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//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (May 1998)
//
// Modifications:
// 30 June 1998 by V. Lara:
//      -Using G4ParticleTable and therefore G4IonTable
//       it can return all kind of fragments produced in 
//       deexcitation
//      -It uses default algorithms for:
//              Evaporation: G4StatEvaporation
//              MultiFragmentation: G4DummyMF (a dummy one)
//              Fermi Breakup model: G4StatFermiBreakUp
//
// 03 September 2008 by J. M. Quesada for external choice of inverse 
//    cross section option
// 06 September 2008 JMQ Also external choices have been added for 
//    superimposed Coulomb barrier (if useSICBis set true, by default is false) 
// 23 January 2012 by V.Ivanchenko remove obsolete data members; added access
//    methods to deexcitation components
//                   

#ifndef G4ExcitationHandler_h
#define G4ExcitationHandler_h 1

#include "globals.hh"
#include "G4Fragment.hh"
#include "G4ReactionProductVector.hh"
#include "G4IonTable.hh"
#include "G4DeexPrecoParameters.hh"
#include "G4NistManager.hh"

class G4VMultiFragmentation;
class G4VFermiBreakUp;
class G4VEvaporation;
class G4VEvaporationChannel;
class G4ParticleTable;

class G4ExcitationHandler 
{
public:

  G4ExcitationHandler(); 
  ~G4ExcitationHandler();

  G4ReactionProductVector* BreakItUp(const G4Fragment &theInitialState);

  // short model description used for automatic web documentation
  void ModelDescription(std::ostream& outFile) const;

  void Initialise();

  // user defined sub-models
  // deletion is responsibility of this handler if isLocal=true 
  void SetEvaporation(G4VEvaporation* ptr, G4bool isLocal=false);
  void SetMultiFragmentation(G4VMultiFragmentation* ptr);
  void SetFermiModel(G4VFermiBreakUp* ptr);
  void SetPhotonEvaporation(G4VEvaporationChannel* ptr);
  void SetDeexChannelsType(G4DeexChannelType val);

  //======== Obsolete methods to be removed =====

  // parameters of sub-models
  inline void SetMaxZForFermiBreakUp(G4int aZ);
  inline void SetMaxAForFermiBreakUp(G4int anA);
  inline void SetMaxAandZForFermiBreakUp(G4int anA,G4int aZ);
  void SetMinEForMultiFrag(G4double anE);

  // access methods
  G4VEvaporation* GetEvaporation();
  G4VMultiFragmentation* GetMultiFragmentation();
  G4VFermiBreakUp* GetFermiModel();
  G4VEvaporationChannel* GetPhotonEvaporation();

  // for inverse cross section choice
  inline void SetOPTxs(G4int opt);
  // for superimposed Coulomb Barrier for inverse cross sections
  inline void UseSICB();

  //==============================================

  G4ExcitationHandler(const G4ExcitationHandler &right) = delete;
  const G4ExcitationHandler & operator
  =(const G4ExcitationHandler &right) = delete;
  G4bool operator==(const G4ExcitationHandler &right) const = delete;
  G4bool operator!=(const G4ExcitationHandler &right) const = delete;

private:

  void SetParameters();

  inline void SortSecondaryFragment(G4Fragment*);
  
  G4VEvaporation* theEvaporation{nullptr};
  G4VMultiFragmentation* theMultiFragmentation{nullptr};
  G4VFermiBreakUp* theFermiModel;
  G4VEvaporationChannel* thePhotonEvaporation;
  G4ParticleTable* thePartTable;
  G4IonTable* theTableOfIons;
  G4NistManager* nist;

  const G4ParticleDefinition* theElectron;
  const G4ParticleDefinition* theNeutron;
  const G4ParticleDefinition* theProton;
  const G4ParticleDefinition* theDeuteron;
  const G4ParticleDefinition* theTriton;
  const G4ParticleDefinition* theHe3;
  const G4ParticleDefinition* theAlpha;
  const G4ParticleDefinition* theLambda;

  G4int icID{0};

  G4int maxZForFermiBreakUp{9};
  G4int maxAForFermiBreakUp{17};

  G4int  fVerbose{1};
  G4int  fWarnings{0};

  G4double minExcitation;
  G4double fLambdaMass;

  G4bool isInitialised{false};
  G4bool isEvapLocal{true};
  G4bool isActive{true};

  // list of fragments to store final result   
  std::vector<G4Fragment*> theResults;

  // list of fragments to store intermediate result   
  std::vector<G4Fragment*> results;

  // list of fragments to apply Evaporation or Fermi Break-Up
  std::vector<G4Fragment*> theEvapList;          
};

inline void G4ExcitationHandler::SetMaxZForFermiBreakUp(G4int aZ)
{
  maxZForFermiBreakUp = aZ;
}

inline void G4ExcitationHandler::SetMaxAForFermiBreakUp(G4int anA)
{
  maxAForFermiBreakUp = anA;
}

inline void G4ExcitationHandler::SetMaxAandZForFermiBreakUp(G4int anA, G4int aZ)
{
  SetMaxAForFermiBreakUp(anA);
  SetMaxZForFermiBreakUp(aZ);
}

inline void G4ExcitationHandler::SortSecondaryFragment(G4Fragment* frag)
{ 
  G4int A = frag->GetA_asInt();  

  // gamma, e-, p, n
  if(A <= 1 || frag->IsLongLived()) { 
    theResults.push_back(frag); 
  } else if(frag->GetExcitationEnergy() < minExcitation) {
    // cold fragments
    G4int Z = frag->GetZ_asInt(); 
       
    // is stable or d, t, He3, He4
    if(nist->GetIsotopeAbundance(Z, A) > 0.0 || (A == 3 && (Z == 1 || Z == 2)) ) {
      theResults.push_back(frag); // stable fragment 
    } else {
      theEvapList.push_back(frag);
    }
    // hot fragments are unstable
  } else { 
    theEvapList.push_back(frag);  
  }
}

#endif