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Import Geant4 11.3.2 source tree

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This commit is contained in:
Gabriele Cosmo
2025-04-28 13:52:33 +02:00
parent df176550b3
commit 20a218bbe1
266 changed files with 8007 additions and 7819 deletions
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source/processes/hadronic/util/include/G4HadronicParameters.hh
+39 -5
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@@ -181,6 +181,29 @@ class G4HadronicParameters {
// Getter/Setter for the time threshold of radioactive decays
// (i.e. radioactive decays that happen later than this value are ignored).
inline G4bool IsBertiniAs11_2() const;
void SetBertiniAs11_2( G4bool val );
inline G4bool IsBertiniAngularEmissionsAs11_2() const;
void SetBertiniAngularEmissionsAs11_2( G4bool val );
inline G4bool IsBertiniNucleiModelAs11_2() const;
void SetBertiniNucleiModelAs11_2( G4bool val );
// Getter/Setter for the Bertini model behavior with respect to the
// Geant4 version 11.2.
// The first two methods "*BertiniAs11_2" refer to the overall behavior
// of the Bertini model - the one which should matter the most for the
// majority of applications.
// The methods "*BertiniAngularEmissionsAs11_2" refer to the angular
// distributions of the >= 4-body final state emissions.
// The last two methods "*BertiniNucleiModelAs11_2" refer to the
// modelling of nuclei.
// The overall behavior of Bertini with respect to the version Geant4
// version 11.2 depends on both the angular distributios of the
// >= 4-body final state emissions, and the modelling of nuclei.
// "True" in these methods means that the corresponding behavior of
// the Geant4 version 11.2 is retrieved;
// "False" means that the corresponding behavior of the Geant4 version
// 11.3 is retrieved.
private:
G4HadronicParameters();
@@ -226,6 +249,8 @@ class G4HadronicParameters {
G4bool fNeutronGeneral = false;
G4bool fChargeExchange = false;
G4bool fBinaryDebug = false;
G4bool fBertiniAngularEmissionsAs11_2 = false; // Keep the new G4 11.3 behavior
G4bool fBertiniNucleiModelAs11_2 = false; // Keep the new G4 11.3 behavior
G4String fTypeTablePT = "";
G4String fDirPARTICLEXS = "";
@@ -258,7 +283,6 @@ inline G4double G4HadronicParameters::GetMinEnergyINCLXX_Pbar() const {
inline G4double G4HadronicParameters::GetMaxEnergyINCLXX_Pbar() const {
return fMaxEnergyINCLXX_Pbar;
}
inline G4double G4HadronicParameters::EnergyThresholdForHeavyHadrons() const {
return fEnergyThresholdForHeavyHadrons;
@@ -360,13 +384,11 @@ inline const G4String& G4HadronicParameters::GetDirPARTICLEXS() const {
return fDirPARTICLEXS;
}
inline const G4String& G4HadronicParameters::GetPhysListDocDir() const
{
inline const G4String& G4HadronicParameters::GetPhysListDocDir() const {
return fPhysListDocDir;
}
inline const G4String& G4HadronicParameters::GetPhysListName() const
{
inline const G4String& G4HadronicParameters::GetPhysListName() const {
return fPhysListName;
}
@@ -378,4 +400,16 @@ inline G4double G4HadronicParameters::GetTimeThresholdForRadioactiveDecay() cons
return fTimeThresholdForRadioactiveDecays;
}
inline G4bool G4HadronicParameters::IsBertiniAs11_2() const {
return ( fBertiniAngularEmissionsAs11_2 && fBertiniNucleiModelAs11_2 );
}
inline G4bool G4HadronicParameters::IsBertiniAngularEmissionsAs11_2() const {
return fBertiniAngularEmissionsAs11_2;
}
inline G4bool G4HadronicParameters::IsBertiniNucleiModelAs11_2() const {
return fBertiniNucleiModelAs11_2;
}
#endif