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//
// ********************************************************************
// * 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. *
// ********************************************************************
//
// Author: Elena Guardincerri (Elena.Guardincerri@ge.infn.it)
//
// History:
// -----------
// 16 Sept 2001 First committed to cvs
//
// -------------------------------------------------------------------
// Class description:
// Low Energy Electromagnetic Physics
// Fluorescence data set: shell identifiers, transition probabilities,
// transition energies
// -------------------------------------------------------------------
#ifndef G4FLUODATA_HH
#define G4FLUODATA_HH 1
#include "globals.hh"
#include <vector>
#include <map>
class G4FluoTransition;
class G4DataVector;
class G4FluoData
{
public:
explicit G4FluoData(const G4String& dir);
~G4FluoData();
/// The method returns the number of shells in wich a
/// vacancy can be filled by a radiative transition
std::size_t NumberOfVacancies() const;
/// Given the index of the vacancy returns its identity
G4int VacancyId(G4int vacancyIndex) const;
/// Given the index of a vacancy returns the number of
/// shells starting from wich an electrons can fill the vacancy
std::size_t NumberOfTransitions(G4int vacancyIndex) const;
/// Given the indexes of the starting and final shells for the
/// transition, returns the identity of the starting one
G4int StartShellId(G4int initIndex, G4int vacancyIndex) const;
/// Given the indexes of the starting and final shells for the
/// transition, returns the transition energy
G4double StartShellEnergy(G4int initIndex, G4int vacancyIndex) const;
/// Given the indexes of the starting and final shells for the
/// transition, returns the probability of this transition
G4double StartShellProb(G4int initIndex, G4int vacancyIndex) const;
void LoadData(G4int Z);
void PrintData();
G4FluoData& operator=(const G4FluoData& right) = delete;
G4FluoData(const G4FluoData&) = delete;
private:
std::map<G4int,G4DataVector*,std::less<G4int> > idMap;
std::map<G4int,G4DataVector*,std::less<G4int> > energyMap;
std::map<G4int,G4DataVector*,std::less<G4int> > probabilityMap;
std::vector<G4int> nInitShells;
std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> > fluoTransitionTable;
G4String fluoDirectory;
G4int numberOfVacancies = 0;
};
#endif