$Rev:: 532 $ $Date:: 2011-12-05#$ 1 0 0 0
3.808700+4 8.616230+1 1 0 0 13834 1451 1
0.000000+0 0.000000+0 0 0 0 63834 1451 2
1.000000+0 2.000000+7 1 0 10 73834 1451 3
0.000000+0 0.000000+0 0 0 226 413834 1451 4
38-Sr- 87 JNDC EVAL-MAR90 JNDC FP Nuclear Data W.G. 3834 1451 5
DIST-DEC06 20111222 3834 1451 6
----ENDF/B-VII.1 MATERIAL 3834 3834 1451 7
-----INCIDENT NEUTRON DATA 3834 1451 8
------ENDF-6 FORMAT 3834 1451 9
3834 1451 10
============================================================== 3834 1451 11
File produced by WPEC Subgroup 23 in 2004-2005 3834 1451 12
- WPEC: NEA Working Party on Evaluation Cooperation 3834 1451 13
- SG23: International library of fission product evaluations 3834 1451 14
3834 1451 15
CONVERTED FROM JENDL-3.3 BY NNDC OCT 2004 3834 1451 16
Corrected threshold energy secondary energy distributions 3834 1451 17
in MF=5. 3834 1451 18
Corrected interpolation in MF=5. 3834 1451 19
3834 1451 20
============================================================== 3834 1451 21
3834 1451 22
84-10 EVALUATION FOR JENDL-2 WAS MADE BY JNDC FPND W.G./1/ 3834 1451 23
90-03 MODIFICATION FOR JENDL-3 WAS MADE/2/. 3834 1451 24
3834 1451 25
MF = 1 GENERAL INFORMATION 3834 1451 26
MT=451 COMMENTS AND DICTIONARY 3834 1451 27
3834 1451 28
MF = 2 RESONANCE PARAMETERS 3834 1451 29
MT=151 RESOLVED AND UNRESOLVED RESONANCE PARAMETERS 3834 1451 30
RESOLVED RESONANCE REGION (MLBW FORMULA) : BELOW 14.08 KEV 3834 1451 31
RESONANCE PARAMETERS OF JENDL-2 WERE MODIFIED AS FOLLOWS: 3834 1451 32
EVALUATION OF JENDL-2 WAS PERFORMED ON THE BASIS OF THE 3834 1451 33
MEASUREMENTS BY CAMARDA ET AL./3/ AND MUSGROVE ET AL./4/ 3834 1451 34
NEUTRON WIDTHS WERE DERIVED FROM THE DATA OF 2G*(NEUTRON 3834 1451 35
WIDTH) AND NEUTRON CAPTURE AREAS. NEUTRON ORBITAL ANGULAR 3834 1451 36
MOMENTUM L WAS ASSUMED TO BE 0 FOR ALL RESONANCE LEVELS EXCEPT3834 1451 37
THE 2ND LEVEL (L=1) AT 35.27 EV. HOWEVER, THE VALUES OF TOTAL3834 1451 38
SPIN J WERE UNKNOWN FOR ALL RESONANCE LEVELS. THUS, TARGET 3834 1451 39
SPIN OF 4.5 WAS ADOPTED AS J VALUE. AVERAGE RADIATION WIDTH 3834 1451 40
OF 180.4 MEV WAS OBTAINED BY AVERAGING THE GIVEN RADIATION 3834 1451 41
WIDTHS. HOWEVER, THIS VALUE WAS REDUCED TO 110.72 MEV SO AS 3834 1451 42
TO REPRODUCE THE NEUTRON CAPTURE RESONANCE INTEGRAL OF 118+-303834 1451 43
BARNS GIVEN BY MUGHABGHAB ET AL./5/ A NEGATIVE RESONANCE WAS 3834 1451 44
ALSO ADDED AT -50 EV, AND THE PARAMETERS WERE ADJUSTED SO AS 3834 1451 45
TO REPRODUCE THE THERMAL CAPTURE CROSS SECTION OF 16+-3 BARNS 3834 1451 46
