JENDL-3.3 Te-128 0 0 0 0
5.212800+4 1.268050+2 1 0 0 25249 1451 1
0.000000+0 1.000000+0 0 0 0 65249 1451 2
1.000000+0 2.000000+7 3 0 10 35249 1451 3
0.000000+0 0.000000+0 0 0 208 445249 1451 4
52-TE-128 JNDC EVAL-MAR90 JNDC FP NUCLEAR DATA W.G. 5249 1451 5
DIST-MAR02 REV2-FEB02 20020222 5249 1451 6
----JENDL-3.3 MATERIAL 5249 5249 1451 7
-----INCIDENT NEUTRON DATA 5249 1451 8
------ENDF-6 FORMAT 5249 1451 9
5249 1451 10
=========================================================== 5249 1451 11
JENDL-3.2 data were automatically transformed to JENDL-3.3. 5249 1451 12
Interpolation of spectra: 22 (unit base interpolation) 5249 1451 13
(3,251) deleted, T-matrix of (4,2) deleted, and others. 5249 1451 14
=========================================================== 5249 1451 15
5249 1451 16
HISTORY 5249 1451 17
84-10 EVALUATION FOR JENDL-2 WAS MADE BY JNDC FPND W.G./1/ 5249 1451 18
90-03 MODIFICATION FOR JENDL-3 WAS MADE/2/. 5249 1451 19
5249 1451 20
MF = 1 GENERAL INFORMATION 5249 1451 21
MT=451 COMMENTS AND DICTIONARY 5249 1451 22
5249 1451 23
MF = 2 RESONANCE PARAMETERS 5249 1451 24
MT=151 RESOLVED AND UNRESOLVED RESONANCE PARAMETERS 5249 1451 25
RESOLVED RESONANCE REGION (MLBW FORMULA) : BELOW 8 KEV 5249 1451 26
RESONANCE PARAMETERS WERE TAKEN FROM JENDL-2./1/ 5249 1451 27
EVALUATION FOR JENDL-2 WAS MADE BY KIKUCHI/3/. NEUTRON WIDTHS5249 1451 28
WERE ADOPTED FROM EXPERIMENTAL DATA OF TELLIER ET AL./4/, AND 5249 1451 29
RADIATIVE CAPTURE WIDTHS FROM CAPTURE AREAS MEASURED BY BROWNE5249 1451 30
AND BERMAN/5/. FOR THE RESONANCES ABOVE 7 KEV, THE AVERAGE 5249 1451 31
RADIATION WIDTH OF 0.048+-0.025 EV WAS ASSUMED. A NEGATIVE 5249 1451 32
RESONANCE WAS ADDED AT -600 EV SO AS TO REPRODUCE THE THERMAL 5249 1451 33
CAPTURE CROSS SECTION OF 0.215+-0.008 BARNS/6/. THE EFFECTIVE5249 1451 34
SCATTERING RADIUS OF 5.5 FM WAS TAKEN FROM REF./6/. 5249 1451 35
5249 1451 36
UNRESOLVED RESONANCE REGION : 8 KEV - 100 KEV 5249 1451 37
THE NEUTRON STRENGTH FUNCTION S0 WAS BASED ON THE COMPILATION 5249 1451 38
OF MUGHABGHAB ET AL./6/, AND S1 AND S2 WERE CALCULATED WITH 5249 1451 39
OPTICAL MODEL CODE CASTHY/7/. THE OBSERVED LEVEL SPACING WAS 5249 1451 40
DETERMINED TO REPRODUCE THE CAPTURE CROSS SECTION CALCULATED 5249 1451 41
WITH CASTHY. THE EFFECTIVE SCATTERING RADIUS WAS OBTAINED 5249 1451 42
FROM FITTING TO THE CALCULATED TOTAL CROSS SECTION AT 100 KEV.5249 1451 43
THE RADIATION WIDTH GG WAS BASED ON THE SYSTEMATICS OF 5249 1451 44
MEASURED VALUES FOR NEIGHBORING NUCLIDES. 5249 1451 45
5249 1451 46
