2.50550+ 4 5.44661+ 1 0 0 0 12541 1451 1 0.0 + 0 0.0 + 0 0 0 0 02541 1451 2 0.0 + 0 0.0 + 0 0 0 108 72541 1451 3 25-MN- 55 JAERI,MAPI EVAL-MAR87 K.SHIBATA,T.HOJUYAMA 2541 1451 4 DIST-JUL91 2541 1451 5 HISTORY 2541 1451 6 87-03 RESONANCE PARAMETERS WERE EVALUATED BY T.HOJUYAMA (MAPI). 2541 1451 7 MULTISTEP HAUSER-FESHBACH CALCULATIONS WERE PERFORMED 2541 1451 8 BY K.SHIBATA (JAERI). 2541 1451 9 90-07 GAS-PRODUCTION DATA FILE WAS CREATED FROM JENDL-3 2541 1451 10 BY T.NARITA AND T.NAKAGAWA 2541 1451 11 2541 1451 12 MF=1 GENERAL INFORMATION 2541 1451 13 MT=451 DESCRIPTIVE DATA AND DICTIONARY 2541 1451 14 2541 1451 15 MF=2 RESONANCE PARAMETERS 2541 1451 16 MT=151 SCATTERING RADIUS ONLY 2541 1451 17 2541 1451 18 MF=3 NEUTRON CROSS SECTIONS 2541 1451 19 MT=203 HYDROGEN PRODUCTION CROSS SECTION 2541 1451 20 = MT028 + MT103 2541 1451 21 MT=204 DEUTERIUM PRODUCTION CROSS SECTION 2541 1451 22 = MT104 2541 1451 23 MT=205 TRITIUM PRODUCTION CROSS SECTION 2541 1451 24 = MT105 2541 1451 25 MT=206 HE-3 PRODUCTION CROSS SECTION 2541 1451 26 = MT106 2541 1451 27 MT=207 HE-4 PRODUCTION CROSS SECTION 2541 1451 28 = MT022 + MT107 2541 1451 29 2541 1451 30 **** ORIGINAL DESCRIPTIVE DATA IN JENDL-3 **********************2541 1451 31 2541 1451 32 MF=3 NEUTRON CROSS SECTIONS 2541 1451 33 STATISTICAL-MODEL CALCULATIONS WERE PERFORMED USING THE 2541 1451 34 TNG CODE /1/. THE PRECOMPOUND PROCESS WAS CONSIDERED 2541 1451 35 ABOVE 5 MEV. THE OPTICAL POTENTIAL PARAMETERS USED ARE AS2541 1451 36 FOLLOWS/2/ (IN THE UNITS OF MEV AND FM): 2541 1451 37 V = 49.747 - 0.4295*E - 0.0003*E**2 R0 = 1.287 A0 = 0.56 2541 1451 38 WS = 11.2 - 0.09*E RS = 1.345 AS = 0.47 2541 1451 39 VSO= 6.2 RSO= 1.120 ASO = 0.47 2541 1451 40 THE LEVEL SCHEME WAS TAKEN FROM REF./3/. 2541 1451 41 NO. ENERGY(MEV) SPIN-PARITY 2541 1451 42 G.S. 0.0 5/2 - 2541 1451 43 1. 0.126 7/2 - 2541 1451 44 2. 0.984 9/2 - 2541 1451 45 3. 1.290 1/2 - 2541 1451 46 4. 1.292 11/2 - 2541 1451 47 5. 1.293 1/2 - 2541 1451 48 6. 1.528 3/2 - 2541 1451 49 7. 1.884 7/2 - 2541 1451 50 8. 2.015 7/2 - 2541 1451 51 9. 2.198 7/2 - 2541 1451 52 10. 2.215 5/2 - 2541 1451 53 11. 2.252 3/2 - 2541 1451 54 12. 2.267 5/2 - 2541 1451 55 13. 2.312 13/2 - 2541 1451 56 14. 2.366 5/2 - 2541 1451 57 15. 2.398 9/2 + 2541 1451 58 16. 2.427 1/2 + 2541 1451 59 17. 2.563 3/2 - 2541 1451 60 18. 2.727 7/2 - 2541 1451 61 19. 2.753 5/2 - 2541 1451 62 20. 2.822 9/2 - 2541 1451 63 21. 2.824 5/2 - 2541 1451 64 22. 2.873 1/2 - 2541 1451 65 23. 2.954 3/2 - 2541 1451 66 24. 2.976 3/2 - 2541 1451 67 25. 2.992 7/2 - 2541 1451 68 26. 3.006 3/2 - 2541 1451 69 27. 3.036 11/2 - 2541 1451 70 28. 3.038 1/2 - 2541 1451 71 29. 3.040 3/2 + 2541 1451 72 2541 1451 73 LEVELS ABOVE 3.046 MEV WERE ASSUMED TO BE OVERLAPPING. 