JENDL-3.3 Te-130 0 0 0 0
5.213000+4 1.287900+2 1 0 0 25255 1451 1
0.000000+0 1.000000+0 0 0 0 65255 1451 2
1.000000+0 2.000000+7 3 0 10 35255 1451 3
0.000000+0 0.000000+0 0 0 207 405255 1451 4
52-TE-130 JNDC EVAL-MAR90 JNDC FP NUCLEAR DATA W.G. 5255 1451 5
DIST-MAR02 REV2-FEB02 20020222 5255 1451 6
----JENDL-3.3 MATERIAL 5255 5255 1451 7
-----INCIDENT NEUTRON DATA 5255 1451 8
------ENDF-6 FORMAT 5255 1451 9
5255 1451 10
=========================================================== 5255 1451 11
JENDL-3.2 data were automatically transformed to JENDL-3.3. 5255 1451 12
Interpolation of spectra: 22 (unit base interpolation) 5255 1451 13
(3,251) deleted, T-matrix of (4,2) deleted, and others. 5255 1451 14
=========================================================== 5255 1451 15
5255 1451 16
HISTORY 5255 1451 17
90-03 NEW EVALUATION FOR JENDL-3 WAS COMPLETED BY JNDC FPND 5255 1451 18
W.G./1/ 5255 1451 19
5255 1451 20
MF = 1 GENERAL INFORMATION 5255 1451 21
MT=451 COMMENTS AND DICTIONARY 5255 1451 22
5255 1451 23
MF = 2 RESONANCE PARAMETERS 5255 1451 24
MT=151 RESOLVED AND UNRESOLVED RESONANCE PARAMETERS 5255 1451 25
RESOLVED RESONANCE REGION (MLBW FORMULA) : BELOW 30.5 KEV 5255 1451 26
RESONANCE PARAMETERS WERE MAINLY BASED ON MUGHABGHAB ET AL./2/5255 1451 27
SOME RADIATION WIDTHS WERE DERIVED FROM THE DATA OF CAPTURE 5255 1451 28
AREA AND NEUTRON WIDTH GIVEN BY MUGHABGHAB ET AL. NEUTRON 5255 1451 29
ORBITAL ANGULAR MOMENTUM L WAS ESTIMATED WITH A METHOD OF 5255 1451 30
BOLLINGER AND THOMAS/3/. AVERAGED RADIATION WIDTH WAS DEDUCED5255 1451 31
TO BE 107 MEV, AND APPLIED TO THE LEVELS WHOSE RADIATION WIDTH5255 1451 32
WAS UNKNOWN. THE SCATTERING RADIUS OF 7.4 FM WAS TAKEN FROM 5255 1451 33
MUGHABGHAB ET AL. A NEGATIVE RESONANCE WAS ADDED SO AS TO 5255 1451 34
REPRODUCE THE THERMAL CAPTURE CROSS SECTION GIVEN BY 5255 1451 35
MUGHABGHAB ET AL. 5255 1451 36
5255 1451 37
UNRESOLVED RESONANCE REGION : 30.5 KEV - 100 KEV 5255 1451 38
THE NEUTRON STRENGTH FUNCTION S0 WAS BASED ON THE COMPILATION 5255 1451 39
OF MUGHABGHAB ET AL., AND S1 AND S2 WERE CALCULATED WITH 5255 1451 40
OPTICAL MODEL CODE CASTHY/4/. THE OBSERVED LEVEL SPACING WAS 5255 1451 41
DETERMINED TO REPRODUCE THE CAPTURE CROSS SECTION CALCULATED 5255 1451 42
WITH CASTHY. THE EFFECTIVE SCATTERING RADIUS WAS OBTAINED 5255 1451 43
FROM FITTING TO THE CALCULATED TOTAL CROSS SECTION AT 100 KEV.5255 1451 44
THE RADIATION WIDTH GG WAS BASED ON THE SYSTEMATICS OF 5255 1451 45
MEASURED VALUES FOR NEIGHBORING NUCLIDES. 5255 1451 46
5255 1451 47
TYPICAL VALUES OF THE PARAMETERS AT 70 KEV: 5255 1451 48
