4.00900+ 3 8.93476+ 0 0 0 0 1 441 1451 1 0.0 + 0 0.0 + 0 0 0 0 0 441 1451 2 0.0 + 0 0.0 + 0 0 0 89 6 441 1451 3 4-BE- 9 JAERI EVAL-AUG84 K.SHIBATA 441 1451 4 JAERI-M 84-226 DIST-JUL91 441 1451 5 HISTORY 441 1451 6 84-08 REEVALUATED FOR JENDL-3 BY K.SHIBATA. 441 1451 7 DETAILS OF THE EVALUATION ARE GIVEN IN REF/1/. 441 1451 8 89-01 MODIFIED BY CONSIDERING NEUTRON EMISSION SPECTRA 441 1451 9 90-07 GAS-PRODUCTION DATA FILE WAS CREATED FROM JENDL-3 441 1451 10 BY T.NARITA AND T.NAKAGAWA 441 1451 11 441 1451 12 MF=1 GENERAL INFORMATION 441 1451 13 MT=451 DESCRIPTIVE DATA 441 1451 14 441 1451 15 MF=2 RESONANCE PARAMETERS 441 1451 16 MT=151 SCATTERING RADIUS ONLY 441 1451 17 441 1451 18 MF=3 NEUTRON CROSS SECTIONS 441 1451 19 MT=203 HYDROGEN PRODUCTION CROSS SECTION 441 1451 20 = MT103. 441 1451 21 MT=204 DEUTERIUM PRODUCTION CROSS SECTION 441 1451 22 = MT104. 441 1451 23 MT=205 TRITIUM PRODUCTION CROSS SECTION 441 1451 24 = MT105. 441 1451 25 MT=207 HE-4 PRODUCTION CROSS SECTION 441 1451 26 = MT024 + MT107 441 1451 27 441 1451 28 **** ORIGINAL DESCRIPTIVE DATA IN JENDL-3 ********************** 441 1451 29 441 1451 30 THE STATISTICAL MODEL CALCULATION WAS MADE FOR THE CHARGED 441 1451 31 PARTICLE EMISSION REACTIONS BY USING THE COMPUTER CODE 441 1451 32 ELIESE-3/2/. OPTICAL MODEL PARAMETERS FOR NEUTRON WERE 441 1451 33 TAKEN FROM AGEE AND ROSEN /3/. 441 1451 34 V = 49.3 - 0.33E, WS = 5.75 , VSO = 5.5 (MEV) 441 1451 35 R = 1.25 , RS = 1.25 , RSO = 1.25 (FM) 441 1451 36 A = 0.65 , B = 0.70 , ASO = 0.65 (FM) 441 1451 37 MT=24 (N,2N ALPHA) 441 1451 38 THIS IS THE CROSS SECTION FOR THE (N,A1) REACTION. THE 441 1451 39 1ST EXCITED LEVEL OF HE-6 DECAYS BY EMITTING 2 NEUTRONS. 441 1451 40 THE (N,A1) CROSS SECTION WAS CALCULATED WITH THE 441 1451 41 STATISTICAL MODEL. 441 1451 42 ALPHA POTENTIAL PARAMETERS ARE THE FOLLOWING /4/: 441 1451 43 V = 125.0 , WS = 15.0 , VSO = 0.0 (MEV) 441 1451 44 R = 1.56 , RS = 1.56 , RC = 1.22 (FM) 441 1451 45 A = 0.50 , B = 0.11 (FM) 441 1451 46 THE CROSS SECTION WAS NORMALIZED TO THE DATA OF 441 1451 47 PERROUD AND SELLEM /5/ AT 14 MEV. 441 1451 48 MT=103 (N,P) 441 1451 49 CALCULATED WITH THE STATISTICAL MODEL. 