GIVEN BY MUGHABGHAB ET AL. 3834 1451 47
3834 1451 48
FOR JENDL-3, THE VALUES OF TOTAL SPIN J WERE TENTATIVELY 3834 1451 49
ESTIMATED WITH A RANDOM NUMBER METHOD. NEUTRON WIDTHS WERE 3834 1451 50
MODIFIED ON THE BASIS OF THE ESTIMATED J-VALUES. RADIATION 3834 1451 51
WIDTH OF THE NEGATIVE LEVEL WAS SLIGHTLY ADJUSTED SO AS TO 3834 1451 52
REPRODUCE THE THERMAL CAPTURE CROSS SECTION ACCORDING TO THE 3834 1451 53
MODIFICATION OF THE POSITIVE LEVELS. SCATTERING RADIUS WAS 3834 1451 54
TAKEN FROM THE GRAPH (FIG. 1, PART A) GIVEN BY MUGHABGHAB ET 3834 1451 55
AL. 3834 1451 56
3834 1451 57
UNRESOLVED RESONANCE REGION : 14.08 KEV - 100 KEV 3834 1451 58
UNRESOLVED RESONANCE PARAMETERS WERE ADOPTED FROM JENDL-2. 3834 1451 59
THE NEUTRON STRENGTH FUNCTIONS, S0, S1 AND S2 WERE CALCULATED 3834 1451 60
WITH OPTICAL MODEL CODE CASTHY/6/. THE OBSERVED LEVEL SPACING3834 1451 61
WAS DETERMINED TO REPRODUCE THE CAPTURE CROSS SECTION 3834 1451 62
CALCULATED WITH CASTHY. THE EFFECTIVE SCATTERING RADIUS WAS 3834 1451 63
OBTAINED FROM FITTING TO THE CALCULATED TOTAL CROSS SECTION AT3834 1451 64
100 KEV. 3834 1451 65
3834 1451 66
TYPICAL VALUES OF THE PARAMETERS AT 70 KEV: 3834 1451 67
S0 = 0.300E-4, S1 = 4.000E-4, S2 = 0.360E-4, SG = 4.72E-4, 3834 1451 68
GG = 0.116 EV, R = 7.414 FM. 3834 1451 69
3834 1451 70
CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS (BARNS) 3834 1451 71
2200 M/S RES. INTEG. 3834 1451 72
TOTAL 22.90 - 3834 1451 73
ELASTIC 6.897 - 3834 1451 74
CAPTURE 16.00 121 3834 1451 75
3834 1451 76
MF = 3 NEUTRON CROSS SECTIONS 3834 1451 77
BELOW 100 KEV, RESONANCE PARAMETERS WERE GIVEN. 3834 1451 78
ABOVE 100 KEV, THE SPHERICAL OPTICAL AND STATISTICAL MODEL 3834 1451 79
CALCULATION WAS PERFORMED WITH CASTHY, BY TAKING ACCOUNT OF 3834 1451 80
COMPETING REACTIONS, OF WHICH CROSS SECTIONS WERE CALCULATED 3834 1451 81
WITH PEGASUS/7/ STANDING ON A PREEQUILIBRIUM AND MULTI-STEP 3834 1451 82
EVAPORATION MODEL. THE OMP'S FOR NEUTRON GIVEN IN TABLE 1 WERE 3834 1451 83
DETERMINED BY IIJIMA AND KAWAI/8/ TO REPRODUCE A SYSTEMATIC 3834 1451 84
TREND OF THE TOTAL CROSS SECTION. THE OMP'S FOR CHARGED 3834 1451 85
PARTICLES ARE AS FOLLOWS: 3834 1451 86
PROTON = PEREY/9/ 3834 1451 87
ALPHA = HUIZENGA AND IGO/10/ 3834 1451 88
DEUTERON = LOHR AND HAEBERLI/11/ 3834 1451 89
HELIUM-3 AND TRITON = BECCHETTI AND GREENLEES/12/ 3834 1451 90
PARAMETERS FOR THE COMPOSITE LEVEL DENSITY FORMULA OF GILBERT 3834 1451 91
AND CAMERON/13/ WERE EVALUATED BY IIJIMA ET AL./14/ MORE 3834 1451 92
EXTENSIVE DETERMINATION AND MODIFICATION WERE MADE IN THE 3834 1451 93