S0 = 0.160E-4, S1 = 1.600E-4, S2 = 0.990E-4, SG = 0.157E-4, 5255 1451 49
GG = 0.130 EV, R = 6.013 FM. 5255 1451 50
5255 1451 51
CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS (BARNS) 5255 1451 52
2200 M/S RES. INTEG. 5255 1451 53
TOTAL 4.106 - 5255 1451 54
ELASTIC 3.836 - 5255 1451 55
CAPTURE 0.2700 0.285 5255 1451 56
5255 1451 57
MF = 3 NEUTRON CROSS SECTIONS 5255 1451 58
BELOW 100 KEV, RESONANCE PARAMETERS WERE GIVEN. 5255 1451 59
ABOVE 100 KEV, THE SPHERICAL OPTICAL AND STATISTICAL MODEL 5255 1451 60
CALCULATION WAS PERFORMED WITH CASTHY, BY TAKING ACCOUNT OF 5255 1451 61
COMPETING REACTIONS, OF WHICH CROSS SECTIONS WERE CALCULATED 5255 1451 62
WITH PEGASUS/5/ STANDING ON A PREEQUILIBRIUM AND MULTI-STEP 5255 1451 63
EVAPORATION MODEL. THE OMP'S FOR NEUTRON GIVEN IN TABLE 1 WERE 5255 1451 64
DETERMINED TO REPRODUCE A SYSTEMATIC TREND OF THE TOTAL CROSS 5255 1451 65
SECTION BY CHANGING R0 AND RSO OF IIJIMA-KAWAI POTENTIAL/6/. 5255 1451 66
THE OMP'S FOR CHARGED PARTICLES ARE AS FOLLOWS: 5255 1451 67
PROTON = PEREY/7/ 5255 1451 68
ALPHA = HUIZENGA AND IGO/8/ 5255 1451 69
DEUTERON = LOHR AND HAEBERLI/9/ 5255 1451 70
HELIUM-3 AND TRITON = BECCHETTI AND GREENLEES/10/ 5255 1451 71
PARAMETERS FOR THE COMPOSITE LEVEL DENSITY FORMULA OF GILBERT 5255 1451 72
AND CAMERON/11/ WERE EVALUATED BY IIJIMA ET AL./12/ MORE 5255 1451 73
EXTENSIVE DETERMINATION AND MODIFICATION WERE MADE IN THE 5255 1451 74
PRESENT WORK. TABLE 2 SHOWS THE LEVEL DENSITY PARAMETERS USED 5255 1451 75
IN THE PRESENT CALCULATION. ENERGY DEPENDENCE OF SPIN CUT-OFF 5255 1451 76
PARAMETER IN THE ENERGY RANGE BELOW E-JOINT IS DUE TO GRUPPELAAR5255 1451 77
/13/. 5255 1451 78
5255 1451 79
MT = 1 TOTAL 5255 1451 80
SPHERICAL OPTICAL MODEL CALCULATION WAS ADOPTED. 5255 1451 81
5255 1451 82
MT = 2 ELASTIC SCATTERING 5255 1451 83
CALCULATED AS (TOTAL - SUM OF PARTIAL CROSS SECTIONS). 5255 1451 84
5255 1451 85
MT = 4, 51 - 91 INELASTIC SCATTERING 5255 1451 86
SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WAS 5255 1451 87
ADOPTED. THE LEVEL SCHEME WAS BASED ON EVALUATED NUCLEAR 5255 1451 88
STRUCTURE DATA FILE (1987 VERSION)/14/ AND NUCLEAR DATA 5255 1451 89
SHEETS/15/. 5255 1451 90
5255 1451 91
NO. ENERGY(MEV) SPIN-PARITY 5255 1451 92
GR. 0.0 0 + 5255 1451 93
1 0.8394 2 + 5255 1451 94
2 1.5880 2 + 5255 1451 95
3 1.6328 4 + 5255 1451 96
4 1.8150 6 + 5255 1451 97
5 1.9814 4 + 5255 1451 98
6 2.1008 5 - 5255 1451 99
7 2.1460 7 - 5255 1451 100
LEVELS ABOVE 2.191 MEV WERE ASSUMED TO BE OVERLAPPING. 5255 1451 101
5255 1451 102
MT = 102 CAPTURE 5255 1451 103
SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WITH 5255 1451 104
