// // ******************************************************************** // * 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. * // ******************************************************************** // // // // Authors: Elena Guardincerri (Elena.Guardincerri@ge.infn.it) // Alfonso Mantero (Alfonso.Mantero@ge.infn.it) // // History: // ----------- // // 16 Sept 2001 EG Modified according to a design iteration in the // LowEnergy category // // ------------------------------------------------------------------- // Class description: // Low Energy Electromagnetic Physics: create or fills and manages G4RDAtomicShell, // G4RDFluoTransition, G4RDAugerTransition objects. // Further documentation available from http://www.ge.infn.it/geant4/lowE // ------------------------------------------------------------------- #ifndef G4RDAtomicTransitionManager_h #define G4RDAtomicTransitionManager_h 1 #include "G4RDShellData.hh" #include "G4RDFluoData.hh" #include "G4RDAugerData.hh" #include "G4RDFluoTransition.hh" #include "G4RDAtomicShell.hh" // #include "g4std/map" #include #include "globals.hh" // This class is a singleton class G4RDAtomicTransitionManager { public: // The only way to get an instance of this class is to call the // function Instance() static G4RDAtomicTransitionManager* Instance(); // Z is the atomic number of the element, shellIndex is the // index (in EADL) of the shell G4RDAtomicShell* Shell(G4int Z, size_t shellIndex) const; // Z is the atomic number of the element, shellIndex is the // index (in EADL) of the final shell for the transition // This function gives, upon Z and the Index of the initial shell where te vacancy is, // the radiative transition that can happen (originating shell, energy, probability) const G4RDFluoTransition* ReachableShell(G4int Z, size_t shellIndex) const ; // This function gives, upon Z and the Index of the initial shell where te vacancy is, // the NON-radiative transition that can happen with originating shell for the transition, and the // data for the possible auger electrons emitted (originating vacancy, energy amnd probability) const G4RDAugerTransition* ReachableAugerShell(G4int Z, G4int shellIndex) const ; // This function returns the number of shells of the element // whose atomic number is Z G4int NumberOfShells(G4int Z) const; // This function returns the number of those shells of the element // whose atomic number is Z which are reachable through a radiative // transition // This function returns the number of possible radiative transitions for the atom with atomic number Z // i.e. the number of shell in wich a vacancy can be filled with a radiative transition G4int NumberOfReachableShells(G4int Z)const ; // This function returns the number of possible NON-radiative transitions for the atom with atomic number Z // i.e. the number of shell in wich a vacancy can be filled by a NON-radiative transition G4int NumberOfReachableAugerShells(G4int Z)const ; // Gives the sum of the probabilities of radiative transition towards the // shell whose index is shellIndex G4double TotalRadiativeTransitionProbability(G4int Z, size_t shellIndex); // Gives the sum of the probabilities of non radiative transition from the // shell whose index is shellIndex G4double TotalNonRadiativeTransitionProbability(G4int Z, size_t shellIndex); protected: G4RDAtomicTransitionManager(G4int minZ = 1, G4int maxZ = 100, G4int limitInfTable = 6, G4int limitSupTable=100 ); ~G4RDAtomicTransitionManager(); private: // Hide copy constructor and assignment operator G4RDAtomicTransitionManager& operator=(const G4RDAtomicTransitionManager& right); G4RDAtomicTransitionManager(const G4RDAtomicTransitionManager&); static G4RDAtomicTransitionManager* instance; // the first element of the map is the atomic number Z. // the second element is a vector of G4RDAtomicShell*. std::map,std::less > shellTable; // the first element of the map is the atomic number Z. // the second element is a vector of G4AtomicTransition*. std::map,std::less > transitionTable; // since Augereffect data r stored as a table in G4RDAugerData, we have here a pointer to an element of that class itself. G4RDAugerData* augerData; // Minimum and maximum Z in EADL table containing identities and binding // energies of shells G4int zMin; G4int zMax; // Minimum and maximum Z in EADL table containing identities, transition // energies and transition probabilities of shells G4int infTableLimit; G4int supTableLimit; }; #endif