PRESENT WORK. TABLE 2 SHOWS THE LEVEL DENSITY PARAMETERS USED 3834 1451 94
IN THE PRESENT CALCULATION. ENERGY DEPENDENCE OF SPIN CUT-OFF 3834 1451 95
PARAMETER IN THE ENERGY RANGE BELOW E-JOINT IS DUE TO GRUPPELAAR3834 1451 96
/15/. 3834 1451 97
3834 1451 98
MT = 1 TOTAL 3834 1451 99
SPHERICAL OPTICAL MODEL CALCULATION WAS ADOPTED. 3834 1451 100
3834 1451 101
MT = 2 ELASTIC SCATTERING 3834 1451 102
CALCULATED AS (TOTAL - SUM OF PARTIAL CROSS SECTIONS). 3834 1451 103
3834 1451 104
MT = 4, 51 - 91 INELASTIC SCATTERING 3834 1451 105
SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WAS 3834 1451 106
ADOPTED. THE LEVEL SCHEME WAS TAKEN FROM REF./16/. 3834 1451 107
3834 1451 108
NO. ENERGY(MEV) SPIN-PARITY 3834 1451 109
GR. 0.0 9/2 + 3834 1451 110
1 0.3883 1/2 + 3834 1451 111
2 0.8730 3/2 - 3834 1451 112
3 1.2290 5/2 + 3834 1451 113
4 1.2570 5/2 - 3834 1451 114
5 1.7390 13/2 + 3834 1451 115
6 1.7710 5/2 + 3834 1451 116
7 1.9210 7/2 + 3834 1451 117
LEVELS ABOVE 1.997 MEV WERE ASSUMED TO BE OVERLAPPING. 3834 1451 118
3834 1451 119
MT = 102 CAPTURE 3834 1451 120
SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WITH 3834 1451 121
CASTHY WAS ADOPTED. DIRECT AND SEMI-DIRECT CAPTURE CROSS 3834 1451 122
SECTIONS WERE ESTIMATED ACCORDING TO THE PROCEDURE OF BENZI 3834 1451 123
AND REFFO/17/ AND NORMALIZED TO 1 MILLI-BARN AT 14 MEV. 3834 1451 124
3834 1451 125
THE GAMMA-RAY STRENGTH FUNCTION (4.71E-04) WAS ADJUSTED TO 3834 1451 126
REPRODUCE THE CAPTURE CROSS SECTION OF 42 MILLI-BARNS AT 70 3834 1451 127
KEV MEASURED BY MUSGROVE ET AL./4/ 3834 1451 128
3834 1451 129
MT = 16 (N,2N) CROSS SECTION 3834 1451 130
MT = 22 (N,N'A) CROSS SECTION 3834 1451 131
MT = 28 (N,N'P) CROSS SECTION 3834 1451 132
MT = 32 (N,N'D) CROSS SECTION 3834 1451 133
MT =103 (N,P) CROSS SECTION 3834 1451 134
MT =104 (N,D) CROSS SECTION 3834 1451 135
MT =105 (N,T) CROSS SECTION 3834 1451 136
MT =106 (N,HE3) CROSS SECTION 3834 1451 137
MT =107 (N,ALPHA) CROSS SECTION 3834 1451 138
THESE REACTION CROSS SECTIONS WERE CALCULATED WITH THE 3834 1451 139
PREEQUILIBRIUM AND MULTI-STEP EVAPORATION MODEL CODE PEGASUS. 3834 1451 140
3834 1451 141
THE KALBACH'S CONSTANT K (= 394.6) WAS ESTIMATED BY THE 3834 1451 142
FORMULA DERIVED FROM KIKUCHI-KAWAI'S FORMALISM/18/ AND LEVEL 3834 1451 143
DENSITY PARAMETERS. 3834 1451 144
3834 1451 145
FINALLY, THE (N,P) AND (N,ALPHA) CROSS SECTIONS WERE 3834 1451 146
NORMALIZED TO THE FOLLOWING VALUES AT 14.5 MEV: 3834 1451 147
(N,P) 20.60 MB (SYSTEMATICS OF FORREST/19/) 3834 1451 148