TYPICAL VALUES OF THE PARAMETERS AT 70 KEV: 5249 1451 47
S0 = 0.250E-4, S1 = 1.700E-4, S2 = 1.000E-4, SG = 0.540E-4, 5249 1451 48
GG = 0.150 EV, R = 5.897 FM. 5249 1451 49
5249 1451 50
CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS (BARNS) 5249 1451 51
2200 M/S RES. INTEG. 5249 1451 52
TOTAL 4.313 - 5249 1451 53
ELASTIC 4.099 - 5249 1451 54
CAPTURE 0.2140 1.31 5249 1451 55
5249 1451 56
MF = 3 NEUTRON CROSS SECTIONS 5249 1451 57
BELOW 100 KEV, RESONANCE PARAMETERS WERE GIVEN. 5249 1451 58
ABOVE 100 KEV, THE SPHERICAL OPTICAL AND STATISTICAL MODEL 5249 1451 59
CALCULATION WAS PERFORMED WITH CASTHY, BY TAKING ACCOUNT OF 5249 1451 60
COMPETING REACTIONS, OF WHICH CROSS SECTIONS WERE CALCULATED 5249 1451 61
WITH PEGASUS/8/ STANDING ON A PREEQUILIBRIUM AND MULTI-STEP 5249 1451 62
EVAPORATION MODEL. THE OMP'S FOR NEUTRON GIVEN IN TABLE 1 WERE 5249 1451 63
DETERMINED TO REPRODUCE A SYSTEMATIC TREND OF THE TOTAL CROSS 5249 1451 64
SECTION BY CHANGING R0 AND RSO OF IIJIMA-KAWAI POTENTIAL/9/. 5249 1451 65
THE OMP'S FOR CHARGED PARTICLES ARE AS FOLLOWS: 5249 1451 66
PROTON = PEREY/10/ 5249 1451 67
ALPHA = HUIZENGA AND IGO/11/ 5249 1451 68
DEUTERON = LOHR AND HAEBERLI/12/ 5249 1451 69
HELIUM-3 AND TRITON = BECCHETTI AND GREENLEES/13/ 5249 1451 70
PARAMETERS FOR THE COMPOSITE LEVEL DENSITY FORMULA OF GILBERT 5249 1451 71
AND CAMERON/14/ WERE EVALUATED BY IIJIMA ET AL./15/ MORE 5249 1451 72
EXTENSIVE DETERMINATION AND MODIFICATION WERE MADE IN THE 5249 1451 73
PRESENT WORK. TABLE 2 SHOWS THE LEVEL DENSITY PARAMETERS USED 5249 1451 74
IN THE PRESENT CALCULATION. ENERGY DEPENDENCE OF SPIN CUT-OFF 5249 1451 75
PARAMETER IN THE ENERGY RANGE BELOW E-JOINT IS DUE TO GRUPPELAAR5249 1451 76
/16/. 5249 1451 77
5249 1451 78
MT = 1 TOTAL 5249 1451 79
SPHERICAL OPTICAL MODEL CALCULATION WAS ADOPTED. 5249 1451 80
5249 1451 81
MT = 2 ELASTIC SCATTERING 5249 1451 82
CALCULATED AS (TOTAL - SUM OF PARTIAL CROSS SECTIONS). 5249 1451 83
5249 1451 84
MT = 4, 51 - 91 INELASTIC SCATTERING 5249 1451 85
SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WAS 5249 1451 86
ADOPTED. THE LEVEL SCHEME WAS TAKEN FROM REF./17/. 5249 1451 87
5249 1451 88
NO. ENERGY(MEV) SPIN-PARITY 5249 1451 89
GR. 0.0 0 + 5249 1451 90
1 0.7432 2 + 5249 1451 91
2 1.4971 4 + 5249 1451 92
3 1.5232 2 + 5249 1451 93
4 1.8111 6 + 5249 1451 94
5 1.9722 2 + 5249 1451 95
6 1.9822 0 + 5249 1451 96
7 2.0300 4 + 5249 1451 97
8 2.1320 2 + 5249 1451 98
9 2.1335 5 - 5249 1451 99
LEVELS ABOVE 2.197 MEV WERE ASSUMED TO BE OVERLAPPING. 5249 1451 100
