1.40000+ 4 2.78443+ 1 0 0 0 11440 1451 1 0.0 + 0 0.0 + 0 0 0 0 01440 1451 2 0.0 + 0 0.0 + 0 0 0 49 41440 1451 3 14-SI- 0 TIT,JAERI EVAL-MAR88 H.KITAZAWA,Y.HARIMA,T.FUKAHORI 1440 1451 4 DIST-JUL91 1440 1451 5 HISTORY 1440 1451 6 88-03 NEW EVALUATION WAS PERFORMED FOR JENDL-3 BY KITAZAWA, 1440 1451 7 HARIMA (TOKYO INSTITUTE OF TECH.) AND FUKAHORI (JAERI). 1440 1451 8 DETAILS ARE GIVEN IN REF./1/. 1440 1451 9 90-07 GAS-PRODUCTION DATA FILE WAS CREATED FROM JENDL-3 1440 1451 10 BY T.NARITA AND T.NAKAGAWA 1440 1451 11 1440 1451 12 MF=1 GENERAL INFORMATION 1440 1451 13 MT=451 DESCRIPTIVE DATA AND DICTIONARY 1440 1451 14 1440 1451 15 MF=2 RESONANCE PARAMETERS 1440 1451 16 MT=151 SCATTERING RADIUS ONLY 1440 1451 17 1440 1451 18 MF=3 NEUTRON CROSS SECTIONS 1440 1451 19 MT=203 HYDROGEN PRODUCTION CROSS SECTION 1440 1451 20 = MT028 + MT103 + MT111*2 1440 1451 21 MT=207 HE-4 PRODUCTION CROSS SECTION 1440 1451 22 = MT022 + MT107 1440 1451 23 1440 1451 24 **** ORIGINAL DESCRIPTIVE DATA IN JENDL-3 **********************1440 1451 25 1440 1451 26 MF=3 NEUTRON CROSS SECTIONS 1440 1451 27 MT=22 (N,NA) CROSS SECTIONS 1440 1451 28 CALCULATED BY THE STATISTICAL MODEL USING THE GNASH CODE./1,2/ 1440 1451 29 OPTICAL POTENTIAL FOR ALPHA-PARTICLES WAS DETERMINED, USING 1440 1451 30 THE DISPERSION THEORY./3/ 1440 1451 31 MT=28 (N,NP) CROSS SECTIONS 1440 1451 32 CALCULATED BY THE STATISTICAL MODEL USING THE GNASH CODE./1,2/ 1440 1451 33 MT=103 (N,P) CROSS SECTIONS 1440 1451 34 CALCULATED BY THE STATISTICAL MODEL USING THE GNASH CODE./1,2/ 1440 1451 35 THE IMAGINARY POTENTIAL STRENGTH OF THE PROTON SPHERICAL 1440 1451 36 OPTICAL MODEL WAS MODIFIED FROM THAT IN REF./1/ TO BE 1440 1451 37 W = 11.0 MEV BETWEEN 11 AND 20 MEV AND W = 8.8 + 0.2*E (MEV) 1440 1451 38 BELOW 11 MEV. 1440 1451 39 MT=107 (N,A) CROSS SECTIONS 1440 1451 40 CALCULATED BY THE STATISTICAL MODEL USING THE GNASH CODE./1,2/ 1440 1451 41 OPTICAL POTENTIAL FOR ALPHA-PARTICLES WAS DETERMINED, USING 1440 1451 42 THE DISPERSION THEORY./3/ 1440 1451 43 MT=111 (N,2P) CROSS SECTIONS 1440 1451 44 CALCULATED BY THE STATISTICAL MODEL USING THE GNASH CODE./1,2/ 1440 1451 45 1440 1451 46 REFERENCES 1440 1451 47 1) KITAZAWA H. ET AL.: PROC. INT. CONF. NUCLEAR DATA FOR 1440 1451 48 SCIENCE AND TECHNOLOGY, MITO, 1988, P.473, (1988). 1440 1451 49 2) YOUNG P.G. AND ARTHUR E.D.: LA-6947 (1977). 1440 1451 50 3) KITAZAWA H. ET AL.: UNPUBLISHED. 