JEFF-3.2 Release - Neutron File March 2014 0 0 0 9.825400+4 2.519050+2 0 1 2 09867 1451 1 0.000000+0 1.000000+0 0 0 0 69867 1451 2 1.000000+0 2.000000+7 1 0 10 329867 1451 3 0.000000+0 0.000000+0 0 0 143 289867 1451 4 98-Cf-254 TIT EVAL-AUG87 N.TAKAGI 9867 1451 5 DIST-JAN09 20090105 9867 1451 6 ----JEFF32 MATERIAL 9867 9867 1451 7 -----INCIDENT NEUTRON DATA 9867 1451 8 ------ENDF-6 FORMAT 9867 1451 9 ***************************** JEFF-3.2 ***********************9867 1451 10 ** **9867 1451 11 ** Original data taken from: JEFF-3.1.1 **9867 1451 12 ** **9867 1451 13 ******************************************************************9867 1451 14 *************************** JEFF-3.1.1 *************************9867 1451 15 ** **9867 1451 16 ** Original data taken from: JEFF-3.1 **9867 1451 17 ** **9867 1451 18 ******************************************************************9867 1451 19 ***************************** JEFF-3.1 *************************9867 1451 20 ** **9867 1451 21 ** Original data taken from: JEFF-3.0 **9867 1451 22 ** **9867 1451 23 ******************************************************************9867 1451 24 9867 1451 25 ***************************** JEFF-3.0 ***********************9867 1451 26 9867 1451 27 DATA TAKEN FROM :- JENDL-3.2 (DIST-SEP89 REV-JUN94) 9867 1451 28 9867 1451 29 ******************************************************************9867 1451 30 HISTORY 9867 1451 31 87-08 NEW EVALUATION WAS MADE BY N. TAKAGI (TOKYO INSTITUTE OF 9867 1451 32 TECHNOLOGY, TIT) /1/. 9867 1451 33 94-06 JENDL-3.2. 9867 1451 34 NU-P, NU-D AND NU-TOTAL WERE MODIFIED. 9867 1451 35 COMPILED BY T.NAKAGAWA (NDC/JAERI) 9867 1451 36 9867 1451 37 ***** MODIFIED PARTS FOR JENDL-3.2 ******************** 9867 1451 38 (1,452), (1,455), (1,456) 9867 1451 39 *********************************************************** 9867 1451 40 9867 1451 41 9867 1451 42 MF=1 GENERAL INFORMATION 9867 1451 43 MT=451 COMMENT AND DICTIONARY 9867 1451 44 MT=452 NUMBER OF NEUTRONS PER FISSION 9867 1451 45 SUM OF NU-P NAD NU-D. 9867 1451 46 MT=455 DELAYED NEUTRONS PER FISSION 9867 1451 47 AVERAGE VALUES OF SYSTEMATICS BY TUTTLE/2/, BENEDETTI ET 9867 1451 48 AL./3/ AND WALDO ET AL./4/ DECAY CONSTANTS WERE ASSUMED 9867 1451 49 TO BE THE SAME AS THOSE OF CF-252 EVALUATED BY BRADY AND 9867 1451 50 ENGLAND/5/. 9867 1451 51 MT=456 PROMPT NEUTRONS PER FISSION 9867 1451 52 CALCULATED FROM THE SEMI-EMPIRICAL FORMULA OF HOWERTON/6/.9867 1451 53 A. Nouri (Data Bank) 9867 1451 54 use the same representation as for MT=452 9867 1451 55 (ENDF-6 recommendation): convert LNU=1 9867 1451 56 (polynomial (linear) representation) used in 9867 1451 57 JENDL-32 to tabular representation (LNU=2). 