2541 1451 74 2541 1451 75 MT=22,28,103,107 (N,N'A),(N,N'P),(N,P) AND (N,A) CROSS SECTIONS 2541 1451 76 CALCULATED WITH TNG. GLOBAL OPTICAL-POTENTIAL PARAMETERS 2541 1451 77 WERE EMPLOYED FOR PROTONS AND ALPHA-PARTICLES /4,5/. 2541 1451 78 2541 1451 79 MT=104 (N,D) CROSS SECTION 2541 1451 80 THE EXCITATION FUNCTION OF THE (N,P) CROSS SECTION 2541 1451 81 CALCULATED WITH TNG WAS USED FOR THE (N,D) REACTION BY 2541 1451 82 SHIFTING THE THRESHOLD ENERGY. THE CROSS SECTIONS WERE 2541 1451 83 NORMALIZED TO THE EXPERIMENTAL DATUM AT 14.1 MEV /6/. 2541 1451 84 2541 1451 85 MT=105 (N,T) CROSS SECTION 2541 1451 86 THE EXCITATION FUNCTION OF THE (N,P) CROSS SECTION 2541 1451 87 CALCULATED WITH TNG WAS USED FOR THE (N,T) REACTION BY 2541 1451 88 SHIFTING THE THRESHOLD ENERGY. THE CROSS SECTIONS WERE 2541 1451 89 NORMALIZED TO THE EXPERIMENTAL DATUM AT 14.7 MEV /7/. 2541 1451 90 2541 1451 91 MT=106 (N,HE-3) CROSS SECTION 2541 1451 92 BASED ON THE EXPERIMENTAL DATA /8,9/. 2541 1451 93 2541 1451 94 REFERENCES 2541 1451 95 1) FU, C.Y.: "A CONSISTENT NUCLEAR MODEL FOR COMPOUND AND 2541 1451 96 PRECOMPOUND REACTIONS WITH CONSERVATION OF ANGULAR 2541 1451 97 MOMENTUM", ORNL/TM-7042 (1980). 2541 1451 98 2) FU, C.Y.: PRIVATE COMMUNICATION (1985). 2541 1451 99 3) ZHOU ENCHEN, HUO JUNDE, ZHOU CHUNMEI, LU XIANE AND 2541 1451 100 WANG LIZHENG: NUCL. DATA SHEETS, 44, 463 (1985). 2541 1451 101 4) PEREY, F.G.: PHYS. REV., 131, 745 (1963). 2541 1451 102 5) HUIZENGA, J.R. AND IGO, G.J.: NUCL. PHYS., 29, 462 (1962). 2541 1451 103 6) COLLI, L., IORI, I., MICHELETTI, S. AND PIGNANELLI, M.: 2541 1451 104 NUOVO. CIM., 21, 966 (1962). 2541 1451 105 7) SUDAR, S. AND CSIKAI, J.: NUCL. PHYS., A319, 157 (1979). 2541 1451 106 8) DIKSIC, M., STROHAL, P. AND SLAUS, I.: J. INORG. NUCL. 2541 1451 107 CHEM., 36, 477 (1974). 2541 1451 108 9) WU, C.H., WOELFLE, R. AND QAIM, S.M.: NUCL. PHYS., A329, 2541 1451 109 63 (1979). 2541 1451 110 2541 1451 111 1 451 118 12541 1451 112 2 151 4 12541 1451 113 3 203 13 12541 1451 114 3 204 9 12541 1451 115 3 205 7 12541 1451 116 3 206 6 12541 1451 117 3 207 12 12541 1451 118 2541 1 0 119 2541 0 0 120 2.50550+ 4 5.44661+ 1 0 0 1 02541 2151 121 2.50550+ 4 1.00000+ 0 0 0 1 02541 2151 122 0.0 + 0 0.0 + 0 0 0 0 02541 2151 123 2.50000+ 0 5.15000- 1 0 0 0 02541 2151 124 2541 2 0 125 2541 0 0 126 2.50550+ 4 5.44661+ 1 0 99 0 02541 3203 127 0.0 + 0-1.82120+ 6 0 0 1 292541 3203 128 29 2 0 0 0 02541 3203 129 1.85464+ 6 0.0 + 0 2.75000+ 6 6.15229- 8 3.00000+ 6 2.64180- 62541 3203 130 3.50000+ 6 5.96840- 5 4.00000+ 6 3.84940- 4 4.50000+ 6 1.37790- 32541 3203 131 5.00000+ 6 1.94200- 3 5.50000+ 6 5.71970- 3 6.00000+ 6 8.22390- 32541 3203 132 6.50000+ 6 1.03580- 2 7.00000+ 