(N,ALPHA) 6.81 MB (SYSTEMATICS OF FORREST) 3834 1451 149
3834 1451 150
MT = 251 MU-BAR 3834 1451 151
CALCULATED WITH CASTHY. 3834 1451 152
3834 1451 153
MF = 4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 3834 1451 154
LEGENDRE POLYNOMIAL COEFFICIENTS FOR ANGULAR DISTRIBUTIONS ARE 3834 1451 155
GIVEN IN THE CENTER-OF-MASS SYSTEM FOR MT=2 AND DISCRETE INELAS-3834 1451 156
TIC LEVELS, AND IN THE LABORATORY SYSTEM FOR MT=91. THEY WERE 3834 1451 157
CALCULATED WITH CASTHY. FOR OTHER REACTIONS, ISOTROPIC DISTRI- 3834 1451 158
BUTIONS IN THE LABORATORY SYSTEM WERE ASSUMED. 3834 1451 159
3834 1451 160
MF = 5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS 3834 1451 161
ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS WERE CALCULATED WITH 3834 1451 162
PEGASUS FOR INELASTIC SCATTERING TO OVERLAPPING LEVELS AND FOR 3834 1451 163
OTHER NEUTRON EMITTING REACTIONS. 3834 1451 164
3834 1451 165
TABLE 1 NEUTRON OPTICAL POTENTIAL PARAMETERS 3834 1451 166
3834 1451 167
DEPTH (MEV) RADIUS(FM) DIFFUSENESS(FM) 3834 1451 168
---------------------- ------------ --------------- 3834 1451 169
V = 46.0-0.25E R0 = 5.893 A0 = 0.62 3834 1451 170
WS = 7.0 RS = 6.393 AS = 0.35 3834 1451 171
VSO= 7.0 RSO= 5.893 ASO= 0.62 3834 1451 172
THE FORM OF SURFACE ABSORPTION PART IS DER. WOODS-SAXON TYPE. 3834 1451 173
3834 1451 174
TABLE 2 LEVEL DENSITY PARAMETERS 3834 1451 175
3834 1451 176
NUCLIDE A(1/MEV) T(MEV) C(1/MEV) EX(MEV) PAIRING 3834 1451 177
--------------------------------------------------------------- 3834 1451 178
36-KR- 83 1.483E+01 6.700E-01 2.532E+00 5.589E+00 1.170E+00 3834 1451 179
36-KR- 84 9.970E+00 9.600E-01 4.942E-01 8.590E+00 2.630E+00 3834 1451 180
36-KR- 85 1.024E+01 8.900E-01 1.570E+00 6.261E+00 1.170E+00 3834 1451 181
36-KR- 86 9.052E+00 8.686E-01 2.185E-01 5.874E+00 2.100E+00 3834 1451 182
3834 1451 183
37-RB- 84 1.106E+01 8.060E-01 5.598E+00 4.438E+00 0.0 3834 1451 184
37-RB- 85 1.190E+01 8.690E-01 2.827E+00 7.561E+00 1.460E+00 3834 1451 185
37-RB- 86 1.002E+01 8.500E-01 3.954E+00 4.312E+00 0.0 3834 1451 186
37-RB- 87 8.806E+00 9.410E-01 1.125E+00 5.465E+00 9.300E-01 3834 1451 187
3834 1451 188
38-SR- 85 1.134E+01 9.100E-01 3.646E+00 7.608E+00 1.240E+00 3834 1451 189
38-SR- 86 1.120E+01 8.900E-01 5.328E-01 8.599E+00 2.700E+00 3834 1451 190
38-SR- 87 1.030E+01 8.610E-01 1.186E+00 5.938E+00 1.240E+00 3834 1451 191
38-SR- 88 9.160E+00 7.510E-01 8.288E-02 4.550E+00 2.170E+00 3834 1451 192
--------------------------------------------------------------- 3834 1451 193
3834 1451 194
