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Toolkit for the simulation of the passage of particles through matter
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G4CameronGilbertShellCorrections.hh
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27// $Id$
28//
29// Hadronic Process: Nuclear De-excitations
30// by V. Lara
31
32#ifndef G4CameronGilbertShellCorrections_h
33#define G4CameronGilbertShellCorrections_h 1
34
36
37#include "globals.hh"
38
39//#define verbose 1
40
42{
43private:
44
46
47 static G4CameronGilbertShellCorrections* theInstance;
48
49
50public:
51
53
55
56 G4double GetShellCorrection(const G4int A, const G4int Z) const
57 {
58 return GetShellZ(Z) + GetShellN(A-Z);
59 }
60
61 G4double GetShellZ(const G4int Z) const
62 {
63 if (IsInTableThisZ(Z)) return ShellZTable[Z-ZTableMin]*CLHEP::MeV;
64 else {
65#ifdef verbose
66 G4cerr << "G4CameronGilbertShellCorrections: out of table for Z = " << Z << G4endl;
67#endif
68 return 0.0;
69 }
70 }
71
72 G4bool IsInTableThisZ(const G4int Z) const
73 {
74 if ( Z >= ZTableMin && Z <= ZTableMax ) return true;
75 else return false;
76 }
77
78
79 G4double GetShellN(const G4int N) const
80 {
81 if (IsInTableThisN(N)) return ShellNTable[N-NTableMin]*CLHEP::MeV;
82 else {
83#ifdef verbose
84 G4cerr << "G4CameronGilbertShellCorrections: out of table for N = " << N << G4endl;
85#endif
86 return 0.0;
87 }
88 }
89
90 G4bool IsInTableThisN(const G4int N) const
91 {
92 if ( N >= NTableMin && N <= NTableMax ) return true;
93 else return false;
94 }
95
96
97
98 enum { ZTableSize = 88, NTableSize = 140, ZTableMin = 11, ZTableMax = 98,
99 NTableMin = 11, NTableMax = 150 };
100
101private:
102
103
104
105 static const G4double ShellZTable[ZTableSize];
106
107 static const G4double ShellNTable[NTableSize];
108
109};
110#endif
double G4double
Definition: G4Types.hh:64
int G4int
Definition: G4Types.hh:66
bool G4bool
Definition: G4Types.hh:67
#define G4endl
Definition: G4ios.hh:52
G4DLLIMPORT std::ostream G4cerr
static G4CameronGilbertShellCorrections * GetInstance()
G4double GetShellCorrection(const G4int A, const G4int Z) const