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G4InterpolationManager.cc
Go to the documentation of this file.
Or view
the newest version in sPHENIX GitHub for file G4InterpolationManager.cc
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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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// * use in resulting scientific publications, and indicate your *
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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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// neutron_hp -- source file
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// J.P. Wellisch, Nov-1996
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// A prototype of the low energy neutron transport model.
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//
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#include "
G4InterpolationManager.hh
"
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#include "
G4HadronicException.hh
"
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G4InterpolationScheme
G4InterpolationManager::MakeScheme
(
G4int
it
)
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{
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G4InterpolationScheme
result(
LINLIN
);
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switch
(it)
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{
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case
1:
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result =
HISTO
;
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break
;
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case
2:
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result =
LINLIN
;
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break
;
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case
3:
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result =
LINLOG
;
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break
;
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case
4:
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result =
LOGLIN
;
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break
;
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case
5:
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result =
LOGLOG
;
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break
;
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case
11:
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result =
CHISTO
;
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break
;
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case
12:
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result =
CLINLIN
;
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break
;
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case
13:
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result =
CLINLOG
;
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break
;
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case
14:
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result =
CLOGLIN
;
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break
;
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case
15:
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result =
CLOGLOG
;
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break
;
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case
21:
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result =
UHISTO
;
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break
;
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case
22:
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result =
ULINLIN
;
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break
;
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case
23:
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result =
ULINLOG
;
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break
;
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case
24:
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result =
ULOGLIN
;
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break
;
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case
25:
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result =
ULOGLOG
;
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break
;
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default
:
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throw
G4HadronicException
(__FILE__, __LINE__,
"G4InterpolationManager: unknown interpolation scheme"
);
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break
;
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}
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return
result;
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}
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void
G4InterpolationManager::AppendScheme
(
G4int
aPoint,
const
G4InterpolationScheme
& aScheme)
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{
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if
(aPoint!=
nEntries
)
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{
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G4cout
<<
"G4InterpolationManager::AppendScheme - "
<<aPoint<<
" "
<<
nEntries
<<
G4endl
;
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throw
G4HadronicException
(__FILE__, __LINE__,
"Wrong usage of G4InterpolationManager::AppendScheme"
);
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}
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if
(
nEntries
==0)
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{
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nEntries
= 1;
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nRanges
= 1;
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start
[0] = 0;
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range
[0] = 1;
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scheme
[0] = aScheme;
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}
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else
if
(aScheme==
scheme
[
nRanges
-1])
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{
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++
range
[
nRanges
-1];
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nEntries
++;
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}
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else
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{
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nEntries
++;
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nRanges
++;
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G4int
i;
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G4int
*
buffer
=
new
G4int
[
nRanges
];
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G4int
* buffer1 =
new
G4int
[
nRanges
];
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G4InterpolationScheme
* buff2 =
new
G4InterpolationScheme
[
nRanges
];
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for
(i=0; i<
nRanges
-1; i++)
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{
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buffer[i] =
start
[i];
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buffer1[i] =
range
[i];
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buff2[i] =
scheme
[i];
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}
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delete
[]
start
;
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delete
[]
range
;
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delete
[]
scheme
;
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start
=
buffer
;
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range
= buffer1;
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scheme
= buff2;
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start
[nRanges-1] =
start
[nRanges-2]+
range
[nRanges-2];
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range[nRanges-1] = 1;
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scheme
[nRanges-1] = aScheme;
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}
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}
geant4
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geant4-10.6-release
source
processes
hadronic
models
particle_hp
src
G4InterpolationManager.cc
Built by
Jin Huang
. updated:
Wed Jun 29 2022 17:25:48
using
1.8.2 with
ECCE GitHub integration