Gabriele Cosmo
79 lines
3.6 KiB
C++
79 lines
3.6 KiB
C++
// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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/// \file HadronPhysicsCRMC_FTFP_BERT.hh
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/// \brief Definition of the HadronPhysicsCRMC_FTFP_BERT class
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//---------------------------------------------------------------------------
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//
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// ClassName: HadronPhysicsCRMC_FTFP_BERT
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//
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// Author: 2018 Alberto Ribon
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//
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// This is a variant of HadronPhysicsFTFP_BERT whereby CRMC is used
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// for modeling final-state for pion- , kaon- , proton- and neutron-
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// nuclear inelastic interactions at very high energies.
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// For other hadron projectile types (e.g. hyperons, antinucleons and
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// antihyperons) the usual FTFP_BERT approach is used at all energies.
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// The inelastic hadronic cross sections are, for all hadron projectiles
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// and energies, the usual ones (exactly as in FTFP_BERT).
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//
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// Modified:
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// - 18-May-2021 Alberto Ribon : Migrated to newer physics constructor
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// and used the latest Geant4-CRMC interface.
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//
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//----------------------------------------------------------------------------
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//
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#ifndef HadronPhysicsCRMC_FTFP_BERT_h
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#define HadronPhysicsCRMC_FTFP_BERT_h 1
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#include "G4HadronPhysicsFTFP_BERT.hh"
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class HadronPhysicsCRMC_FTFP_BERT : public G4HadronPhysicsFTFP_BERT
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{
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public:
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HadronPhysicsCRMC_FTFP_BERT(G4int verbose = 1);
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HadronPhysicsCRMC_FTFP_BERT(const G4String& name, G4bool quasiElastic = false);
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~HadronPhysicsCRMC_FTFP_BERT() override;
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// copy constructor and hide assignment operator
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HadronPhysicsCRMC_FTFP_BERT(HadronPhysicsCRMC_FTFP_BERT&) = delete;
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HadronPhysicsCRMC_FTFP_BERT& operator=(const HadronPhysicsCRMC_FTFP_BERT& right) = delete;
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protected:
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virtual void Neutron() override;
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virtual void Proton() override;
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virtual void Pion() override;
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virtual void Kaon() override;
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private:
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G4int fModel; // 0:EPOS-LHC, 1:EPOS-1.99, 2:QGSJET:01, 6:SIBYLL-2.3,
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static const std::array<std::string, 13>
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fModelNames; // 7:QGSJETII-04, 11:QGSJETII-03, 12:DPMJET-3.06
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G4double fMinCRMC;
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G4double fMaxFTFP;
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};
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#endif
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