5249 1451 101
MT = 102 CAPTURE 5249 1451 102
SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WITH 5249 1451 103
CASTHY WAS ADOPTED. DIRECT AND SEMI-DIRECT CAPTURE CROSS 5249 1451 104
SECTIONS WERE ESTIMATED ACCORDING TO THE PROCEDURE OF BENZI 5249 1451 105
AND REFFO/18/ AND NORMALIZED TO 1 MILLI-BARN AT 14 MEV. 5249 1451 106
5249 1451 107
THE GAMMA-RAY STRENGTH FUNCTION (4.85E-05) WAS ADJUSTED TO 5249 1451 108
REPRODUCE THE CAPTURE CROSS SECTION OF 48 MILLI-BARNS AT 20 5249 1451 109
KEV MEASURED BY BERGMAN AND ROMANOV/19/. 5249 1451 110
5249 1451 111
MT = 16 (N,2N) CROSS SECTION 5249 1451 112
MT = 17 (N,3N) CROSS SECTION 5249 1451 113
MT = 22 (N,N'A) CROSS SECTION 5249 1451 114
MT = 28 (N,N'P) CROSS SECTION 5249 1451 115
MT =103 (N,P) CROSS SECTION 5249 1451 116
MT =104 (N,D) CROSS SECTION 5249 1451 117
MT =105 (N,T) CROSS SECTION 5249 1451 118
MT =107 (N,ALPHA) CROSS SECTION 5249 1451 119
THESE REACTION CROSS SECTIONS WERE CALCULATED WITH THE 5249 1451 120
PREEQUILIBRIUM AND MULTI-STEP EVAPORATION MODEL CODE PEGASUS. 5249 1451 121
5249 1451 122
THE KALBACH'S CONSTANT K (= 116.8) WAS ESTIMATED BY THE 5249 1451 123
FORMULA DERIVED FROM KIKUCHI-KAWAI'S FORMALISM/20/ AND LEVEL 5249 1451 124
DENSITY PARAMETERS. 5249 1451 125
5249 1451 126
FINALLY, THE (N,P) AND (N,ALPHA) CROSS SECTIONS WERE 5249 1451 127
NORMALIZED TO THE FOLLOWING VALUES AT 14.5 MEV: 5249 1451 128
(N,P) 2.40 MB (RECOMMENDED BY FORREST/21/) 5249 1451 129
(N,ALPHA) 0.95 MB (RECOMMENDED BY FORREST) 5249 1451 130
5249 1451 131
MT = 251 MU-BAR 5249 1451 132
CALCULATED WITH CASTHY/7/. 5249 1451 133
5249 1451 134
MF = 4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 5249 1451 135
LEGENDRE POLYNOMIAL COEFFICIENTS FOR ANGULAR DISTRIBUTIONS ARE 5249 1451 136
GIVEN IN THE CENTER-OF-MASS SYSTEM FOR MT=2 AND DISCRETE INELAS-5249 1451 137
TIC LEVELS, AND IN THE LABORATORY SYSTEM FOR MT=91. THEY WERE 5249 1451 138
CALCULATED WITH CASTHY. FOR OTHER REACTIONS, ISOTROPIC DISTRI- 5249 1451 139
BUTIONS IN THE LABORATORY SYSTEM WERE ASSUMED. 5249 1451 140
5249 1451 141
MF = 5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS 5249 1451 142
ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS WERE CALCULATED WITH 5249 1451 143
PEGASUS FOR INELASTIC SCATTERING TO OVERLAPPING LEVELS AND FOR 5249 1451 144
OTHER NEUTRON EMITTING REACTIONS. 5249 1451 145
5249 1451 146
TABLE 1 NEUTRON OPTICAL POTENTIAL PARAMETERS 5249 1451 147
5249 1451 148
DEPTH (MEV) RADIUS(FM) DIFFUSENESS(FM) 5249 1451 149
