IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0
1.00300+ 3 2.99014+ 0 0 0 6 131169 1451 1
0.00000+ 0 0.00000+ 0 0 0 171 01169 1451 2
1-H - 3 LASL EVAL-FEB65 LEONA STEWART 1169 1451 3
DIST-FEB74 REV-OCT74 1169 1451 4
1169 1451 5
*************************************************************** 1169 1451 6
FILE=1 MT=457 RADIOACTIVE DECAY DATA 1169 1451 7
EVALUATED BY C.W.REICH (ANC) ADDED FEB74 1169 1451 8
REFERENCES= 1169 1451 9
Q- 1973 REVISION OF THE WAPSTRA-GOVE MASS TABLE 1169 1451 10
HALF-LIFE - N.E. HOLDEN, CHART OF THE NUCLIDES(1973);1169 1451 11
AND PRIVATE COMMUNICATION (JAN.,1974) 1169 1451 12
OTHER- M.J. MARTIN AND P.H. BLICHERT-TOFT NUCLEAR 1169 1451 13
DATA TABLES A, NOS.1-2, P.1 (1970) 1169 1451 14
1169 1451 15
***************** DNA 4169 MOD 1 ****************** 1169 1451 16
1169 1451 17
THE MT=102 MEASURED CROSS SECTION IS LESS THAN 1169 1451 18
6.7 MICROBARNS AT THERMAL ENERGY. SINCE THE 1169 1451 19
Q VALUE IS EITHER ZERO OR POSITIVE, THIS CROSS 1169 1451 20
SECTION WAS ASSUMED ZERO AT ALL ENERGIES AND 1169 1451 21
WAS REMOVED FROM FILE 3 FOR THIS MOD. 1169 1451 22
1169 1451 23
*************************************************************** 1169 1451 24
1169 1451 25
1169 1451 26
***************** DNA 4169 MOD 0 ****************** 1169 1451 27
1169 1451 28
1169 1451 29
* * * * * * 1169 1451 30
TRITIUM IN ENDF/B-IV FORMAT 1169 1451 31
1169 1451 32
PRIMARY REFERENCE LA-3270 BY 1169 1451 33
LEONA STEWART (FEBRUARY 1965, UPDATED 1169 1451 34
AUGUST 1967) 1169 1451 35
LOS ALAMOS SCIENTIFIC LABORATORY 1169 1451 36
1169 1451 37
DATA INPUT FEBRUARY, 1971 1169 1451 38
1169 1451 39
MF=1 1169 1451 40
MT=451 ATOMIC MASS = 3.01605 1169 1451 41
1169 1451 42
MT=457 DECAY DATA, SEE INSERT ABOVE. 1169 1451 43
1169 1451 44
MF=2 1169 1451 45
1169 1451 46
MT=151 SCATTERING LENGTH=0.32164 X 1.0E-12 CM1169 1451 47
1169 1451 48
MF=3 1169 1451 49
MT=1 TOTAL CROSS SECTIONS. TOTAL CROSS 1169 1451 50
SECTIONS FROM 290 KEV TO 20 MEV FROM 1169 1451 51
LASL MEASUREMENTS (REF.1). ESTIMATED 1169 1451 52
BELOW 290 KEV. 1169 1451 53
1169 1451 54
MT=2. ELASTIC SCATTERING. INPUT AS 1169 1451 55
PROBABILITY VERSUS COSINE IN THE 1169 1451 56
CENTER-OF-MASS SYSTEM. DATA TAKEN FROM1169 1451 57
MEASUREMENTS (REF. 2 TO 10) UP TO 1967 1169 1451 58
ON N-T AND P-HE3 SYSTEMS. 1169 1451 59
ALSO, RECENT MEASUREMENTS ON N-T BY 1169 1451 60
SEAGRAVE ET AL. (REF.11) AND ON P-HE3 1169 1451 61
BY MORALES AND CAHILL (REF.12) AND BY 1169 1451 62
HUTSON ET AL (REF.13) HAVE BEEN USED TO1169 1451 63
UPDATE THE ELASTIC ANGULAR DISTRIBUT- 1169 1451 64
IONS ABOVE 15 MEV. (FEBRUARY 1971) 1169 1451 65
