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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 // 57 58 #include <cmath> 59 #include "G4fissionEvent.hh" 60 61 G4int G4fissionEvent::G4SmpNuDistDataPu239_241_MC(G4double nubar) { 62 63 /* 64 Description 65 Sample Number of Neutrons from fission in Pu-239 and Pu-241 using 66 Zucker and Holden's tabulated data for Pu-239 67 The 11 P(nu) distributions are given as a function of nubar, 68 the average number of neutrons from induced fission for the 69 11 different energies (0 to 10 MeV), based on the Pu-239 data 70 from Zucker and Holden. 71 */ 72 73 /* 74 Input 75 nubar - average number of neutrons per fission 76 Output 77 G4SmpNuDistDataPu239_241_MC - sampled multiplicity 78 79 */ 80 81 static G4double Pu239nu [11] [9] = { 82 {.0108826, .0994916, .2748898, .3269196, .2046061, .0726834, .0097282, .0006301, .0001685}, 83 {.0084842, .0790030, .2536175, .3289870, .2328111, .0800161, .0155581, .0011760, .0003469}, 84 {.0062555, .0611921, .2265608, .3260637, .2588354, .0956070, .0224705, .0025946, .0005205}, 85 {.0045860, .0477879, .1983002, .3184667, .2792811, .1158950, .0301128, .0048471, .0007233}, 86 {.0032908, .0374390, .1704196, .3071862, .2948565, .1392594, .0386738, .0078701, .0010046}, 87 {.0022750, .0291416, .1437645, .2928006, .3063902, .1641647, .0484343, .0116151, .0014149}, 88 {.0014893, .0222369, .1190439, .2756297, .3144908, .1892897, .0597353, .0160828, .0029917}, 89 {.0009061, .0163528, .0968110, .2558524, .3194566, .2134888, .0729739, .0213339, .0020017}, 90 {.0004647, .0113283, .0775201, .2335926, .3213289, .2356614, .0886183, .0274895, .0039531}, 91 {.0002800, .0071460, .0615577, .2089810, .3200121, .2545846, .1072344, .0347255, .0054786}, 92 {.0002064, .0038856, .0492548, .1822078, .3154159, .2687282, .1295143, .0432654, .0075217} 93 }; 94 static G4double Pu239nubar [11] = { 95 2.8760000, 96 3.0088800, 97 3.1628300, 98 3.3167800, 99 3.4707300, 100 3.6246800, 101 3.7786300, 102 3.9325800, 103 4.0865300, 104 4.2404900, 105 4.3944400 106 }; 107 G4double fraction, r, cum; 108 G4int engind, nu; 109 110 /* 111 Check if nubar is within the range of experimental values 112 */ 113 if(nubar >= Pu239nubar[0] && nubar <= Pu239nubar[10]) { 114 /* 115 Use Zucker and Holden Data 116 */ 117 engind = 1; 118 while (nubar > Pu239nubar[engind]){ engind++;} 119 // Loop checking, 11.03.2015, T. Koi 120 fraction = (nubar-Pu239nubar[engind-1])/(Pu239nubar[engind]-Pu239nubar[engind-1]); 121 if(fisslibrng() > fraction) engind--; 122 123 r = fisslibrng(); 124 nu = 0; 125 cum = Pu239nu[engind][0]; 126 while (r > cum && nu < 8){ 127 // Loop checking, 11.03.2015, T. Koi 128 nu++; 129 cum += Pu239nu[engind][nu]; 130 } 131 return nu; 132 } else { 133 /* 134 Use Terrell's formula 135 */ 136 return (G4int) G4SmpTerrell(nubar); 137 } 138 } 139