---------------------- ------------ --------------- 5249 1451 150
V = 45.97-0.199E R0 = 6.481 A0 = 0.62 5249 1451 151
WS = 6.502 RS = 6.926 AS = 0.35 5249 1451 152
VSO= 7.0 RSO= 6.49 ASO= 0.62 5249 1451 153
THE FORM OF SURFACE ABSORPTION PART IS DER. WOODS-SAXON TYPE. 5249 1451 154
5249 1451 155
TABLE 2 LEVEL DENSITY PARAMETERS 5249 1451 156
5249 1451 157
NUCLIDE A(1/MEV) T(MEV) C(1/MEV) EX(MEV) PAIRING 5249 1451 158
--------------------------------------------------------------- 5249 1451 159
50-SN-124 1.601E+01 6.160E-01 3.224E-01 6.294E+00 2.280E+00 5249 1451 160
50-SN-125 1.591E+01 6.210E-01 1.927E+00 5.249E+00 1.190E+00 5249 1451 161
50-SN-126 1.646E+01 6.270E-01 4.012E-01 6.778E+00 2.390E+00 5249 1451 162
50-SN-127 1.577E+01 6.140E-01 1.633E+00 5.075E+00 1.190E+00 5249 1451 163
5249 1451 164
51-SB-125 1.700E+01 5.120E-01 7.883E-01 3.792E+00 1.090E+00 5249 1451 165
51-SB-126 1.700E+01 5.250E-01 7.566E+00 2.897E+00 0.0 5249 1451 166
51-SB-127 1.700E+01 5.120E-01 6.326E-01 3.902E+00 1.200E+00 5249 1451 167
51-SB-128 1.468E+01 5.600E-01 4.264E+00 2.658E+00 0.0 5249 1451 168
5249 1451 169
52-TE-126 1.706E+01 6.100E-01 5.154E-01 6.554E+00 2.230E+00 5249 1451 170
52-TE-127 2.004E+01 5.380E-01 3.633E+00 5.165E+00 1.140E+00 5249 1451 171
52-TE-128 1.800E+01 6.090E-01 6.586E-01 7.010E+00 2.340E+00 5249 1451 172
52-TE-129 2.015E+01 5.350E-01 3.588E+00 5.141E+00 1.140E+00 5249 1451 173
--------------------------------------------------------------- 5249 1451 174
5249 1451 175
SPIN CUTOFF PARAMETERS WERE CALCULATED AS 0.146*SQRT(A)*A**(2/3).5249 1451 176
IN THE CASTHY CALCULATION, SPIN CUTOFF FACTORS AT 0 MEV WERE 5249 1451 177
ASSUMED TO BE 7.680 FOR TE-128 AND 5.913 FOR TE-129. 5249 1451 178
5249 1451 179
REFERENCES 5249 1451 180
1) AOKI, T. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR BASIC 5249 1451 181
AND APPLIED SCIENCE, SANTA FE., VOL. 2, P.1627 (1985). 5249 1451 182
2) KAWAI, M. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR SCIENCE5249 1451 183
AND TECHNOLOGY, MITO, P. 569 (1988). 5249 1451 184
3) KIKUCHI, Y. ET AL.: JAERI-M 86-030 (1986). 5249 1451 185
4) TELLIER, H., ET AL.: CEA-N-1268 (1970). 5249 1451 186
5) BROWNE, J.C., BERMAN, B.L.: PHYS. REV., C8, 2405 (1973). 5249 1451 187
6) MUGHABGHAB, S.F. ET AL.: "NEUTRON CROSS SECTIONS, VOL. I, 5249 1451 188
PART A", ACADEMIC PRESS (1981). 5249 1451 189
7) IGARASI, S.: J. NUCL. SCI. TECHNOL., 12, 67 (1975). 5249 1451 190
8) IIJIMA, S. ET AL.: JAERI-M 87-025, P. 337 (1987). 5249 1451 191
9) IIJIMA, S. AND KAWAI, M.: J. NUCL. SCI. TECHNOL., 20, 77 5249 1451 192
