Geant4  v4-10.4-release
 모두 클래스 네임스페이스들 파일들 함수 변수 타입정의 열거형 타입 열거형 멤버 Friends 매크로 그룹들 페이지들
G4SmpNuDistDataU233_235_MC.cc
이 파일의 문서화 페이지로 가기
1 //
2 // ********************************************************************
3 // * License and Disclaimer *
4 // * *
5 // * The Geant4 software is copyright of the Copyright Holders of *
6 // * the Geant4 Collaboration. It is provided under the terms and *
7 // * conditions of the Geant4 Software License, included in the file *
8 // * LICENSE and available at http://cern.ch/geant4/license . These *
9 // * include a list of copyright holders. *
10 // * *
11 // * Neither the authors of this software system, nor their employing *
12 // * institutes,nor the agencies providing financial support for this *
13 // * work make any representation or warranty, express or implied, *
14 // * regarding this software system or assume any liability for its *
15 // * use. Please see the license in the file LICENSE and URL above *
16 // * for the full disclaimer and the limitation of liability. *
17 // * *
18 // * This code implementation is the result of the scientific and *
19 // * technical work of the GEANT4 collaboration. *
20 // * By using, copying, modifying or distributing the software (or *
21 // * any work based on the software) you agree to acknowledge its *
22 // * use in resulting scientific publications, and indicate your *
23 // * acceptance of all terms of the Geant4 Software license. *
24 // ********************************************************************
25 //
26 //
27 // This software was developed by Lawrence Livermore National Laboratory.
28 //
29 // Redistribution and use in source and binary forms, with or without
30 // modification, are permitted provided that the following conditions are met:
31 //
32 // 1. Redistributions of source code must retain the above copyright notice,
33 // this list of conditions and the following disclaimer.
34 // 2. Redistributions in binary form must reproduce the above copyright notice,
35 // this list of conditions and the following disclaimer in the documentation
36 // and/or other materials provided with the distribution.
37 // 3. The name of the author may not be used to endorse or promote products
38 // derived from this software without specific prior written permission.
39 //
40 // THIS SOFTWARE IS PROVIDED BY THE AUTHOR ``AS IS'' AND ANY EXPRESS OR IMPLIED
41 // WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF
42 // MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO
43 // EVENT SHALL THE AUTHOR BE LIABLE FOR ANY DIRECT, INDIRECT, INCIDENTAL,
44 // SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING, BUT NOT LIMITED TO,
45 // PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES; LOSS OF USE, DATA, OR PROFITS;
46 // OR BUSINESS INTERRUPTION) HOWEVER CAUSED AND ON ANY THEORY OF LIABILITY,
47 // WHETHER IN CONTRACT, STRICT LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR
48 // OTHERWISE) ARISING IN ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF
49 // ADVISED OF THE POSSIBILITY OF SUCH DAMAGE.
50 //
51 // Copyright (c) 2006 The Regents of the University of California.
52 // All rights reserved.
53 // UCRL-CODE-224807
54 //
55 //
56 // $Id: G4SmpNuDistDataU233_235_MC.cc 68799 2013-04-05 13:29:46Z gcosmo $
57 //
58 
59 #include <cmath>
60 #include "G4fissionEvent.hh"
61 
63 
64 /*
65  Description
66  Sample Number of Neutrons from fission in U-233 and U-235 using
67  Zucker and Holden's tabulated data for U-235
68  The 11 P(nu) distributions are given as a function of nubar,
69  the average number of neutrons from induced fission for the
70  11 different energies (0 to 10 MeV), based on the U-235 data
71  from Zucker and Holden.
72 */
73 
74 /*
75  Input
76  nubar - average number of neutrons per fission
77  Output
78  G4SmpNuDistDataU233_235_MC - sampled multiplicity
79 
80 */
81 
82  static G4double U235nu [11] [8] = {
83  {.0317223, .1717071, .3361991, .3039695, .1269459, .0266793, .0026322, .0001449},
84  {.0237898, .1555525, .3216515, .3150433, .1444732, .0356013, .0034339, .0004546},
85  {.0183989, .1384891, .3062123, .3217566, .1628673, .0455972, .0055694, .0011093},
86  {.0141460, .1194839, .2883075, .3266568, .1836014, .0569113, .0089426, .0019504},
87  {.0115208, .1032624, .2716849, .3283426, .2021206, .0674456, .0128924, .0027307},
88  {.0078498, .0802010, .2456595, .3308175, .2291646, .0836912, .0187016, .0039148},
89  {.0046272, .0563321, .2132296, .3290407, .2599806, .1045974, .0265604, .0056322},
90  {.0024659, .0360957, .1788634, .3210507, .2892537, .1282576, .0360887, .0079244},
91  {.0012702, .0216090, .1472227, .3083032, .3123950, .1522540, .0462449, .0107009},
92  {.0007288, .0134879, .1231200, .2949390, .3258251, .1731879, .0551737, .0135376},
93  {.0004373, .0080115, .1002329, .2779283, .3342611, .1966100, .0650090, .0175099}
94  };
95  static G4double U235nubar [11] = {
96  2.4140000,
97  2.5236700,
98  2.6368200,
99  2.7623400,
100  2.8738400,
101  3.0386999,
102  3.2316099,
103  3.4272800,
104  3.6041900,
105  3.7395900,
106  3.8749800
107  };
108  G4double fraction, r, cum;
109  G4int engind, nu;
110 
111 /*
112  Check if nubar is within the range of experimental values
113 */
114  if(nubar >= U235nubar[0] && nubar <= U235nubar[10]) {
115 /*
116  Use Zucker and Holden Data
117 */
118  engind = 1;
119  while (nubar > U235nubar[engind]){ engind++;}
120  // Loop checking, 11.03.2015, T. Koi
121  fraction = (nubar-U235nubar[engind-1])/(U235nubar[engind]-U235nubar[engind-1]);
122  if(fisslibrng() > fraction) engind--;
123 
124  r = fisslibrng();
125  nu = 0;
126  cum = U235nu[engind][0];
127  while (r > cum && nu < 7){
128  // Loop checking, 11.03.2015, T. Koi
129  nu++;
130  cum += U235nu[engind][nu];
131  }
132  return nu;
133  } else {
134 /*
135  Use Terrell's formula
136 */
137  return (G4int) G4SmpTerrell(nubar);
138  }
139 }
double G4double
Definition: G4Types.hh:76
int G4int
Definition: G4Types.hh:78
G4int G4SmpNuDistDataU233_235_MC(G4double nubar)
G4double G4SmpTerrell(G4double nubar)
Definition: G4SmpTerrell.cc:69
static G4double fisslibrng(void)
Definition: G4rngc.cc:65