441 1451 50 PROTON POTENTIAL PARAMETERS ARE THE FOLLOWING /6/: 441 1451 51 V = 59.5 - 0.36E, WS = 12.0 + 0.07E, VSO = 4.9 (MEV) 441 1451 52 R = 1.24 , RS = 1.36 , RSO = 1.2 (FM) 441 1451 53 RC= 1.3 (FM) 441 1451 54 A = 0.63 , B = 0.35 , ASO = 0.31 (FM) 441 1451 55 THE CROSS SECTION WAS NORMALIZED TO THE EXPERIMENTAL DATA 441 1451 56 OF AUGUSTSON AND MENLOVE /7/, WHO MEASURED DELAYED 441 1451 57 NEUTROS, BY TAKING ACCOUNT OF THE BRANCHING RATIO 441 1451 58 OF 49.5% FOR LI-9 => BE-9* => 2A + N. 441 1451 59 MT=104 (N,D) 441 1451 60 BASED ON THE EXPERIMENTAL DATA OF SCOBEL /8/. 441 1451 61 MT=105 (N,T) 441 1451 62 SUM OF MT=740 AND 741. 441 1451 63 MT=107 (N,A0) 441 1451 64 BASED ON THE EXPERIMENTAL DATA /4,5,9,10,11,12/. 441 1451 65 MT=740, 741 (N,T0) AND (N,T1) 441 1451 66 CALCULATED WITH THE STATISTICAL MODEL. 441 1451 67 TRITON POTENTIAL PARAMETERS ARE THE FOLLOWING /13/: 441 1451 68 V = 140.0 , WS = 7.5 , VSO = 6.0 (MEV) 441 1451 69 R = 1.20 , RS = 2.69 , RSO = 1.20 , RC = 1.30 (FM) 441 1451 70 A = 0.45 , B = 0.36 , ASO = 0.7 (FM) 441 1451 71 NORMALIZATION WAS TAKEN SO THAT THE TOTAL (N,T) CROSS 441 1451 72 SECTION MIGHT BE CONSISTENT WITH THE EXPERIMENTAL DATA 441 1451 73 OF BOEDY ET AL./14/ 441 1451 74 441 1451 75 REFERENCES 441 1451 76 1) SHIBATA, K.: JAERI-M 84-226 (1984). 441 1451 77 2) IGARASI, S.: JAERI 1224 (1972). 441 1451 78 3) AGEE, F.P. AND ROSEN, L.: LA-3538-MS (1966). 441 1451 79 4) SHIBATA, K. AND SHIRATO, S.: J. PHYS. SOC. JPN. 52 (1983) 3748 441 1451 80 5) PERROUD, J.P. AND SELLEM, CH.: NUCL. PHYS. A227 (1974) 330. 441 1451 81 6) VOTAVA, H.J. ET AL.: NUCL. PHYS. A204 (1973) 529. 441 1451 82 7) AUGUSTSON, R.H. AND MENLOVE, H.O.: NUCL. SCI. ENG. 54(1974)190 441 1451 83 8) SCOBEL, W.: Z. NATURFORSCH. A24 (1969) 289. 441 1451 84 9) BATTAT, M.E. AND RIBE, F.L.: NUCL. PHYS. 89 (1953) 80. 441 1451 85 10) STELSON, P.H. AND CAMPBELL, E.C.: NUCL. PHYS. 106 (1957) 1252. 441 1451 86 11) BASS, R. ET AL.: NUCL. PHYS. 23 (1961) 122. 441 1451 87 12) PAIC, G. ET AL.: NUCL. PHYS. A96 (1967) 476. 441 1451 88 13) LUEDECKE, H. ET AL.: NUCL. PHYS. A109 (1968) 676. 