CASTHY WAS ADOPTED. DIRECT AND SEMI-DIRECT CAPTURE CROSS 5255 1451 105
SECTIONS WERE ESTIMATED ACCORDING TO THE PROCEDURE OF BENZI 5255 1451 106
AND REFFO/16/ AND NORMALIZED TO 1 MILLI-BARN AT 14 MEV. 5255 1451 107
5255 1451 108
THE GAMMA-RAY STRENGTH FUNCTION (1.41E-05) WAS ADJUSTED TO 5255 1451 109
REPRODUCE THE CAPTURE CROSS SECTION OF 11 MILLI-BARNS AT 60 5255 1451 110
KEV MEASURED BY BERGMAN AND ROMANOV/17/. 5255 1451 111
5255 1451 112
MT = 16 (N,2N) CROSS SECTION 5255 1451 113
MT = 17 (N,3N) CROSS SECTION 5255 1451 114
MT = 22 (N,N'A) CROSS SECTION 5255 1451 115
MT = 28 (N,N'P) CROSS SECTION 5255 1451 116
MT =103 (N,P) CROSS SECTION 5255 1451 117
MT =104 (N,D) CROSS SECTION 5255 1451 118
MT =105 (N,T) CROSS SECTION 5255 1451 119
MT =107 (N,ALPHA) CROSS SECTION 5255 1451 120
THESE REACTION CROSS SECTIONS WERE CALCULATED WITH THE 5255 1451 121
PREEQUILIBRIUM AND MULTI-STEP EVAPORATION MODEL CODE 5255 1451 122
PEGASUS. 5255 1451 123
5255 1451 124
THE KALBACH'S CONSTANT K (= 159.1) WAS ESTIMATED BY THE 5255 1451 125
FORMULA DERIVED FROM KIKUCHI-KAWAI'S FORMALISM/18/ AND LEVEL 5255 1451 126
DENSITY PARAMETERS. 5255 1451 127
5255 1451 128
FINALLY, THE (N,P) CROSS SECTIONS WAS NORMALIZED TO THE 5255 1451 129
FOLLOWING VALUE AT 14.5 MEV: 5255 1451 130
(N,P) 1.80 MB (RECOMMENDED BY FORREST/19/) 5255 1451 131
5255 1451 132
MT = 251 MU-BAR 5255 1451 133
CALCULATED WITH CASTHY. 5255 1451 134
5255 1451 135
MF = 4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 5255 1451 136
LEGENDRE POLYNOMIAL COEFFICIENTS FOR ANGULAR DISTRIBUTIONS ARE 5255 1451 137
GIVEN IN THE CENTER-OF-MASS SYSTEM FOR MT=2 AND DISCRETE INELAS-5255 1451 138
TIC LEVELS, AND IN THE LABORATORY SYSTEM FOR MT=91. THEY WERE 5255 1451 139
CALCULATED WITH CASTHY. FOR OTHER REACTIONS, ISOTROPIC DISTRI- 5255 1451 140
BUTIONS IN THE LABORATORY SYSTEM WERE ASSUMED. 5255 1451 141
5255 1451 142
MF = 5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS 5255 1451 143
ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS WERE CALCULATED WITH 5255 1451 144
PEGASUS FOR INELASTIC SCATTERING TO OVERLAPPING LEVELS AND FOR 5255 1451 145
OTHER NEUTRON EMITTING REACTIONS. 5255 1451 146
5255 1451 147
TABLE 1 NEUTRON OPTICAL POTENTIAL PARAMETERS 5255 1451 148
5255 1451 149
DEPTH (MEV) RADIUS(FM) DIFFUSENESS(FM) 5255 1451 150
---------------------- ------------ --------------- 5255 1451 151
V = 45.97-0.199E R0 = 6.481 A0 = 0.62 5255 1451 152
WS = 6.502 RS = 6.926 AS = 0.35 5255 1451 153
VSO= 7.0 RSO= 6.49 ASO= 0.62 5255 1451 154
THE FORM OF SURFACE ABSORPTION PART IS DER. WOODS-SAXON TYPE. 5255 1451 155
5255 1451 156
