Import Geant4 9.2.0 source tree

source/processes/hadronic/models/de_excitation/handler/include/G4ExcitationHandler.hh

@@ -24,11 +24,15 @@
 // ********************************************************************
 //
 //
-// $Id: G4ExcitationHandler.hh,v 1.7 2006/08/19 19:55:59 dennis Exp $
-// GEANT4 tag $Name: geant4-09-01 $
+// $Id: G4ExcitationHandler.hh,v 1.8 2008/09/19 13:32:54 ahoward Exp $
+// GEANT4 tag $Name: geant4-09-02 $
 //
 // Hadronic Process: Nuclear De-excitations
 // by V. Lara (May 1998)
+//
+// Modif (03 September 2008) by J. M. Quesada for external choice of inverse 
+// cross section option
+//
 // Modif (30 June 1998) by V. Lara:
 //      -Using G4ParticleTable and therefore G4IonTable
 //       it can return all kind of fragments produced in 
@@ -37,7 +41,11 @@
 //              Evaporation: G4StatEvaporation
 //              MultiFragmentation: G4DummyMF (a dummy one)
 //              Fermi Breakup model: G4StatFermiBreakUp
-
+//
+// Modif (03 September 2008) by J. M. Quesada for external choice of inverse 
+// cross section option
+// JMQ (06 September 2008) Also external choices have been added for 
+// superimposed Coulomb barrier (if useSICBis set true, by default is false) 
 
 #ifndef G4ExcitationHandler_h
 #define G4ExcitationHandler_h 1
@@ -90,6 +98,11 @@ public:
   void SetMaxAandZForFermiBreakUp(G4int anA,G4int aZ);
   void SetMinEForMultiFrag(G4double anE);
 
+// for inverse cross section choice
+  inline void SetOPTxs(G4int opt) { OPTxs = opt;}
+// for superimposed Coulomb Barrir for inverse cross sections
+  inline void UseSICB(){useSICB=true;}
+
 private:
 
   G4ReactionProductVector * Transform(G4FragmentVector * theFragmentVector) const;
@@ -131,6 +144,9 @@ private:
   G4bool MyOwnFermiBreakUpClass;
   G4bool MyOwnPhotonEvaporationClass;
 
+  G4int OPTxs;
+  G4bool useSICB;
+
   struct DeleteFragment 
   {
     template<typename T>