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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::G4SmpNuDistDataU232_234_236_238_MC(G4double nubar) { 62 63 /* 64 Description 65 Sample Number of Neutrons from fission in U-232, U-234, U-236, 66 and U-238 using Zucker and Holden's tabulated data for U-238 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 U-238 data 70 from Zucker and Holden. 71 */ 72 73 /* 74 Input 75 nubar - average number of neutrons per fission 76 Output 77 G4SmpNuDistDataU232_234_236_238_MC - sampled multiplicity 78 79 */ 80 81 static G4double U238nu [11] [9] = { 82 {.0396484, .2529541, .2939544, .2644470, .1111758, .0312261, .0059347, .0005436, .0001158}, 83 {.0299076, .2043215, .2995886, .2914889, .1301480, .0363119, .0073638, .0006947, .0001751}, 84 {.0226651, .1624020, .2957263, .3119098, .1528786, .0434233, .0097473, .0009318, .0003159}, 85 {.0170253, .1272992, .2840540, .3260192, .1779579, .0526575, .0130997, .0013467, .0005405}, 86 {.0124932, .0984797, .2661875, .3344938, .2040116, .0640468, .0173837, .0020308, .0008730}, 87 {.0088167, .0751744, .2436570, .3379711, .2297901, .0775971, .0225619, .0030689, .0013626}, 88 {.0058736, .0565985, .2179252, .3368863, .2541575, .0933127, .0286200, .0045431, .0031316}, 89 {.0035997, .0420460, .1904095, .3314575, .2760413, .1112075, .0355683, .0065387, .0031316}, 90 {.0019495, .0309087, .1625055, .3217392, .2943792, .1313074, .0434347, .0091474, .0046284}, 91 {.0008767, .0226587, .1356058, .3076919, .3080816, .1536446, .0522549, .0124682, .0067176}, 92 {.0003271, .0168184, .1111114, .2892434, .3160166, .1782484, .0620617, .0166066, .0095665} 93 }; 94 static G4double U238nubar [11] = { 95 2.2753781, 96 2.4305631, 97 2.5857481, 98 2.7409331, 99 2.8961181, 100 3.0513031, 101 3.2064881, 102 3.3616731, 103 3.5168581, 104 3.6720432, 105 3.8272281 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 >= U238nubar[0] && nubar <= U238nubar[10]) { 114 /* 115 Use Zucker and Holden Data 116 */ 117 engind = 1; 118 while (nubar > U238nubar[engind]){ engind++;} 119 // Loop checking, 11.03.2015, T. Koi 120 fraction = (nubar-U238nubar[engind-1])/(U238nubar[engind]-U238nubar[engind-1]); 121 if(fisslibrng() > fraction) engind--; 122 123 r = fisslibrng(); 124 nu = 0; 125 cum = U238nu[engind][0]; 126 while (r > cum && nu < 8){ 127 // Loop checking, 11.03.2015, T. Koi 128 nu++; 129 cum += U238nu[engind][nu]; 130 } 131 return nu; 132 } else { 133 /* 134 Use Terrell's formula 135 */ 136 return (G4int) G4SmpTerrell(nubar); 137 } 138 } 139