SPIN CUTOFF PARAMETERS WERE CALCULATED AS 0.146*SQRT(A)*A**(2/3).3834 1451 195
IN THE CASTHY CALCULATION, SPIN CUTOFF FACTORS AT 0 MEV WERE 3834 1451 196
ASSUMED TO BE 6.928 FOR SR- 87 AND 5.839 FOR SR- 88. 3834 1451 197
3834 1451 198
REFERENCES 3834 1451 199
1) AOKI, T. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR BASIC 3834 1451 200
AND APPLIED SCIENCE, SANTA FE., VOL. 2, P.1627 (1985). 3834 1451 201
2) KAWAI, M. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR SCIENCE3834 1451 202
AND TECHNOLOGY, MITO, P. 569 (1988). 3834 1451 203
3) CAMARDA, H., ET AL.: NCSAC-31, 40 (1970). 3834 1451 204
4) MUSGROVE, A.R. DE L., ET AL.: PROC. INT. CONF. ON NEUTRON 3834 1451 205
PHYSICS AND NUCL. DATA FOR REACTORS, HARWELL 1978, 449. 3834 1451 206
5) MUGHABGHAB, S.F. ET AL.: "NEUTRON CROSS SECTIONS, VOL. I, 3834 1451 207
PART A", ACADEMIC PRESS (1981). 3834 1451 208
6) IGARASI, S.: J. NUCL. SCI. TECHNOL., 12, 67 (1975). 3834 1451 209
7) IIJIMA, S. ET AL.: JAERI-M 87-025, P. 337 (1987). 3834 1451 210
8) IIJIMA, S. AND KAWAI, M.: J. NUCL. SCI. TECHNOL., 20, 77 3834 1451 211
(1983). 3834 1451 212
9) PEREY, F.G: PHYS. REV. 131, 745 (1963). 3834 1451 213
10) HUIZENGA, J.R. AND IGO, G.: NUCL. PHYS. 29, 462 (1962). 3834 1451 214
11) LOHR, J.M. AND HAEBERLI, W.: NUCL. PHYS. A232, 381 (1974). 3834 1451 215
12) BECCHETTI, F.D., JR. AND GREENLEES, G.W.: POLARIZATION 3834 1451 216
PHENOMENA IN NUCLEAR REACTIONS ((EDS) H.H. BARSHALL AND 3834 1451 217
W. HAEBERLI), P. 682, THE UNIVERSITY OF WISCONSIN PRESS. 3834 1451 218
(1971). 3834 1451 219
13) GILBERT, A. AND CAMERON, A.G.W.: CAN. J. PHYS., 43, 1446 3834 1451 220
(1965). 3834 1451 221
14) IIJIMA, S., ET AL.: J. NUCL. SCI. TECHNOL. 21, 10 (1984). 3834 1451 222
15) GRUPPELAAR, H.: ECN-13 (1977). 3834 1451 223
16) LEDERER, C.M., ET AL.: "TABLE OF ISOTOPES, 7TH ED.", WILEY- 3834 1451 224
INTERSCIENCE PUBLICATION (1978). 3834 1451 225
17) BENZI, V. AND REFFO, G.: CCDN-NW/10 (1969). 3834 1451 226
18) KIKUCHI, K. AND KAWAI, M.: "NUCLEAR MATTER AND NUCLEAR 3834 1451 227
REACTIONS", NORTH HOLLAND (1968). 3834 1451 228
19) FORREST, R.A.: AERE-R 12419 (1986). 3834 1451 229
3834 1451 230
1 451 271 13834 1451 231
2 151 271 03834 1451 232
3 1 24 03834 1451 233
3 2 24 03834 1451 234
3 4 14 03834 1451 235
3 16 9 03834 1451 236
3 22 10 03834 1451 237
3 28 9 03834 1451 238
3 32 5 03834 1451 239
3 51 14 03834 1451 240
3 52 12 03834 1451 241
3 53 11 03834 1451 242
3 54 11 03834 1451 243
3 55 10 03834 1451 244
3 56 9 03834 1451 245
3 57 9 03834 1451 246
3 91 8 03834 1451 247
3 102 19 03834 1451 248
