// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // $Id: G4PreCompoundTransitions.hh,v 1.8 2010-08-28 15:16:55 vnivanch Exp $ // GEANT4 tag $Name: not supported by cvs2svn $ // // by V. Lara // 01.05.2008 J. M. Quesada . New methods for accessing to individual transition // probabilities (landa+, landa-, landa0) from G4PreCompoundModel // 20.08.2010 V.Ivanchenko move constructor and destructor to the source #ifndef G4PreCompoundTransitions_h #define G4PreCompoundTransitions_h 1 // Compute transition probailities: // TransitionProb1 => probability of transition with \Delta N = +2 // number of excitons will be increased on 2 // TransitionProb2 => probability of transition with \Delta N = -2 // number of excitons will be decreased on 2 // TransitionProb3 => probability of transition with \Delta N = 0 // number of excitons will be the same #include "G4VPreCompoundTransitions.hh" #include "globals.hh" #include "G4Fragment.hh" class G4ParticleDefinition; class G4Pow; class G4PreCompoundTransitions : public G4VPreCompoundTransitions { public: G4PreCompoundTransitions(); virtual ~G4PreCompoundTransitions(); virtual G4double CalculateProbability(const G4Fragment & aFragment); virtual void PerformTransition(G4Fragment & aFragment); private: G4PreCompoundTransitions(const G4PreCompoundTransitions &); const G4PreCompoundTransitions& operator=(const G4PreCompoundTransitions &right); G4bool operator==(const G4PreCompoundTransitions &right) const; G4bool operator!=(const G4PreCompoundTransitions &right) const; G4Pow* g4pow; const G4ParticleDefinition* proton; G4double FermiEnergy; G4double r0; // Nuclear radius G4double aLDP;// Level density parameter }; #endif