9867 1451 58 9867 1451 59 MF=2 RESONANCE PARAMETERS 9867 1451 60 MT=151 RESONANCE PARAMETERS 9867 1451 61 NO RESONANCE PARAMETERS WERE GIVEN. 9867 1451 62 9867 1451 63 2200-M/S CROSS SECTIONS AND RESONANCE INTEGRALS 9867 1451 64 2200 M/S VALUE RES. INT. 9867 1451 65 TOTAL 17.10 B - 9867 1451 66 ELASTIC 10.60 B - 9867 1451 67 FISSION 2.00 B 24.3 B 9867 1451 68 CAPTURE 4.50 B 6.5 B 9867 1451 69 9867 1451 70 MF=3 NEUTRON CROSS SECTIONS 9867 1451 71 MT=1 TOTAL CROSS SECTION 9867 1451 72 BELOW 120 EV, CALCULATED AS SUM OF MT'S = 2, 18 AND 102. 9867 1451 73 ABOVE 120 EV, OPTICAL MODEL CALCULATION WAS MADE WITH 9867 1451 74 CASTHY/7/. THE POTENTIAL PARAMETERS/8/ USED ARE AS 9867 1451 75 FOLLOWS, 9867 1451 76 V = 43.4 - 0.107*EN (MEV) 9867 1451 77 WS= 6.95 - 0.339*EN + 0.0531*EN**2 (MEV) 9867 1451 78 WV= 0 , VSO = 7.0 (MEV) 9867 1451 79 R = RSO = 1.282 , RS = 1.29 (FM) 9867 1451 80 A = ASO = 0.60 , B = 0.5 (FM) 9867 1451 81 9867 1451 82 MT=2 ELASTIC SCATTERING CROSS SECTION 9867 1451 83 BELOW 120 EV, THE CONSTANT CROSS SECTION OF 10.6 BARNS WAS9867 1451 84 ASSUMED, WHICH WAS THE SHAPE ELASTIC SCATTERING CROSS 9867 1451 85 SECTION CALCULATED WITH OPTICAL MODEL. ABOVE THIS ENERGY, 9867 1451 86 OPTICAL MODEL CALCULATION WAS ADOPTED. 9867 1451 87 9867 1451 88 MT=4,51,91 INELASTIC SCATTERING CROSS SECTIONS. 9867 1451 89 OPTICAL AND STATISTICAL MODEL CALCULATION WAS MADE WITH 9867 1451 90 CASTHY/7/. THE LEVEL SCHEME WAS TAKEN FROM REF./9/. 9867 1451 91 NO ENERGY(KEV) SPIN-PARITY 9867 1451 92 G.S. 0.0 0 + 9867 1451 93 1 45.0 2 + 9867 1451 94 LEVELS ABOVE 140 KEV WERE ASSUMED TO BE OVERLAPPING. 9867 1451 95 THE LEVEL DENSITY PARAMETERS WERE TAKEN FROM REF./10/. 9867 1451 96 9867 1451 97 MT=16,17,37 (N,2N), (N,3N) AND (N,4N) REACTION CROSS SECTIONS 9867 1451 98 CALCULATED WITH EVAPORATION MODEL. 9867 1451 99 9867 1451 100 MT=18 FISSION CROSS SECTION 9867 1451 101 THE THERMAL CROSS SECTION OF 2.0 BARNS WAS ESTIMATED FROM 9867 1451 102 THE RATIO OF FISSION AND CAPTURE CROSS SECTIONS AT 1 EV 9867 1451 103 AND MEASURED CAPTURE CROSS SECTION AT 0.0253 EV. THE FORM9867 1451 104 OF 1/V WAS ASSUMED BELOW 120 EV. FOR ENERGY ABOVE 120 EV,9867 1451 105 THE SHAPE OF CF-252 FISSION CROSS SECTION WAS ADOPTED AND 9867 1451 106 IT WAS NORMALIZED TO THE SYSTEMATICS OF BEHRENS AND 9867 1451 107 HOWERTON/11/. 9867 1451 108 9867 1451 109 MT=102 CAPTURE CROSS SECTION 9867 1451 110 MEASURED THERMAL CROSS SECTION OF 4.5 BARNS WAS TAKEN FROM9867 1451 111 REF./12/, AND 1/V FORM WAS ASSUMED BELOW 120 EV. ABOVE 9867 1451 112 120 EV, THE CROSS SECTION WAS CALCULATED WITH CASTHY. THE9867 1451 113 GAMMA-RAY STRENGTH FUNCTION WAS ESTIMATED FROM GAMMA-GAMMA9867 1451 114 = 0.040 EV AND LEVEL SPACING = 240 EV. 9867 1451 115 9867 1451 116 MT=251 MU-L 9867 1451 117 CALCULATED WITH CASTHY. 