6 1.18100- 2 7.50000+ 6 1.31040- 22541 3203 133 8.00000+ 6 1.44430- 2 8.21602+ 6 1.51222- 2 8.50000+ 6 1.60150- 22541 3203 134 9.00000+ 6 1.80970- 2 9.50000+ 6 2.07828- 2 1.00000+ 7 2.43118- 22541 3203 135 1.10000+ 7 3.61696- 2 1.20000+ 7 4.84505- 2 1.30000+ 7 6.05556- 22541 3203 136 1.40000+ 7 7.39830- 2 1.45000+ 7 8.14370- 2 1.50000+ 7 8.92600- 22541 3203 137 1.60000+ 7 1.05962- 1 1.70000+ 7 1.23616- 1 1.80000+ 7 1.41845- 12541 3203 138 1.90000+ 7 1.59777- 1 2.00000+ 7 1.76619- 1 2541 3203 139 2541 3 0 140 2.50550+ 4 5.44661+ 1 0 99 0 02541 3204 141 0.0 + 0-5.84330+ 6 0 0 1 172541 3204 142 17 2 0 0 0 02541 3204 143 5.95058+ 6 0.0 + 0 8.00000+ 6 0.0 + 0 8.50000+ 6 2.57000- 42541 3204 144 9.00000+ 6 4.40000- 4 9.50000+ 6 7.80000- 4 1.00000+ 7 1.50000- 32541 3204 145 1.10000+ 7 2.16000- 3 1.20000+ 7 2.64000- 3 1.30000+ 7 3.37000- 32541 3204 146 1.40000+ 7 4.40000- 3 1.45000+ 7 4.90000- 3 1.50000+ 7 5.70000- 32541 3204 147 1.60000+ 7 7.38000- 3 1.70000+ 7 9.00000- 3 1.80000+ 7 1.02000- 22541 3204 148 1.90000+ 7 1.08000- 2 2.00000+ 7 1.09000- 2 2541 3204 149 2541 3 0 150 2.50550+ 4 5.44661+ 1 0 99 0 02541 3205 151 0.0 + 0-9.30500+ 6 0 0 1 122541 3205 152 12 2 0 0 0 02541 3205 153 9.47584+ 6 0.0 + 0 1.15000+ 7 0.0 + 0 1.20000+ 7 8.50000- 52541 3205 154 1.30000+ 7 3.60000- 4 1.40000+ 7 8.70000- 4 1.45000+ 7 1.01000- 32541 3205 155 1.50000+ 7 1.15000- 3 1.60000+ 7 1.43000- 3 1.70000+ 7 1.83000- 32541 3205 156 1.80000+ 7 2.38000- 3 1.90000+ 7 3.05000- 3 2.00000+ 7 3.95000- 32541 3205 157 2541 3 0 158 2.50550+ 4 5.44661+ 1 0 99 0 02541 3206 159 0.0 + 0-1.27070+ 7 0 0 1 92541 3206 160 9 2 0 0 0 02541 3206 161 1.29403+ 7 0.0 + 0 1.40000+ 7 0.0 + 0 1.45000+ 7 8.00000- 52541 3206 162 1.50000+ 7 1.10000- 4 1.60000+ 7 1.80000- 4 1.70000+ 7 2.50000- 42541 3206 163 1.80000+ 7 3.20000- 4 1.90000+ 7 3.90000- 4 2.00000+ 7 4.60000- 42541 3206 164 2541 3 0 165 2.50550+ 4 5.44661+ 1 0 99 0 02541 3207 166 0.0 + 0-6.24300+ 5 0 0 1 262541 3207 167 26 2 0 0 0 02541 3207 168 6.35762+ 5 0.0 + 0 4.00000+ 6 3.58730- 7 4.50000+ 6 5.04830- 62541 3207 169 5.00000+ 6 3.48640- 5 5.50000+ 6 1.58460- 4 6.00000+ 6 5.27270- 42541 3207 170 6.50000+ 6 1.36890- 3 7.00000+ 6 2.80790- 3 7.50000+ 6 4.78850- 32541 3207 171 8.00000+ 6 6.92070- 3 8.08150+ 6 7.24311- 3 8.50000+ 6 8.89887- 32541 3207 172 9.00000+ 6 1.07164- 2 9.50000+ 6 1.23596- 2 1.00000+ 7 1.38258- 22541 3207 173 1.10000+ 7 1.67242- 2 1.20000+ 7 1.99716- 2 1.30000+ 7 2.39305- 22541 3207 174 1.40000+ 7 2.86921- 2 1.45000+ 7 3.15048- 2 1.50000+ 7 3.45688- 22541 3207 175 1.60000+ 7 4.17634- 2 1.70000+ 7 4.96596- 2 1.80000+ 7 5.75070- 22541 3207 176 1.90000+ 7 6.48899- 2 2.00000+ 7 7.18300- 2 2541 3207 177 2541 3 0 178 2541 0 0 179 0 0 0 180 -1 0 0 0