TABLE 2 LEVEL DENSITY PARAMETERS 5255 1451 157
5255 1451 158
NUCLIDE SYST A(1/MEV) T(MEV) C(1/MEV) EX(MEV) PAIRING 5255 1451 159
--------------------------------------------------------------- 5255 1451 160
50-SN-126 1.646E+01 6.270E-01 4.012E-01 6.778E+00 2.390E+00 5255 1451 161
50-SN-127 1.577E+01 6.140E-01 1.633E+00 5.075E+00 1.190E+00 5255 1451 162
50-SN-128 * 1.584E+01 5.822E-01 1.831E-01 5.627E+00 2.230E+00 5255 1451 163
50-SN-129 * 1.554E+01 5.798E-01 9.299E-01 4.443E+00 1.190E+00 5255 1451 164
5255 1451 165
51-SB-127 1.700E+01 5.120E-01 6.326E-01 3.902E+00 1.200E+00 5255 1451 166
51-SB-128 1.468E+01 5.600E-01 4.264E+00 2.658E+00 0.0 5255 1451 167
51-SB-129 1.596E+01 5.040E-01 5.308E-01 3.333E+00 1.040E+00 5255 1451 168
51-SB-130 1.566E+01 5.000E-01 3.630E+00 2.154E+00 0.0 5255 1451 169
5255 1451 170
52-TE-128 1.800E+01 6.090E-01 6.586E-01 7.010E+00 2.340E+00 5255 1451 171
52-TE-129 2.015E+01 5.350E-01 3.588E+00 5.141E+00 1.140E+00 5255 1451 172
52-TE-130 1.800E+01 5.470E-01 2.657E-01 5.735E+00 2.180E+00 5255 1451 173
52-TE-131 1.846E+01 5.360E-01 1.800E+00 4.651E+00 1.140E+00 5255 1451 174
--------------------------------------------------------------- 5255 1451 175
SYST: * = LDP'S WERE DETERMINED FROM SYSTEMATICS. 5255 1451 176
5255 1451 177
SPIN CUTOFF PARAMETERS WERE CALCULATED AS 0.146*SQRT(A)*A**(2/3).5255 1451 178
IN THE CASTHY CALCULATION, SPIN CUTOFF FACTORS AT 0 MEV WERE 5255 1451 179
ASSUMED TO BE 12.98 FOR TE-130 AND 5.0 FOR TE-131. 5255 1451 180
5255 1451 181
REFERENCES 5255 1451 182
1) KAWAI, M. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR SCIENCE5255 1451 183
AND TECHNOLOGY, MITO, P. 569 (1988). 5255 1451 184
2) MUGHABGHAB, S.F. ET AL.: "NEUTRON CROSS SECTIONS, VOL. I, 5255 1451 185
PART A", ACADEMIC PRESS (1981). 5255 1451 186
3) BOLLINGER, L.M. AND THOMAS, G.E.: PHYS. REV., 171,1293(1968). 5255 1451 187
4) IGARASI, S.: J. NUCL. SCI. TECHNOL., 12, 67 (1975). 5255 1451 188
5) IIJIMA, S. ET AL.: JAERI-M 87-025, P. 337 (1987). 5255 1451 189
6) IIJIMA, S. AND KAWAI, M.: J. NUCL. SCI. TECHNOL., 20, 77 5255 1451 190
(1983). 5255 1451 191
7) PEREY, F.G: PHYS. REV. 131, 745 (1963). 5255 1451 192
8) HUIZENGA, J.R. AND IGO, G.: NUCL. PHYS. 29, 462 (1962). 5255 1451 193
9) LOHR, J.M. AND HAEBERLI, W.: NUCL. PHYS. A232, 381 (1974). 5255 1451 194
10) BECCHETTI, F.D., JR. AND GREENLEES, G.W.: POLARIZATION 5255 1451 195
PHENOMENA IN NUCLEAR REACTIONS ((EDS) H.H. BARSHALL AND 5255 1451 196
W. HAEBERLI), P. 682, THE UNIVERSITY OF WISCONSIN PRESS. 5255 1451 197
(1971). 5255 1451 198
11) GILBERT, A. AND CAMERON, A.G.W.: CAN. J. PHYS., 43, 1446 5255 1451 199
