source: trunk/source/processes/electromagnetic/lowenergy/include/G4AtomicTransitionManager.hh @ 1315

Last change on this file since 1315 was 1315, checked in by garnier, 14 years ago

update geant4-09-04-beta-cand-01 interfaces-V09-03-09 vis-V09-03-08

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26//
27// $Id: G4AtomicTransitionManager.hh,v 1.2 ????
28// GEANT4 tag $Name: geant4-09-04-beta-cand-01 $
29//
30// Authors: Elena Guardincerri (Elena.Guardincerri@ge.infn.it)
31//          Alfonso Mantero (Alfonso.Mantero@ge.infn.it)
32//
33// History:
34// -----------
35// 
36//  16 Sept 2001 EG  Modified according to a design iteration in the
37//                   LowEnergy category
38//
39// -------------------------------------------------------------------
40
41// Class description:
42// Low Energy Electromagnetic Physics: create or fills and manages G4AtomicShell,
43// G4FluoTransition, G4AugerTransition objects.
44// Further documentation available from http://www.ge.infn.it/geant4/lowE
45
46// -------------------------------------------------------------------
47
48#ifndef G4AtomicTransitionManager_h
49#define G4AtomicTransitionManager_h 1
50
51#include "G4ShellData.hh"
52#include "G4FluoData.hh"
53#include "G4AugerData.hh"
54#include "G4FluoTransition.hh"
55#include "G4AtomicShell.hh"
56// #include "g4std/map"
57#include <vector>
58#include "globals.hh"
59
60// This class is a singleton
61class G4AtomicTransitionManager {
62
63public: 
64
65  // The only way to get an instance of this class is to call the
66  // function Instance()
67  static G4AtomicTransitionManager* Instance();
68 
69  // Z is the atomic number of the element, shellIndex is the
70  // index (in EADL) of the shell
71  G4AtomicShell* Shell(G4int Z, size_t shellIndex) const;
72   
73  // Z is the atomic number of the element, shellIndex is the
74  // index (in EADL) of the final shell for the transition
75  // This function gives, upon Z and the Index of the initial shell where te vacancy is,
76  // the radiative transition that can happen (originating shell, energy, probability)
77  const G4FluoTransition* ReachableShell(G4int Z, size_t shellIndex) const ;
78
79  // This function gives, upon Z and the Index of the initial shell where te vacancy is,
80  // the NON-radiative transition that can happen with originating shell for the transition, and the
81  // data for the possible auger electrons emitted (originating vacancy, energy amnd probability)
82 
83  const G4AugerTransition* ReachableAugerShell(G4int Z, G4int shellIndex) const ;
84 
85  // This function returns the number of shells of the element
86  // whose atomic number is Z
87  G4int NumberOfShells(G4int Z) const;
88 
89  // This function returns the number of those shells of the element
90  // whose atomic number is Z which are reachable through a radiative
91  // transition
92 
93  // This function returns the number of possible radiative transitions for the atom with atomic number Z
94  // i.e. the number of shell in wich a vacancy can be filled with a radiative transition
95 
96  G4int NumberOfReachableShells(G4int Z)const ;
97
98// This function returns the number of possible NON-radiative transitions for the atom with atomic number Z
99// i.e. the number of shell in wich a vacancy can be filled by a NON-radiative transition
100
101  G4int NumberOfReachableAugerShells(G4int Z)const ;
102
103  // Gives the sum of the probabilities of radiative transition towards the
104  // shell whose index is shellIndex
105  G4double TotalRadiativeTransitionProbability(G4int Z, size_t shellIndex);
106 
107  // Gives the sum of the probabilities of non radiative transition from the
108  // shell whose index is shellIndex
109  G4double TotalNonRadiativeTransitionProbability(G4int Z, size_t shellIndex);
110   
111protected:
112
113  G4AtomicTransitionManager(G4int minZ = 1, G4int maxZ = 100, 
114                            G4int limitInfTable = 6, G4int limitSupTable=100 );
115  ~G4AtomicTransitionManager();
116
117private:
118  // Hide copy constructor and assignment operator
119  G4AtomicTransitionManager& operator=(const G4AtomicTransitionManager& right);
120  G4AtomicTransitionManager(const G4AtomicTransitionManager&);
121 
122  static G4AtomicTransitionManager* instance;
123 
124  // the first element of the map is the atomic number Z.
125  // the second element is a vector of G4AtomicShell*.
126  std::map<G4int,std::vector<G4AtomicShell*>,std::less<G4int> > shellTable;
127 
128  // the first element of the map is the atomic number Z.
129  // the second element is a vector of G4AtomicTransition*.
130  std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> > transitionTable;
131 
132  // since Augereffect data r stored as a table in G4AugerData, we have here a pointer to an element of that class itself.
133
134  G4AugerData* augerData;
135
136  // Minimum and maximum Z in EADL table containing identities and binding
137  // energies of shells
138  G4int zMin;
139  G4int zMax;
140 
141  // Minimum and maximum Z in EADL table containing identities, transition
142  // energies and transition probabilities of shells
143  G4int infTableLimit;
144  G4int supTableLimit;
145 
146 
147};
148
149#endif
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