9867 1451 118 9867 1451 119 MF=4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 9867 1451 120 MT=2,51,91 CALCULATED WITH OPTICAL MODEL. 9867 1451 121 MT=16,17,18,37 ISOTROPIC IN THE LAB SYSTEM. 9867 1451 122 9867 1451 123 MF=5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS 9867 1451 124 MT=16,17,37,91 EVAPORATION SPECTRA. 9867 1451 125 OBTAINED FROM LEVEL DENSITY PARAMETERS. 9867 1451 126 9867 1451 127 MT=18 MAXWELLIAN FISSION SPECTRUM. 9867 1451 128 TEMPERATURE WAS ESTIMATED FROM Z**2/A DEPENDENCE/13/. 9867 1451 129 9867 1451 130 REFERENCES 9867 1451 131 1) TAKAGI N. ET AL.: J. NUCL. SCI. TECHNOL., 27, 853 (1990). 9867 1451 132 2) TUTTLE R.J.: INDC(NDS)-107/G+SPECIAL, P.29 (1979), 9867 1451 133 3) BENEDETTI G. ET AL.: NUCL. SCI. ENG., 80, 379 (1982). 9867 1451 134 4) WALDO R. ET AL.: PHYS. REV., C23, 1113 (1981). 9867 1451 135 5) BRADY M.C. AND ENGLAND T.R.: NUCL. SCI. ENG., 103, 129 (1989).9867 1451 136 6) HOWERTON R.J.: NUCL. SCI. ENG., 62, 438 (1977). 9867 1451 137 7) IGARASI S. AND FUKAHORI T.: JAERI 1321 (1991). 9867 1451 138 8) IGARASI S. AND NAKAGAWA T.: JAERI-M 8342 (1979). 9867 1451 139 9) SCHMORAK M.R.: NUCL. DATA SHEETS, 32, 87 (1981). 9867 1451 140 10) GILBERT A. AND CAMERON A.G.W.: CAN. J. PHYS., 43, 1446 (1965).9867 1451 141 11) BEHRENS J.W. AND HOWERTON R.J: NUCL. SCI. ENG., 65, 464(1978).9867 1451 142 12) MUGHABGHAB S.F.: "NEUTRON CROSS SECTIONS, VOL.1, NEUTRON 9867 1451 143 RESONANCE PARAMETERS AND THERMAL CROSS SECTIONS , PART B, 9867 1451 144 Z=61-100", ACADEMIC PRESS (1984). 9867 1451 145 13) SMITH A.B. ET AL.: ANL/NDM-50 (1979). 9867 1451 146 9867 1451 147 1 451 175 09867 1451 148 1 452 5 09867 1451 149 1 455 7 09867 1451 150 1 456 5 09867 1451 151 2 151 4 09867 1451 152 3 1 26 09867 1451 153 3 2 21 09867 1451 154 3 4 17 09867 1451 155 3 16 8 09867 1451 156 3 17 7 09867 1451 157 3 18 21 09867 1451 158 3 37 5 09867 1451 159 3 51 17 09867 1451 160 3 91 15 09867 1451 161 3 102 21 09867 1451 162 3 251 21 09867 1451 163 4 2 246 09867 1451 164 4 16 10 09867 1451 165 4 17 10 09867 1451 166 4 18 10 09867 1451 167 4 37 10 09867 1451 168 4 51 28 09867 1451 169 4 91 28 09867 1451 170 5 16 17 09867 1451 171 5 17 22 09867 1451 172 5 18 7 09867 1451 173 5 37 25 09867 1451 174 5 91 10 09867 1451 175 0.000000+0 0.000000+0 0 0 0 09867 1 099999 9.825400+4 2.519050+2 0 2 0 09867 1452 1 0.000000+0 0.000000+0 0 0 1 59867 1452 2 5 2 9867 1452 3 1.000000-5 3.850800+0 2.530000-2 3.850800+0 5.500000+6 5.192800+09867 1452 4 7.000000+6 5.552600+0 2.000000+7 8.724600+0 9867 1452 5 0.000000+0 0.000000+0 0 0 0 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