441 1451 89 14) BOEDY, Z.T. ET AL.: PROC. INT. CONF. NUCLEAR DATA FOR SCIENCE 441 1451 90 AND TECHNOLOGY, ANTWERP 1982, (1983), P.368. 441 1451 91 441 1451 92 1 451 98 1 441 1451 93 2 151 4 1 441 1451 94 3 203 6 1 441 1451 95 3 204 10 1 441 1451 96 3 205 7 1 441 1451 97 3 207 33 1 441 1451 98 441 1 0 99 441 0 0 100 4.00900+ 3 8.93476+ 0 0 0 1 0 441 2151 101 4.00900+ 3 1.00000+ 0 0 0 1 0 441 2151 102 0.0 + 0 0.0 + 0 0 0 0 0 441 2151 103 1.50000+ 0 4.00000- 1 0 0 0 0 441 2151 104 441 2 0 105 441 0 0 106 4.00900+ 3 8.93476+ 0 0 99 0 0 441 3203 107 0.0 + 0-1.28244+ 7 0 0 1 7 441 3203 108 7 2 0 0 0 0 441 3203 109 1.42597+ 7 0.0 + 0 1.50000+ 7 4.82851- 4 1.60000+ 7 7.43060- 4 441 3203 110 1.70000+ 7 8.89255- 4 1.80000+ 7 1.03914- 3 1.90000+ 7 1.18005- 3 441 3203 111 2.00000+ 7 1.28236- 3 441 3203 112 441 3 0 113 4.00900+ 3 8.93476+ 0 0 99 0 0 441 3204 114 0.0 + 0-1.46635+ 7 0 0 1 21 441 3204 115 21 2 0 0 0 0 441 3204 116 1.63047+ 7 0.0 + 0 1.66081+ 7 1.66509- 4 1.66239+ 7 2.18032- 4 441 3204 117 1.66398+ 7 2.75960- 4 1.66714+ 7 4.10180- 4 1.67031+ 7 5.67395- 4 441 3204 118 1.67348+ 7 7.45989- 4 1.67981+ 7 1.16036- 3 1.68614+ 7 1.63979- 3 441 3204 119 1.69881+ 7 2.73926- 3 1.71148+ 7 3.93592- 3 1.72415+ 7 5.12124- 3 441 3204 120 1.73681+ 7 6.18669- 3 1.74948+ 7 7.02375- 3 1.76215+ 7 7.52394- 3 441 3204 121 1.78917+ 7 8.33005- 3 1.81620+ 7 9.29966- 3 1.84322+ 7 1.01506- 2 441 3204 122 1.87025+ 7 1.06007- 2 1.90149+ 7 1.08984- 2 2.00000+ 7 1.16690- 2 441 3204 123 441 3 0 124 4.00900+ 3 8.93476+ 0 0 99 0 0 441 3205 125 0.0 + 0-1.04387+ 7 0 0 1 11 441 3205 126 11 2 0 0 0 0 441 3205 127 1.16070+ 7 0.0 + 0 1.20000+ 7 6.98397- 4 1.21381+ 7 1.65404- 3 441 3205 128 1.30000+ 7 9.44131- 3 1.40000+ 7 1.83575- 2 1.50000+ 7 2.46176- 2 441 3205 129 1.60000+ 7 2.85511- 2 1.70000+ 7 2.99133- 2 1.80000+ 7 2.98976- 2 441 3205 130 1.90000+ 7 2.93066- 2 2.00000+ 7 2.84052- 2 441 3205 131 441 3 0 132 4.00900+ 3 8.93476+ 0 0 99 0 0 441 3207 133 0.0 + 0-6.02300+ 5 0 0 1 88 441 3207 134 88 2 0 0 0 0 441 3207 135 6.69700+ 5 0.0 + 0 8.41804+ 5 6.27232- 5 8.50249+ 5 6.38567- 5 441 3207 136 8.58695+ 5 6.63976- 5 8.67140+ 5 7.04797- 5 8.75585+ 5 7.62371- 5 441 3207 137 8.84030+ 5 8.38042- 5 8.92475+ 5 9.33150- 5 9.00920+ 