(1983). 5249 1451 193
10) PEREY, F.G: PHYS. REV. 131, 745 (1963). 5249 1451 194
11) HUIZENGA, J.R. AND IGO, G.: NUCL. PHYS. 29, 462 (1962). 5249 1451 195
12) LOHR, J.M. AND HAEBERLI, W.: NUCL. PHYS. A232, 381 (1974). 5249 1451 196
13) BECCHETTI, F.D., JR. AND GREENLEES, G.W.: POLARIZATION 5249 1451 197
PHENOMENA IN NUCLEAR REACTIONS ((EDS) H.H. BARSHALL AND 5249 1451 198
W. HAEBERLI), P. 682, THE UNIVERSITY OF WISCONSIN PRESS. 5249 1451 199
(1971). 5249 1451 200
14) GILBERT, A. AND CAMERON, A.G.W.: CAN. J. PHYS., 43, 1446 5249 1451 201
(1965). 5249 1451 202
15) IIJIMA, S., ET AL.: J. NUCL. SCI. TECHNOL. 21, 10 (1984). 5249 1451 203
16) GRUPPELAAR, H.: ECN-13 (1977). 5249 1451 204
17) MATSUMOTO, J.: PRIVATE COMMUNICATION (1981). 5249 1451 205
18) BENZI, V. AND REFFO, G.: CCDN-NW/10 (1969). 5249 1451 206
19) BERGMAN, A.A. AND ROMANOV, S.A.: YADERNAYA FIZIKA, 20, 252 5249 1451 207
(1974). 5249 1451 208
20) KIKUCHI, K. AND KAWAI, M.: "NUCLEAR MATTER AND NUCLEAR 5249 1451 209
REACTIONS", NORTH HOLLAND (1968). 5249 1451 210
21) FORREST, R.A.: AERE-R 12419 (1986). 5249 1451 211
5249 1451 212
1 451 256 15249 1451 213
2 151 116 15249 1451 214
3 1 25 15249 1451 215
3 2 25 15249 1451 216
3 4 14 15249 1451 217
3 16 10 15249 1451 218
3 17 6 15249 1451 219
3 22 13 15249 1451 220
3 28 9 15249 1451 221
3 51 14 15249 1451 222
3 52 12 15249 1451 223
3 53 11 15249 1451 224
3 54 11 15249 1451 225
3 55 10 15249 1451 226
3 56 10 15249 1451 227
3 57 9 15249 1451 228
3 58 9 15249 1451 229
3 59 9 15249 1451 230
3 91 8 15249 1451 231
3 102 20 15249 1451 232
3 103 13 15249 1451 233
3 104 11 15249 1451 234
3 105 10 15249 1451 235
3 107 15 15249 1451 236
4 2 171 25249 1451 237
4 16 10 15249 1451 238
4 17 10 15249 1451 239
4 22 10 15249 1451 240
4 28 10 15249 1451 241
4 51 26 15249 1451 242
4 52 23 15249 1451 243
4 53 23 15249 1451 244
4 54 23 15249 1451 245
4 55 23 15249 1451 246
4 56 23 15249 1451 247
4 57 23 15249 1451 248
4 58 23 15249 1451 249
4 59 22 15249 1451 250
4 91 23 15249 1451 251
5 16 65 25249 1451 252
5 17 34 25249 1451 253
5 22 199 25249 1451 254
5 28 89 25249 1451 255
5 91 129 25249 1451 256
5249 1 099999
5249 0 0 0
5.212800+4 1.268050+2 0 0 1 05249 2151 1
5.212800+4 1.000000+0 0 0 2 05249 2151 2
1.000000-5 8.000000+3 1 2 0 05249 2151 3
0.000000+0 5.500000-1 0 0 2 05249 2151 4
1.268050+2 0.000000+0 0 0 120 205249 2151 5
-6.000000+2 5.000000-1 2.512000+0 2.320000+0 1.920000-1 0.000000+05249 2151 6
3.481000+2 5.000000-1 4.824000-2 2.400000-4 4.800000-2 0.000000+05249 2151 7
