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9.6.p02
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geant4_9_6_p02
source
processes
hadronic
models
lll_fission
include
G4LLNLFission.hh
Go to the documentation of this file.
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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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//
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// This software was developed by Lawrence Livermore National Laboratory.
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//
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// Redistribution and use in source and binary forms, with or without
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// modification, are permitted provided that the following conditions are met:
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//
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// 1. Redistributions of source code must retain the above copyright notice,
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// this list of conditions and the following disclaimer.
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// 2. Redistributions in binary form must reproduce the above copyright notice,
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// this list of conditions and the following disclaimer in the documentation
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// and/or other materials provided with the distribution.
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// 3. The name of the author may not be used to endorse or promote products
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// derived from this software without specific prior written permission.
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//
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// THIS SOFTWARE IS PROVIDED BY THE AUTHOR ``AS IS'' AND ANY EXPRESS OR IMPLIED
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// WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF
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// MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO
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// EVENT SHALL THE AUTHOR BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL,
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// SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO,
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// PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS;
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// OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY,
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// WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR
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// OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF
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// ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
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//
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// Copyright (c) 2006 The Regents of the University of California.
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// All rights reserved.
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// UCRL-CODE-224807
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//
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// $Id: G4LLNLFission.hh 69860 2013-05-16 14:39:02Z gcosmo $
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//
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//
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// This class is a copy of Fission.hh, made for use with Geant4.
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//
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extern
void
genspfissevt_
(
G4int
*isotope,
G4double
*time);
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/*
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* This function is called to trigger a spontaneous fission.
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* Multiple neutrons and photons are generated and stored
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* in a stack along with their energies, directions and
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* emission times.
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* The arguments of this function are
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* isotope: 94239 for Pu-239 for instance
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* time: the time of the spontaneous fission
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*/
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extern
void
genfissevt_
(
G4int
*isotope,
G4double
*time,
G4double
*nubar,
G4double
*eng);
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/*
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* This function is called to trigger a neutron-induced fission.
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* Multiple neutrons and photons are generated and stored
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* in a stack along with their energies, directions and
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* emission times. In addition to the arguments above, this
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* function needs
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* nubar: user-specified average number of neutrons emitted
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* per fission (e.g. as tabulated in the cross-section
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* libraries used by the particle transport code)
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* eng: energy of the neutron inducing fission
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*/
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extern
G4int
getnnu_
();
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/*
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* This function returns the number of neutrons emitted by the
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* fission, -1 if there is no neutron data for that isotope in
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* the fission library.
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*/
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extern
G4int
getpnu_
();
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/*
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* This function returns the number of photons emitted by the
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* fission, -1 if there is no photon data for that isotope in
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* the fission library.
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*/
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extern
G4double
getneng_
(
G4int
*
index
);
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/*
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* Given the index of the emitted neutron, this function returns
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* its energy, -1 if index isout of range.
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*/
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extern
G4double
getnvel_
(
G4int
*
index
);
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/*
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* Given the index of the emitted neutron, this function returns
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* the amplitude of its velocity, -1 if index is out of range.
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*/
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extern
G4double
getndircosu_
(
G4int
*
index
);
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extern
G4double
getndircosv_
(
G4int
*
index
);
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extern
G4double
getndircosw_
(
G4int
*
index
);
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/*
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* Given the index of the emitted neutron, this function returns
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* the direction cosines of its velocity vector on the x, y and z
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* axes.
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*/
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extern
G4double
getpeng_
(
G4int
*
index
);
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/*
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* Given the index of the emitted photon, this function returns
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* its energy, -1 if index is out of range.
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*/
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extern
G4double
getpvel_
(
G4int
*
index
);
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/*
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* Given the index of the emitted photon, this function returns
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* the amplitude of its velocity, -1 if index is out of range.
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*/
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extern
G4double
getpdircosu_
(
G4int
*
index
);
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extern
G4double
getpdircosv_
(
G4int
*
index
);
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extern
G4double
getpdircosw_
(
G4int
*
index
);
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/*
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* Given the index of the emitted photon, this function returns
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* the direction cosines of its velocity.
