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1 // ******************************************************************** 2 // * License and Disclaimer * 3 // * * 4 // * The Geant4 software is copyright of the Copyright Holders of * 5 // * the Geant4 Collaboration. It is provided under the terms and * 6 // * conditions of the Geant4 Software License, included in the file * 7 // * LICENSE and available at http://cern.ch/geant4/license . These * 8 // * include a list of copyright holders. * 9 // * * 10 // * Neither the authors of this software system, nor their employing * 11 // * institutes,nor the agencies providing financial support for this * 12 // * work make any representation or warranty, express or implied, * 13 // * regarding this software system or assume any liability for its * 14 // * use. Please see the license in the file LICENSE and URL above * 15 // * for the full disclaimer and the limitation of liability. * 16 // * * 17 // * This code implementation is the result of the scientific and * 18 // * technical work of the GEANT4 collaboration. * 19 // * By using, copying, modifying or distributing the software (or * 20 // * any work based on the software) you agree to acknowledge its * 21 // * use in resulting scientific publications, and indicate your * 22 // * acceptance of all terms of the Geant4 Software license. * 23 // ******************************************************************** 24 // 25 /// \file hadronic/Hadr02/include/HadronPhysicsCRMC_FTFP_BERT.hh 26 /// \brief Definition of the HadronPhysicsCRMC_FTFP_BERT class 27 // 28 // 29 //--------------------------------------------------------------------------- 30 // 31 // ClassName: HadronPhysicsCRMC_FTFP_BERT 32 // 33 // Author: 2018 Alberto Ribon 34 // 35 // This is a variant of HadronPhysicsFTFP_BERT whereby CRMC is used 36 // for modeling final-state for pion- , kaon- , proton- and neutron- 37 // nuclear inelastic interactions at very high energies. 38 // For other hadron projectile types (e.g. hyperons, antinucleons and 39 // antihyperons) the usual FTFP_BERT approach is used at all energies. 40 // The inelastic hadronic cross sections are, for all hadron projectiles 41 // and energies, the usual ones (exactly as in FTFP_BERT). 42 // 43 // Modified: 44 // - 18-May-2021 Alberto Ribon : Migrated to newer physics constructor 45 // and used the latest Geant4-CRMC interface. 46 // 47 //---------------------------------------------------------------------------- 48 // 49 #ifndef HadronPhysicsCRMC_FTFP_BERT_h 50 #define HadronPhysicsCRMC_FTFP_BERT_h 1 51 52 #include "G4HadronPhysicsFTFP_BERT.hh" 53 54 class HadronPhysicsCRMC_FTFP_BERT : public G4HadronPhysicsFTFP_BERT 55 { 56 public: 57 HadronPhysicsCRMC_FTFP_BERT(G4int verbose = 1); 58 HadronPhysicsCRMC_FTFP_BERT(const G4String& name, G4bool quasiElastic = false); 59 ~HadronPhysicsCRMC_FTFP_BERT() override; 60 61 // copy constructor and hide assignment operator 62 HadronPhysicsCRMC_FTFP_BERT(HadronPhysicsCRMC_FTFP_BERT&) = delete; 63 HadronPhysicsCRMC_FTFP_BERT& operator=(const HadronPhysicsCRMC_FTFP_BERT& right) = delete; 64 65 protected: 66 virtual void Neutron() override; 67 virtual void Proton() override; 68 virtual void Pion() override; 69 virtual void Kaon() override; 70 71 private: 72 G4int fModel; // 0:EPOS-LHC, 1:EPOS-1.99, 2:QGSJET:01, 6:SIBYLL-2.3, 73 static const std::array<std::string, 13> 74 fModelNames; // 7:QGSJETII-04, 11:QGSJETII-03, 12:DPMJET-3.06 75 G4double fMinCRMC; 76 G4double fMaxFTFP; 77 }; 78 79 #endif 80