Geant4
11.2.2
Toolkit for the simulation of the passage of particles through matter
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G4CookShellCorrections.hh
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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//
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// Hadronic Process: Nuclear De-excitations
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// by V. Lara
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//
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// Modified:
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// 21.03.2013 V.Ivanchenko redesigned and cleaned up
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#ifndef G4CookShellCorrections_h
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#define G4CookShellCorrections_h 1
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#include "
globals.hh
"
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class
G4CookShellCorrections
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{
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public
:
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explicit
G4CookShellCorrections
();
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inline
G4bool
GetShellCorrection
(
G4int
N
,
G4int
Z,
G4double
& result)
const
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{
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G4bool
res =
false
;
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if
(Z >=
ZTableMin
&& Z <= ZTableMax && N >=
NTableMin
&&
N
<=
NTableMax
) {
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result = ShellZTable[Z-
ZTableMin
] + ShellNTable[
N
-
NTableMin
];
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res =
true
;
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}
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return
res;
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}
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enum
{
ZTableSize
= 68,
NTableSize
= 118,
ZTableMin
= 28,
ZTableMax
= 95,
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NTableMin
= 33,
NTableMax
= 150 };
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private
:
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G4CookShellCorrections
(
const
G4CookShellCorrections
& right) =
delete
;
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const
G4CookShellCorrections
& operator=(
const
G4CookShellCorrections
& right) =
delete
;
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static
G4double
ShellZTable[
ZTableSize
];
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static
G4double
ShellNTable[
NTableSize
];
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};
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#endif
G4double
double G4double
Definition
G4Types.hh:83
G4bool
bool G4bool
Definition
G4Types.hh:86
G4int
int G4int
Definition
G4Types.hh:85
G4CookShellCorrections
Definition
G4CookShellCorrections.hh:39
G4CookShellCorrections::G4CookShellCorrections
G4CookShellCorrections()
Definition
G4CookShellCorrections.cc:68
G4CookShellCorrections::NTableMin
@ NTableMin
Definition
G4CookShellCorrections.hh:55
G4CookShellCorrections::NTableMax
@ NTableMax
Definition
G4CookShellCorrections.hh:55
G4CookShellCorrections::ZTableMax
@ ZTableMax
Definition
G4CookShellCorrections.hh:54
G4CookShellCorrections::NTableSize
@ NTableSize
Definition
G4CookShellCorrections.hh:54
G4CookShellCorrections::ZTableMin
@ ZTableMin
Definition
G4CookShellCorrections.hh:54
G4CookShellCorrections::ZTableSize
@ ZTableSize
Definition
G4CookShellCorrections.hh:54
G4CookShellCorrections::GetShellCorrection
G4bool GetShellCorrection(G4int N, G4int Z, G4double &result) const
Definition
G4CookShellCorrections.hh:44
N
#define N
Definition
crc32.c:57
globals.hh
geant4-v11.2.2
source
processes
hadronic
models
de_excitation
util
include
G4CookShellCorrections.hh
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