5 1.04904- 4 441 3207 138 9.09365+ 5 1.18704- 4 9.26256+ 5 1.53480- 4 9.43145+ 5 1.98711- 4 441 3207 139 9.60035+ 5 2.55474- 4 9.76925+ 5 3.24841- 4 9.93815+ 5 4.07886- 4 441 3207 140 1.01070+ 6 5.05680- 4 1.02759+ 6 6.19299- 4 1.04449+ 6 7.49814- 4 441 3207 141 1.06138+ 6 8.98313- 4 1.08249+ 6 1.12191- 3 1.10360+ 6 1.39743- 3 441 3207 142 1.12471+ 6 1.72377- 3 1.14583+ 6 2.09991- 3 1.18805+ 6 2.99718- 3 441 3207 143 1.23028+ 6 4.08070- 3 1.27250+ 6 5.34185- 3 1.31473+ 6 6.77211- 3 441 3207 144 1.39918+ 6 1.01055- 2 1.48363+ 6 1.40124- 2 1.56808+ 6 1.84241- 2 441 3207 145 1.73698+ 6 2.84880- 2 1.74940+ 6 2.92556- 2 1.90588+ 6 3.89263- 2 441 3207 146 2.07478+ 6 4.92096- 2 2.24369+ 6 6.00503- 2 2.41259+ 6 7.21609- 2 441 3207 147 2.54771+ 6 8.33578- 2 2.67140+ 6 9.33032- 2 2.68283+ 6 9.42275- 2 441 3207 148 2.81795+ 6 1.01891- 1 2.95307+ 6 1.03362- 1 3.00000+ 6 1.02497- 1 441 3207 149 3.12197+ 6 1.03547- 1 3.29087+ 6 1.05457- 1 3.45978+ 6 1.08098- 1 441 3207 150 3.62868+ 6 1.11745- 1 3.89892+ 6 1.14606- 1 4.00000+ 6 1.13824- 1 441 3207 151 4.16916+ 6 1.09498- 1 4.43940+ 6 1.02000- 1 4.57453+ 6 9.93942- 2 441 3207 152 4.70965+ 6 9.82785- 2 5.00000+ 6 9.78028- 2 5.14879+ 6 9.50524- 2 441 3207 153 5.58793+ 6 8.65733- 2 6.00000+ 6 7.80647- 2 6.02708+ 6 7.77584- 2 441 3207 154 6.46622+ 6 7.19762- 2 6.83780+ 6 6.79959- 2 7.00000+ 6 6.71876- 2 441 3207 155 7.20939+ 6 6.53538- 2 7.58097+ 6 6.34569- 2 7.95255+ 6 6.21460- 2 441 3207 156 8.00000+ 6 6.19564- 2 9.00000+ 6 5.30119- 2 9.03352+ 6 5.27827- 2 441 3207 157 1.00000+ 7 4.52188- 2 1.01145+ 7 4.46284- 2 1.10000+ 7 3.93772- 2 441 3207 158 1.11955+ 7 3.87158- 2 1.20000+ 7 3.55436- 2 1.22764+ 7 3.45558- 2 441 3207 159 1.27493+ 7 3.29703- 2 1.30000+ 7 3.23301- 2 1.32223+ 7 3.09612- 2 441 3207 160 1.36952+ 7 2.83838- 2 1.40000+ 7 2.69110- 2 1.41681+ 7 2.60433- 2 441 3207 161 1.46410+ 7 2.38522- 2 1.50000+ 7 2.23462- 2 1.51140+ 7 2.19378- 2 441 3207 162 1.60000+ 7 1.91859- 2 1.60598+ 7 1.90255- 2 1.70000+ 7 1.68089- 2 441 3207 163 1.79515+ 7 1.49127- 2 1.80000+ 7 1.48351- 2 1.90000+ 7 1.36578- 2 441 3207 164 2.00000+ 7 1.28345- 2 441 3207 165 441 3 0 166 441 0 0 167 0 0 0 168 -1 0 0 0