3 103 14 03834 1451 249
3 104 11 03834 1451 250
3 105 8 03834 1451 251
3 106 8 03834 1451 252
3 107 14 03834 1451 253
4 2 159 03834 1451 254
4 16 10 03834 1451 255
4 22 10 03834 1451 256
4 28 10 03834 1451 257
4 32 10 03834 1451 258
4 51 24 03834 1451 259
4 52 24 03834 1451 260
4 53 22 03834 1451 261
4 54 22 03834 1451 262
4 55 22 03834 1451 263
4 56 22 03834 1451 264
4 57 22 03834 1451 265
4 91 22 03834 1451 266
5 16 50 13834 1451 267
5 22 123 13834 1451 268
5 28 82 13834 1451 269
5 32 29 13834 1451 270
5 91 107 03834 1451 271
0.000000+0 0.000000+0 0 0 0 03834 1 099999
0.000000+0 0.000000+0 0 0 0 03834 0 0 0
3.808700+4 8.616230+1 0 0 1 03834 2151 1
3.808700+4 1.000000+0 0 0 2 03834 2151 2
1.000000-5 1.408000+4 1 2 0 03834 2151 3
4.500000+0 7.110000-1 0 0 2 03834 2151 4
8.616230+1 0.000000+0 0 0 690 1153834 2151 5
-5.000000+1 5.000000+0 3.406700-1 2.300000-1 1.106700-1 0.000000+03834 2151 6
3.530000+0 5.000000+0 2.056180-1 6.182000-4 2.050000-1 0.000000+03834 2151 7
3.213000+2 4.000000+0 1.160510-1 5.333000-3 1.107180-1 0.000000+03834 2151 8
5.430000+2 4.000000+0 1.138290-1 3.111000-3 1.107180-1 0.000000+03834 2151 9
6.483000+2 4.000000+0 7.996180-1 6.889000-1 1.107180-1 0.000000+03834 2151 10
6.759000+2 5.000000+0 1.598080-1 4.909000-2 1.107180-1 0.000000+03834 2151 11
7.375000+2 4.000000+0 5.107180-1 4.000000-1 1.107180-1 0.000000+03834 2151 12
7.469000+2 4.000000+0 1.462780-1 3.556000-2 1.107180-1 0.000000+03834 2151 13
9.664000+2 4.000000+0 1.329380-1 2.222000-2 1.107180-1 0.000000+03834 2151 14
1.184000+3 4.000000+0 1.240480-1 1.333000-2 1.107180-1 0.000000+03834 2151 15
1.259000+3 5.000000+0 1.307180-1 2.000000-2 1.107180-1 0.000000+03834 2151 16
1.335000+3 4.000000+0 4.221720+0 4.111000+0 1.107180-1 0.000000+03834 2151 17
1.402000+3 4.000000+0 2.996180-1 1.889000-1 1.107180-1 0.000000+03834 2151 18
1.700000+3 4.000000+0 1.173850-1 6.667000-3 1.107180-1 0.000000+03834 2151 19
1.719000+3 4.000000+0 1.329380-1 2.222000-2 1.107180-1 0.000000+03834 2151 20
2.013000+3 5.000000+0 1.325380-1 2.182000-2 1.107180-1 0.000000+03834 2151 21
2.092000+3 4.000000+0 1.284980-1 1.778000-2 1.107180-1 0.000000+03834 2151 22
2.112000+3 4.000000+0 6.440180-1 5.333000-1 1.107180-1 0.000000+03834 2151 23
2.353000+3 5.000000+0 1.543580-1 4.364000-2 1.107180-1 0.000000+03834 2151 24
2.439000+3 4.000000+0 4.885180-1 3.778000-1 1.107180-1 0.000000+03834 2151 25
2.756000+3 5.000000+0 5.652180-1 4.545000-1 1.107180-1 0.000000+03834 2151 26
2.978000+3 5.000000+0 1.143540-1 3.636000-3 1.107180-1 0.000000+03834 2151 27