(1965). 5255 1451 200
12) IIJIMA, S., ET AL.: J. NUCL. SCI. TECHNOL. 21, 10 (1984). 5255 1451 201
13) GRUPPELAAR, H.: ECN-13 (1977). 5255 1451 202
14) ENSDF: EVALUATED NUCLEAR STRUCTURE DATA FILE (JUNE 1987). 5255 1451 203
15) NUCLEAR DATA SHEETS, 13, 133 (1974). 5255 1451 204
16) BENZI, V. AND REFFO, G.: CCDN-NW/10 (1969). 5255 1451 205
17) BERGMAN, A.A. AND ROMANOV, S.A.: YADERNAYA FIZIKA, 20, 252 5255 1451 206
(1974). 5255 1451 207
18) KIKUCHI, K. AND KAWAI, M.: "NUCLEAR MATTER AND NUCLEAR 5255 1451 208
REACTIONS", NORTH HOLLAND (1968). 5255 1451 209
19) FORREST, R.A.: AERE-R 12419 (1986). 5255 1451 210
5255 1451 211
1 451 251 15255 1451 212
2 151 79 15255 1451 213
3 1 25 15255 1451 214
3 2 25 15255 1451 215
3 4 13 15255 1451 216
3 16 10 15255 1451 217
3 17 6 15255 1451 218
3 22 13 15255 1451 219
3 28 9 15255 1451 220
3 51 13 15255 1451 221
3 52 11 15255 1451 222
3 53 11 15255 1451 223
3 54 10 15255 1451 224
3 55 10 15255 1451 225
3 56 9 15255 1451 226
3 57 9 15255 1451 227
3 91 8 15255 1451 228
3 102 21 15255 1451 229
3 103 12 15255 1451 230
3 104 11 15255 1451 231
3 105 10 15255 1451 232
3 107 15 15255 1451 233
4 2 165 25255 1451 234
4 16 10 15255 1451 235
4 17 10 15255 1451 236
4 22 10 15255 1451 237
4 28 10 15255 1451 238
4 51 26 15255 1451 239
4 52 23 15255 1451 240
4 53 23 15255 1451 241
4 54 23 15255 1451 242
4 55 23 15255 1451 243
4 56 22 15255 1451 244
4 57 22 15255 1451 245
4 91 23 15255 1451 246
5 16 63 25255 1451 247
5 17 36 25255 1451 248
5 22 177 25255 1451 249
5 28 87 25255 1451 250
5 91 129 25255 1451 251
5255 1 099999
5255 0 0 0
5.213000+4 1.287900+2 0 0 1 05255 2151 1
5.213000+4 1.000000+0 0 0 2 05255 2151 2
1.000000-5 3.050000+4 1 2 0 05255 2151 3
0.000000+0 5.400000-1 0 0 2 05255 2151 4
1.287900+2 0.000000+0 0 0 30 55255 2151 5
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2.976000+4 5.000000-1 2.310700+1 2.300000+1 1.070000-1 0.000000+05255 2151 10
1.287900+2 0.000000+0 1 0 108 185255 2151 11
1.140500+3 5.000000-1 1.195000-1 9.500000-3 1.100000-1 0.000000+05255 2151 12
1.713000+3 5.000000-1 1.065000-1 4.250000-2 6.399990-2 0.000000+05255 2151 13
2.235000+3 5.000000-1 1.150000-1 7.999990-3 1.070000-1 0.000000+05255 2151 14
3.200000+3 5.000000-1 1.530000-1 5.100000-2 1.020000-1 0.000000+05255 2151 15
4.444000+3 5.000000-1 3.975000-1 3.475000-1 5.000000-2 0.000000+05255 2151 16
5.555000+3 5.000000-1 3.950000-1 2.350000-1 1.600000-1 0.000000+05255 2151 17
5.785000+3 5.000000-1 1.190000-1 1.200000-2 1.070000-1 0.000000+05255 2151 18
8.047000+3 5.000000-1 1.015000+0 9.080000-1 1.070000-1 0.000000+05255 2151 19
