public: 59 public: 60 CRMC_FTFP_BERT(G4int ver = 1); << 60 CRMC_FTFP_BERT( G4int ver = 1 ); 61 virtual ~CRMC_FTFP_BERT() = default; 61 virtual ~CRMC_FTFP_BERT() = default; 62 62 63 CRMC_FTFP_BERT(const CRMC_FTFP_BERT&) = de << 63 CRMC_FTFP_BERT( const CRMC_FTFP_BERT & ) = delete; 64 CRMC_FTFP_BERT& operator=(const CRMC_FTFP_ << 64 CRMC_FTFP_BERT & operator=( const CRMC_FTFP_BERT & ) = delete; 65 }; 65 }; 66 66 67 #endif 67 #endif 68 68