4.240000+2 5.000000-1 9.000000-2 6.100000-2 2.900000-2 0.000000+05249 2151 8
1.459000+3 5.000000-1 1.590000-1 1.150000-1 4.400000-2 0.000000+05249 2151 9
1.837000+3 5.000000-1 6.370000-1 6.000000-1 3.700000-2 0.000000+05249 2151 10
2.971000+3 5.000000-1 1.990000+0 1.960000+0 3.000000-2 0.000000+05249 2151 11
6.108000+3 5.000000-1 2.870000-1 2.130000-1 7.399990-2 0.000000+05249 2151 12
7.076000+3 5.000000-1 9.230000-1 8.900000-1 3.300000-2 0.000000+05249 2151 13
1.001200+4 5.000000-1 9.080000-1 8.600000-1 4.800000-2 0.000000+05249 2151 14
1.065600+4 5.000000-1 7.498000+0 7.450000+0 4.800000-2 0.000000+05249 2151 15
1.083000+4 5.000000-1 2.048000+0 2.000000+0 4.800000-2 0.000000+05249 2151 16
1.149500+4 5.000000-1 1.244800+1 1.240000+1 4.800000-2 0.000000+05249 2151 17
1.289300+4 5.000000-1 5.023000+0 4.975000+0 4.800000-2 0.000000+05249 2151 18
1.308000+4 5.000000-1 1.406000+0 1.358000+0 4.800000-2 0.000000+05249 2151 19
1.460000+4 5.000000-1 3.248000+0 3.200000+0 4.800000-2 0.000000+05249 2151 20
1.701000+4 5.000000-1 4.123000+0 4.075000+0 4.800000-2 0.000000+05249 2151 21
1.752000+4 5.000000-1 2.823000+0 2.775000+0 4.800000-2 0.000000+05249 2151 22
1.799000+4 5.000000-1 1.738000+0 1.690000+0 4.800000-2 0.000000+05249 2151 23
1.942000+4 5.000000-1 3.573000+0 3.525000+0 4.800000-2 0.000000+05249 2151 24
2.182000+4 5.000000-1 1.419800+1 1.415000+1 4.800000-2 0.000000+05249 2151 25
1.268050+2 0.000000+0 1 0 120 205249 2151 26
4.355000+2 5.000000-1 5.850000-2 1.850000-2 4.000000-2 0.000000+05249 2151 27
9.410000+2 5.000000-1 5.070000-2 1.470000-2 3.600000-2 0.000000+05249 2151 28
1.320500+3 5.000000-1 3.900000-2 1.100000-2 2.800000-2 0.000000+05249 2151 29
1.583000+3 5.000000-1 5.550000-2 1.050000-2 4.500000-2 0.000000+05249 2151 30
3.265000+3 1.500000+0 1.365000-1 4.750000-2 8.900000-2 0.000000+05249 2151 31
3.544000+3 1.500000+0 8.000000-2 3.200000-2 4.800000-2 0.000000+05249 2151 32
4.080000+3 1.500000+0 7.400000-2 2.600000-2 4.800000-2 0.000000+05249 2151 33
5.330000+3 1.500000+0 4.870000-1 2.700000-1 2.170000-1 0.000000+05249 2151 34
6.603000+3 5.000000-1 6.640000-2 1.840000-2 4.800000-2 0.000000+05249 2151 35
7.936000+3 5.000000-1 1.880000-1 1.400000-1 4.800000-2 0.000000+05249 2151 36
1.035500+4 5.000000-1 1.480000-1 1.000000-1 4.800000-2 0.000000+05249 2151 37
1.209800+4 5.000000-1 3.480000-1 3.000000-1 4.800000-2 0.000000+05249 2151 38
1.282800+4 5.000000-1 5.480000-1 5.000000-1 4.800000-2 0.000000+05249 2151 39
1.296000+4 5.000000-1 2.980000-1 2.500000-1 4.800000-2 0.000000+05249 2151 40