1440 1451 51 1440 1451 52 1 451 56 11440 1451 53 2 151 4 11440 1451 54 3 203 17 11440 1451 55 3 207 18 11440 1451 56 1440 1 0 57 1440 0 0 58 1.40000+ 4 2.78443+ 1 0 0 1 01440 2151 59 1.40000+ 4 1.00000+ 0 0 0 1 01440 2151 60 0.0 + 0 0.0 + 0 0 0 0 01440 2151 61 0.0 + 0 4.80000- 1 0 0 0 01440 2151 62 1440 2 0 63 1440 0 0 64 1.40000+ 4 2.78443+ 1 0 99 0 01440 3203 65 0.0 + 0-2.89783+ 6 0 0 1 421440 3203 66 42 2 0 0 0 01440 3203 67 3.00190+ 6 0.0 + 0 3.10000+ 6 0.0 + 0 3.99899+ 6 6.69967- 51440 3203 68 4.00000+ 6 6.70719- 5 5.00000+ 6 5.63391- 3 6.00000+ 6 7.29154- 21440 3203 69 7.00000+ 6 1.79136- 1 8.00000+ 6 2.27043- 1 8.01993+ 6 2.27729- 11440 3203 70 8.30000+ 6 2.37368- 1 8.50000+ 6 2.44253- 1 8.80000+ 6 2.53431- 11440 3203 71 9.00000+ 6 2.59530- 1 9.50000+ 6 2.67870- 1 1.00000+ 7 2.78135- 11440 3203 72 1.03000+ 7 2.82043- 1 1.10000+ 7 2.77408- 1 1.15000+ 7 2.66752- 11440 3203 73 1.20000+ 7 2.56062- 1 1.20030+ 7 2.56004- 1 1.25000+ 7 2.46673- 11440 3203 74 1.27630+ 7 2.46453- 1 1.28000+ 7 2.46422- 1 1.30000+ 7 2.46274- 11440 3203 75 1.35000+ 7 2.67149- 1 1.38637+ 7 2.93847- 1 1.38967+ 7 2.96270- 11440 3203 76 1.39000+ 7 2.96512- 1 1.39620+ 7 3.00867- 1 1.40000+ 7 3.03536- 11440 3203 77 1.45000+ 7 3.37629- 1 1.46000+ 7 3.43794- 1 1.50000+ 7 3.68569- 11440 3203 78 1.60000+ 7 4.09967- 1 1.66000+ 7 4.25278- 1 1.70000+ 7 4.35501- 11440 3203 79 1.78000+ 7 4.47125- 1 1.80000+ 7 4.52375- 1 1.90000+ 7 4.55765- 11440 3203 80 1.90038+ 7 4.55762- 1 1.98000+ 7 4.55267- 1 2.00000+ 7 4.55143- 11440 3203 81 1440 3 0 82 1.40000+ 4 2.78443+ 1 0 99 0 01440 3207 83 0.0 + 0-3.31500+ 4 0 0 1 441440 3207 84 44 2 0 0 0 01440 3207 85 3.43405+ 4 0.0 + 0 4.00000+ 4 0.0 + 0 1.00000+ 6 2.34950-111440 3207 86 2.00000+ 6 1.92765- 6 2.74849+ 6 5.69216- 5 3.00000+ 6 7.54009- 51440 3207 87 3.10000+ 6 1.23869- 4 4.00000+ 6 7.01779- 4 4.34118+ 6 1.06415- 31440 3207 88 4.40000+ 6 1.12663- 3 5.00000+ 6 1.76390- 3 6.00000+ 6 1.38741- 21440 3207 89 7.00000+ 6 7.91453- 2 8.00000+ 6 1.35386- 1 8.30000+ 6 1.45944- 11440 3207 90 8.50000+ 6 1.53002- 1 8.80000+ 6 1.61526- 1 9.00000+ 6 1.67243- 11440 3207 91 9.50000+ 6 1.89009- 1 1.00000+ 7 2.01530- 1 1.03000+ 7 2.08724- 11440 3207 92 1.03447+ 7 2.09458- 1 1.10000+ 7 2.20214- 1 1.10009+ 7 2.20222- 11440 3207 93 1.15000+ 7 2.24395- 1 1.15140+ 7 2.24510- 1 1.20000+ 7 2.28513- 11440 3207 94 1.25000+ 7 2.30717- 1 1.28000+ 7 2.30712- 1 1.30000+ 7 2.30751- 11440 3207 95 1.35000+ 7 2.28528- 1 1.39000+ 7 2.26684- 1 1.40000+ 7 2.25824- 11440 3207 96 1.45000+ 7 2.21489- 1 1.46000+ 7 2.20991- 1 1.50000+ 7 2.18969- 11440 3207 97 1.60000+ 7 2.21138- 1 1.66000+ 7 2.24660- 1 1.70000+ 7 2.27061- 11440 3207 98 1.78000+ 7 2.32308- 1 1.80000+ 7 2.31818- 1 1.90000+ 7 2.38952- 11440 3207 99 1.98000+ 7 2.43701- 1 2.00000+ 7 2.44905- 1 1440 3207 100 1440 3 0 101 1440 0 0 102 0 0 0 103 -1 0 0 0