Geant4-11
G4EvaporationLevelDensityParameter.cc
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26//
27// Hadronic Process: Nuclear De-excitations
28// by V. Lara (Oct 1998)
29//
30// Modified:
31// 21.03.2013 V.Ivanchenko redesigned and comment out unused part
32
34#include "G4NuclearLevelData.hh"
35
37{
39}
40
42{}
43
46{
47 return fNucData->GetLevelDensity(Z, A, U);
48}
49
50/*
51#include "G4ShellCorrections.hh"
52#include "G4SystemOfUnits.hh"
53
54// Those values are from table 3 in
55// A.S. Iljinov et al. Nucl Phys A543 (1992) 517-557
56// Table 3. alpha, beta and gamma for Cameron Shell corrections
57// whithout collective effects. f-factor = 2.31.
58
59//JMQ 17-04-08 these are not used at present in G4Evaporation
60const G4double
61G4EvaporationLevelDensityParameter::ConstEvapLevelDensityParameter = 0.125/MeV;
62const G4double
63G4EvaporationLevelDensityParameter::ConstEvapLevelDensityParameter= 0.0769231/MeV;
64const G4double G4EvaporationLevelDensityParameter::alpha = 0.072/MeV;
65const G4double G4EvaporationLevelDensityParameter::beta = 0.257/MeV;
66const G4double G4EvaporationLevelDensityParameter::gamma = 0.059/MeV;
67const G4double G4EvaporationLevelDensityParameter::Bs = 1.0;
68
69// Asymptotic Level Density Parameter
70//G4double AsymptoticLDP = (alpha*A + beta*g4pow-Z23(A)*Bs)/MeV;
71
72// Shape of the LDP U dependence
73G4double exponent = -gamma*U;
74G4double f = 1.;
75if (exponent > -300.) f -= G4Exp(exponent);
76G4double a = AsymptoticLDP*(1. + ShellCorrection(Z,N)*f/U);
77return a;
78*/
double G4double
Definition: G4Types.hh:83
int G4int
Definition: G4Types.hh:85
const G4int Z[17]
const G4double A[17]
G4double LevelDensityParameter(G4int A, G4int Z, G4double U) const final
G4double GetLevelDensity(G4int Z, G4int A, G4double U)
static G4NuclearLevelData * GetInstance()