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*/
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extern
G4double
getnage_
(
G4int
*
index
);
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/*
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* Given the index of the emitted neutron, this function returns
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* its age, -1 if index is out of range.
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* This age will be different from the time specified
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* in generateFissionEvent and generateSpontaneousFissionEvent
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* for non-prompt neutrons, i.e. delayed neutrons.
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*/
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extern
G4double
getpage_
(
G4int
*
index
);
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/*
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* Given the index of the emitted photon, this function returns
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* its age, -1 of index is out of range.
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* This age will be different from the time specified
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* in generateFissionEvent and generateSpontaneousFissionEvent
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* for photons that are emitted by beta-decay of the fission
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* fragments.
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*/
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extern
void
setdelay_
(
G4int
*delay);
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/*
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* This function is called to enable delayed neutrons and photons
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* Input
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* delay:
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* 0 (default) for strictly prompt neutrons and
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* photons
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* 1 (n/a) for prompt neutrons, prompt and delayed
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* photons
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* 2 (n/a) for prompt and delayed neutrons, prompt
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* photons
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* 3 (n/a) for prompt and delayed neutrons, prompt
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* and delayed photons
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*/
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extern
void
setcorrel_
(
G4int
*correlation);
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/*
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* This function is called to set the type of neutron photon correlation
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* Input
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* correlation:
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* 0 (default) for no correlation between neutrons and
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* photons
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* 1 (n/a) for number correlation between neutrons and
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* photons
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* 2 (n/a) for number and energy correlation between
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* neutrons and photons
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*/
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extern
void
setnudist_
(
G4int
*nudist);
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/*
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* This function is called to set the data to be sampled for the neutron
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* number distributions in induced fissions
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* Input
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* nudist:
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* 0 to use the fit to the Zucker and Holden tabulated
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* P(nu) distributions as a function of energy for
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* U235, U238 and Pu239. Terrell for other isotopes.
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* 1 to use fits to the Zucker and Holden tabulated
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* P(nu) distribution as a function of energy for
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* U238 and Pu239, and a fit to the Zucker and Holden
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* data as well as the Gwin, Spencer and Ingle data
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* (at thermal energies) as a function of energy for
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* U235. Terrell for other isotopes.
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* 2 (default) to use the fit to the Zucker and Holden
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* tabulated P(nu) distributions as a function of nubar.
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* The U238 fit is used for the U232, U234, U236 and
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* U238 isotopes, the U235 fit for U233 and U235, the
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* Pu239 fit for Pu239 and Pu241. Terrell for other
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* isotopes.
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*/
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extern
void
setcf252_
(
G4int
*ndist,
G4int
*neng);
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/*
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* This function is called to set the data to be sampled for the
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* (a) Cf252 spontaneous fission number distribution, and
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* (b) Cf252 spontaneous fission neutron energy spectrum
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* Input
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* ndist:
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* 0 (default) to sample the number of neutrons from the
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* tabulated data measured by Spencer
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* 1 to sample the number of neutrons from Boldeman's data
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* neng:
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* 0 to sample the spontaneous fission neutron energy from
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* Mannhart corrected Maxwellian spectrum
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* 1 to sample the spontaneous fission neutron energy from
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* Madland-Nix theoretical spectrum
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* 2 to sample the spontaneous fission neutron energy from
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* the Froehner Watt spectrum
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*/
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extern
void
setrngf_
(
G4float
(*funcptr) (
void
));
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/*
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* This function sets the random number generator to the user-defined
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* one specified in the argument. If either setrngf_ or setrngd_ are
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* not specified, the default system call srand48 will be called.
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* Input
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* funcptr:
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* a random number generator function that returns a
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* variable of type G4float
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*/
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extern
void
setrngd_
(
G4double
(*funcptr) (
void
));
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/*
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* This function sets the random number generator to the user-defined
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* one specified in the argument. If either setrngf_ or setrngd_ are
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* not specified, the default system call srand48 will be called.
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* Input
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* funcptr:
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* a random number generator function that returns a
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* variable of type G4double
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*/
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// }
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