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G4AtomicTransitionManager.hh
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26 //
27 // $Id: G4AtomicTransitionManager.hh,v 1.2 ????
28 //
29 // Authors: Elena Guardincerri (Elena.Guardincerri@ge.infn.it)
30 // Alfonso Mantero (Alfonso.Mantero@ge.infn.it)
31 //
32 // History:
33 // -----------
34 //
35 // 16 Sept 2001 EG Modified according to a design iteration in the
36 // LowEnergy category
37 //
38 // -------------------------------------------------------------------
39 
40 // Class description:
41 // Low Energy Electromagnetic Physics: create or fills and manages G4AtomicShell,
42 // G4FluoTransition, G4AugerTransition objects.
43 // Further documentation available from http://www.ge.infn.it/geant4/lowE
44 
45 // -------------------------------------------------------------------
46 
47 #ifndef G4AtomicTransitionManager_h
48 #define G4AtomicTransitionManager_h 1
49 
50 #include "G4ShellData.hh"
51 #include "G4FluoTransition.hh"
52 #include "G4AugerTransition.hh"
53 #include "G4AtomicShell.hh"
54 #include <vector>
55 #include "globals.hh"
56 
57 class G4AugerData;
58 
59 // This class is a singleton
61 
62 public:
63 
64  // The only way to get an instance of this class is to call the
65  // function Instance()
67 
68  // needs to be called once from other code before start of run
69  void Initialise();
70 
71  // Z is the atomic number of the element, shellIndex is the
72  // index (in EADL) of the shell
73  G4AtomicShell* Shell(G4int Z, size_t shellIndex) const;
74 
75  // Z is the atomic number of the element, shellIndex is the
76  // index (in EADL) of the final shell for the transition
77  // This function gives, upon Z and the Index of the initial shell where
78  // the vacancy is, the radiative transition that can happen (originating
79  // shell, energy, probability)
80  const G4FluoTransition* ReachableShell(G4int Z, size_t shellIndex) const;
81 
82  // This function gives, upon Z and the Index of the initial shell where
83  // the vacancy is, the NON-radiative transition that can happen with
84  // originating shell for the transition, and the data for the possible
85  // auger electrons emitted (originating vacancy, energy amnd probability)
86 
87  const G4AugerTransition* ReachableAugerShell(G4int Z, G4int shellIndex) const;
88 
89  // This function returns the number of shells of the element
90  // whose atomic number is Z
91  G4int NumberOfShells(G4int Z) const;
92 
93  // This function returns the number of those shells of the element
94  // whose atomic number is Z which are reachable through a radiative
95  // transition
97 
98  // This function returns the number of possible NON-radiative transitions
99  // for the atom with atomic number Z i.e. the number of shell in wich
100  // a vacancy can be filled by a NON-radiative transition
101 
103 
104  // Gives the sum of the probabilities of radiative transition towards the
105  // shell whose index is shellIndex
106  G4double
107  TotalRadiativeTransitionProbability(G4int Z, size_t shellIndex) const;
108 
109  // Gives the sum of the probabilities of non radiative transition from the
110  // shell whose index is shellIndex
111  G4double
112  TotalNonRadiativeTransitionProbability(G4int Z, size_t shellIndex) const;
113 
114  // Verbosity control
117 
118 private:
119 
121 
123 
124  // Hide copy constructor and assignment operator
127 
129 
130  // the first element of the map is the atomic number Z.
131  // the second element is a vector of G4AtomicShell*.
132  std::map<G4int,std::vector<G4AtomicShell*>,std::less<G4int> > shellTable;
133 
134  // the first element of the map is the atomic number Z.
135  // the second element is a vector of G4AtomicTransition*.
136  std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> > transitionTable;
137 
138  // since Augereffect data r stored as a table in G4AugerData, we have
139  // here a pointer to an element of that class itself.
141 
142  // Minimum and maximum Z in EADL table containing identities and binding
143  // energies of shells
146 
147  // Minimum and maximum Z in EADL table containing identities, transition
148  // energies and transition probabilities of shells
151 
153 
155 };
156 
157 #endif
G4double TotalNonRadiativeTransitionProbability(G4int Z, size_t shellIndex) const
G4double TotalRadiativeTransitionProbability(G4int Z, size_t shellIndex) const
G4AtomicShell * Shell(G4int Z, size_t shellIndex) const
std::map< G4int, std::vector< G4FluoTransition * >, std::less< G4int > > transitionTable
Float_t Z
double G4double
Definition: G4Types.hh:76
bool G4bool
Definition: G4Types.hh:79
G4int NumberOfReachableShells(G4int Z) const
int G4int
Definition: G4Types.hh:78
G4AtomicTransitionManager & operator=(const G4AtomicTransitionManager &right)
const G4FluoTransition * ReachableShell(G4int Z, size_t shellIndex) const
static G4AtomicTransitionManager * Instance()
static G4AtomicTransitionManager * instance
const G4AugerTransition * ReachableAugerShell(G4int Z, G4int shellIndex) const
std::map< G4int, std::vector< G4AtomicShell * >, std::less< G4int > > shellTable
G4int NumberOfReachableAugerShells(G4int Z) const