3.067000+3 4.000000+0 2.638130-1 6.667000-2 1.971430-1 0.000000+03834 2151 28
3.221000+3 5.000000+0 1.144910-1 3.773000-3 1.107180-1 0.000000+03834 2151 29
3.299000+3 5.000000+0 1.302580-1 1.954000-2 1.107180-1 0.000000+03834 2151 30
3.401000+3 4.000000+0 3.222180-1 2.115000-1 1.107180-1 0.000000+03834 2151 31
3.443000+3 5.000000+0 1.164820-1 5.764000-3 1.107180-1 0.000000+03834 2151 32
3.671000+3 5.000000+0 1.074600+0 9.091000-1 1.655010-1 0.000000+03834 2151 33
3.764000+3 4.000000+0 1.699980-1 5.928000-2 1.107180-1 0.000000+03834 2151 34
3.942000+3 5.000000+0 2.979180-1 1.872000-1 1.107180-1 0.000000+03834 2151 35
4.049000+3 5.000000+0 3.460450+0 3.364000+0 9.645000-2 0.000000+03834 2151 36
4.057000+3 4.000000+0 1.750080-1 6.429000-2 1.107180-1 0.000000+03834 2151 37
4.142000+3 5.000000+0 1.770980-1 6.638000-2 1.107180-1 0.000000+03834 2151 38
4.189000+3 4.000000+0 1.447580-1 3.404000-2 1.107180-1 0.000000+03834 2151 39
4.441000+3 5.000000+0 1.435230+0 1.364000+0 7.122900-2 0.000000+03834 2151 40
4.498000+3 5.000000+0 1.935980-1 8.288000-2 1.107180-1 0.000000+03834 2151 41
4.781000+3 4.000000+0 3.497560+0 3.333000+0 1.645570-1 0.000000+03834 2151 42
4.854000+3 4.000000+0 2.923180-1 1.816000-1 1.107180-1 0.000000+03834 2151 43
4.945000+3 4.000000+0 2.196180-1 1.089000-1 1.107180-1 0.000000+03834 2151 44
4.981000+3 4.000000+0 2.242020+0 2.178000+0 6.402500-2 0.000000+03834 2151 45
4.993000+3 4.000000+0 4.013260+0 3.889000+0 1.242600-1 0.000000+03834 2151 46
5.211000+3 5.000000+0 2.328420+0 2.182000+0 1.464190-1 0.000000+03834 2151 47
5.367000+3 5.000000+0 1.859660+0 1.727000+0 1.326580-1 0.000000+03834 2151 48
5.391000+3 5.000000+0 4.609180-1 3.502000-1 1.107180-1 0.000000+03834 2151 49
5.519000+3 5.000000+0 2.485670+0 2.273000+0 2.126740-1 0.000000+03834 2151 50
5.567000+3 4.000000+0 1.229280-1 1.221000-2 1.107180-1 0.000000+03834 2151 51
5.746000+3 5.000000+0 2.298180-1 1.191000-1 1.107180-1 0.000000+03834 2151 52
5.796000+3 5.000000+0 2.900480+0 2.727000+0 1.734840-1 0.000000+03834 2151 53
6.077000+3 5.000000+0 8.318020+0 8.182000+0 1.360250-1 0.000000+03834 2151 54
6.172000+3 4.000000+0 1.126850+1 1.111000+1 1.584720-1 0.000000+03834 2151 55
6.181000+3 5.000000+0 2.137180-1 1.030000-1 1.107180-1 0.000000+03834 2151 56
6.528000+3 4.000000+0 1.484780-1 3.776000-2 1.107180-1 0.000000+03834 2151 57
6.587000+3 5.000000+0 2.042260+0 1.924000+0 1.182590-1 0.000000+03834 2151 58
6.704000+3 5.000000+0 1.743870+0 1.638000+0 1.058750-1 0.000000+03834 2151 59
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