1.533000+4 5.000000-1 5.480000-1 5.000000-1 4.800000-2 0.000000+05249 2151 41
1.634000+4 5.000000-1 7.480000-1 7.000000-1 4.800000-2 0.000000+05249 2151 42
1.890000+4 5.000000-1 1.048000+0 1.000000+0 4.800000-2 0.000000+05249 2151 43
1.970000+4 5.000000-1 5.480000-1 5.000000-1 4.800000-2 0.000000+05249 2151 44
2.022000+4 5.000000-1 5.480000-1 5.000000-1 4.800000-2 0.000000+05249 2151 45
2.102500+4 5.000000-1 5.480000-1 5.000000-1 4.800000-2 0.000000+05249 2151 46
8.000000+3 1.000000+5 2 2 0 05249 2151 47
0.000000+0 5.897100-1 0 0 3 05249 2151 48
1.268100+2 0.000000+0 0 0 1 05249 2151 49
5.000000-1 0.000000+0 5 0 72 115249 2151 50
0.000000+0 0.000000+0 0.000000+0 1.000000+0 0.000000+0 0.000000+05249 2151 51
8.000000+3 3.131000+3 0.000000+0 7.827400-2 1.500000-1 0.000000+05249 2151 52
1.000000+4 3.114700+3 0.000000+0 7.786700-2 1.500000-1 0.000000+05249 2151 53
1.500000+4 3.106700+3 0.000000+0 7.766700-2 1.500000-1 0.000000+05249 2151 54
2.500000+4 3.031500+3 0.000000+0 7.578900-2 1.500000-1 0.000000+05249 2151 55
3.000000+4 3.017000+3 0.000000+0 7.542600-2 1.500000-1 0.000000+05249 2151 56
4.000000+4 2.944100+3 0.000000+0 7.360300-2 1.500000-1 0.000000+05249 2151 57
5.000000+4 2.893800+3 0.000000+0 7.234600-2 1.500000-1 0.000000+05249 2151 58
6.000000+4 2.846600+3 0.000000+0 7.116500-2 1.500000-1 0.000000+05249 2151 59
7.000000+4 2.776200+3 0.000000+0 6.940600-2 1.500000-1 0.000000+05249 2151 60
8.000000+4 2.718100+3 0.000000+0 6.795400-2 1.500000-1 0.000000+05249 2151 61
1.000000+5 2.589700+3 0.000000+0 6.474200-2 1.500000-1 0.000000+05249 2151 62
1.268100+2 0.000000+0 1 0 2 05249 2151 63
5.000000-1 0.000000+0 5 0 72 115249 2151 64
0.000000+0 0.000000+0 0.000000+0 1.000000+0 0.000000+0 0.000000+05249 2151 65
8.000000+3 3.131000+3 0.000000+0 5.322600-1 1.500000-1 0.000000+05249 2151 66
1.000000+4 3.114700+3 0.000000+0 5.294900-1 1.500000-1 0.000000+05249 2151 67
1.500000+4 3.106700+3 0.000000+0 5.281400-1 1.500000-1 0.000000+05249 2151 68
2.500000+4 3.031500+3 0.000000+0 5.153600-1 1.500000-1 0.000000+05249 2151 69
3.000000+4 3.017000+3 0.000000+0 5.129000-1 1.500000-1 0.000000+05249 2151 70
4.000000+4 2.944100+3 0.000000+0 5.005000-1 1.500000-1 0.000000+05249 2151 71
5.000000+4 2.893800+3 0.000000+0 4.919500-1 1.500000-1 0.000000+05249 2151 72
6.000000+4 2.846600+3 0.000000+0 4.839200-1 1.500000-1 0.000000+05249 2151 73
7.000000+4 2.776200+3 0.000000+0 4.719600-1 1.500000-1 0.000000+05249 2151 74
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