1.364400+4 5.000000-1 5.070000-1 4.000000-1 1.070000-1 0.000000+05255 2151 20
1.458000+4 5.000000-1 6.070000-1 5.000000-1 1.070000-1 0.000000+05255 2151 21
1.784300+4 5.000000-1 8.070000-1 7.000000-1 1.070000-1 0.000000+05255 2151 22
1.876400+4 5.000000-1 2.307000+0 2.200000+0 1.070000-1 0.000000+05255 2151 23
1.918300+4 5.000000-1 6.070000-1 5.000000-1 1.070000-1 0.000000+05255 2151 24
2.096000+4 5.000000-1 1.307000+0 1.200000+0 1.070000-1 0.000000+05255 2151 25
2.154000+4 5.000000-1 3.307000+0 3.200000+0 1.070000-1 0.000000+05255 2151 26
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3.017000+4 5.000000-1 5.117000+0 5.010000+0 1.070000-1 0.000000+05255 2151 29
3.050000+4 1.000000+5 2 2 0 05255 2151 30
0.000000+0 6.013000-1 0 0 3 05255 2151 31
1.287900+2 0.000000+0 0 0 1 05255 2151 32
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0.000000+0 0.000000+0 0.000000+0 1.000000+0 0.000000+0 0.000000+05255 2151 44
3.050000+4 8.700000+3 0.000000+0 1.392000+0 1.300000-1 0.000000+05255 2151 45
4.000000+4 8.700000+3 0.000000+0 1.392000+0 1.300000-1 0.000000+05255 2151 46
5.000000+4 8.700000+3 0.000000+0 1.392000+0 1.300000-1 0.000000+05255 2151 47
6.000000+4 8.661300+3 0.000000+0 1.385800+0 1.300000-1 0.000000+05255 2151 48
7.000000+4 8.265200+3 0.000000+0 1.322400+0 1.300000-1 0.000000+05255 2151 49
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5.000000+4 4.350000+3 0.000000+0 6.960000-1 1.300000-1 0.000000+05255 2151 56
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8.000000+4 4.009600+3 0.000000+0 6.415400-1 1.300000-1 0.000000+05255 2151 59
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1.287900+2 0.000000+0 2 0 2 05255 2151 61
1.500000+0 0.000000+0 5 0 48 75255 2151 62
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5.000000+4 4.350000+3 0.000000+0 4.306500-1 1.300000-1 0.000000+05255 2151 66
6.000000+4 4.330700+3 0.000000+0 4.287300-1 1.300000-1 0.000000+05255 2151 67
7.000000+4 4.132600+3 0.000000+0 4.091300-1 1.300000-1 0.000000+05255 2151 68
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4.000000+4 2.900000+3 0.000000+0 2.871000-1 1.300000-1 0.000000+05255 2151 74
5.000000+4 2.900000+3 0.000000+0 2.871000-1 1.300000-1 0.000000+05255 2151 75
6.000000+4 2.887100+3 0.000000+0 2.858200-1 1.300000-1 0.000000+05255 2151 76
7.000000+4 2.755100+3 0.000000+0 2.727500-1 1.300000-1 0.000000+05255 2151 77
8.000000+4 2.673100+3 0.000000+0 2.646400-1 1.300000-1 0.000000+05255 2151 78
1.000000+5 2.529600+3 0.000000+0 2.504300-1 1.300000-1 0.000000+05255 2151 79
5255 2 099999
5255 0 0 0
5.213000+4 1.287900+2 0 0 0 05255 3 1 1
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