Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
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G4EvaporationLevelDensityParameter.cc
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26//
27// $Id$
28//
29// Hadronic Process: Nuclear De-excitations
30// by V. Lara (Oct 1998)
31//
32
33
35#include "G4SystemOfUnits.hh"
37
38// Those values are from table 3 in
39// A.S. Iljinov et al. Nucl Phys A543 (1992) 517-557
40// Table 3. alpha, beta and gamma for Cameron Shell corrections
41// whithout collective effects. f-factor = 2.31.
42
43//JMQ 17-04-08 these are not used at present in G4Evaporation
44const G4double G4EvaporationLevelDensityParameter::ConstEvapLevelDensityParameter = 0.125/MeV;
45//const G4double G4EvaporationLevelDensityParameter::ConstEvapLevelDensityParameter= 0.0769231/MeV;
46const G4double G4EvaporationLevelDensityParameter::alpha = 0.072/MeV;
47const G4double G4EvaporationLevelDensityParameter::beta = 0.257/MeV;
48const G4double G4EvaporationLevelDensityParameter::gamma = 0.059/MeV;
49const G4double G4EvaporationLevelDensityParameter::Bs = 1.0;
50
53
56//JMQ (Apr .08) this is the method used in G4Evaporation
57{
58
59 //JMQ 25/04/08 a=A/10 according to original Gudima's prescription
60 G4double a=static_cast<G4double>(A)/10.;
61 return a;
62//
63
64// G4int N = A - Z;
65
66 // Asymptotic Level Density Parameter
67// G4double AsymptoticLDP = (alpha*static_cast<G4double>(A) + beta*std::pow(static_cast<G4double>(A),2./3.)*Bs)/MeV;
68
69 // Shape of the LDP U dependence
70// G4double exponent = -gamma*U;
71// G4double f = 1.;
72// if (exponent > -300.) f -= std::exp(exponent);
73
74 // Level Density Parameter
75// G4double a = AsymptoticLDP*(1. + ShellCorrection(Z,N)*f/U);
76// return a;
77}
78
double G4double
Definition: G4Types.hh:64
int G4int
Definition: G4Types.hh:66
G4double LevelDensityParameter(G4int A, G4int Z, G4double U) const