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/// \file HadronPhysicsCRMC_FTFP_BERT.hh
/// \brief Definition of the HadronPhysicsCRMC_FTFP_BERT class

//---------------------------------------------------------------------------
//
// ClassName: HadronPhysicsCRMC_FTFP_BERT
//
// Author:    2018 Alberto Ribon
//
// This is a variant of HadronPhysicsFTFP_BERT whereby CRMC is used
// for modeling final-state for pion- , kaon- , proton- and neutron-
// nuclear inelastic interactions at very high energies.
// For other hadron projectile types (e.g. hyperons, antinucleons and
// antihyperons) the usual FTFP_BERT approach is used at all energies.
// The inelastic hadronic cross sections are, for all hadron projectiles
// and energies, the usual ones (exactly as in FTFP_BERT).
//
// Modified:
// -  18-May-2021 Alberto Ribon : Migrated to newer physics constructor
//                                and used the latest Geant4-CRMC interface.
//
//----------------------------------------------------------------------------
//
#ifndef HadronPhysicsCRMC_FTFP_BERT_h
#define HadronPhysicsCRMC_FTFP_BERT_h 1

#include "G4HadronPhysicsFTFP_BERT.hh"

class HadronPhysicsCRMC_FTFP_BERT : public G4HadronPhysicsFTFP_BERT
{
  public:
    HadronPhysicsCRMC_FTFP_BERT(G4int verbose = 1);
    HadronPhysicsCRMC_FTFP_BERT(const G4String& name, G4bool quasiElastic = false);
    ~HadronPhysicsCRMC_FTFP_BERT() override;

    // copy constructor and hide assignment operator
    HadronPhysicsCRMC_FTFP_BERT(HadronPhysicsCRMC_FTFP_BERT&) = delete;
    HadronPhysicsCRMC_FTFP_BERT& operator=(const HadronPhysicsCRMC_FTFP_BERT& right) = delete;

  protected:
    virtual void Neutron() override;
    virtual void Proton() override;
    virtual void Pion() override;
    virtual void Kaon() override;

  private:
    G4int fModel;  // 0:EPOS-LHC, 1:EPOS-1.99, 2:QGSJET:01, 6:SIBYLL-2.3,
    static const std::array<std::string, 13>
      fModelNames;  // 7:QGSJETII-04, 11:QGSJETII-03, 12:DPMJET-3.06
    G4double fMinCRMC;
    G4double fMaxFTFP;
};

#endif