(THIS IS THE ONLY CHANGE MADE TO THE 1169 1451 66
EVALUATION FROM THAT DESCRIBED IN 1169 1451 67
LA-3270). 1169 1451 68
1169 1451 69
MT=16 (N,2N) CROSS SECTIONS. ONLY ONE 1169 1451 70
MEASUREMENT EXISTS, THAT OF MATHER AND 1169 1451 71
PAIN (REF.14) AT 14.1 MEV. ESTIMATES 1169 1451 72
OF THIS CROSS SECTION WERE THEREFORE 1169 1451 73
MADE FROM SYSTEMATICS AND THE P-HE3 1169 1451 74
REACTION STUDIES OF ROSEN AND LELAND 1169 1451 75
(REF.9) AND OF ANDERSON (REF.15). 1169 1451 76
1169 1451 77
MT=17 (N,3N) CROSS SECTION. NO DATA GIVEN 1169 1451 78
SINCE ESTIMATES FROM ISOSPIN CON- 1169 1451 79
SIDERATIONS GIVEN ESSENTIALLY ZERO 1169 1451 80
PROBABILITIES. MATHER AND PAIN 1169 1451 81
(REF.14) AND COOKSON (REF. 16) CONFIRM 1169 1451 82
THESE ESTIMATES. 1169 1451 83
1169 1451 84
NOT GIVEN MT=102 THE MEASURED CROSS SECTION IS LESS THAN1169 1451 85
OR EQUAL TO 6.7 MICROBARNS AT THERMAL 1169 1451 86
SINCE THE Q VALUE IS UNCERTAIN 1169 1451 87
BUT EITHER ZERO OF POSITIVE, THIS 1169 1451 88
CROSS SECTION IS ASSUMED ZERO AT ALL 1169 1451 89
ENERGIES. 1169 1451 90
1169 1451 91
MT=251 AVERAGE VALUE OF THE SCATTERING ANGLE 1169 1451 92
IN THE LABORATORY SYSTEM FROM 1.0E-05 1169 1451 93
EV TO 20 MEV. 1169 1451 94
1169 1451 95
MT=252 AVERAGE LOGARITHMETIC ENERGY CHANGE PER1169 1451 96
COLLISION, FROM 1.0E-05 EV TO 20 MEV. 1169 1451 97
1169 1451 98
MT=253 GAMMA, FROM 1.0E-05 EV TO 20 MEV. 1169 1451 99
1169 1451 100
MF=4 1169 1451 101
MT=2 NEUTRON ELASTIC ANGULAR DISTRIBUTIONS 1169 1451 102
IN THE CENTER OF MASS SYSTEM. 1169 1451 103
THESE ARE GIVEN AS NORMALIZED 1169 1451 104
PROBABILITIES VERSUS COSINE OF THE 1169 1451 105
SCATTERING ANGLE. 1169 1451 106
1169 1451 107
MT=16 (N,2N) ANGULAR DISTRIBUTIONS ARE GIVEN 1169 1451 108
IN THE LABORATORY SYSTEM AS NORMALIZED 1169 1451 109
PROBABILITIES VERSUS COSINE OF THE 1169 1451 110
SCATTERING ANGLE. SEE LA-3270 FOR 1169 1451 111
DETAILS ON THESE DISTRIBUTION 1169 1451 112
FUNCTIONS. 1169 1451 113
1169 1451 114
MF=5 1169 1451 115
MT=16 (N,2N) ENERGY DISTRIBUTIONS ARE GIVEN 1169 1451 116
AS NORMALIZED PROBABILITIES VERSUS 1169 1451 117
ENERGY OF THE OUT GOING NEUTRON IN THE 1169 1451 118
LABORATORY SYSTEM. SEE LA-3270 FOR 1169 1451 119
DETAILS ON THESE DISTRIBUTION 1169 1451 120
FUNCTIONS. 1169 1451 121
1169 1451 122
MF=12,13,14,15 1169 1451 123
ONLY RADIATIVE CAPTURE PRODUCES GAMMA 1169 1451 124
RAYS. SINCE THE CAPTURE CROSS SECTION 1169 1451 125
IS ASSUMED ZERO AT ALL ENERGIES, 1169 1451 126
THESE FILES ARE PURPOSELY LEFT EMPTY. 1169 1451 127
1169 1451 128
1169 1451 129
REFERENCES 1169 1451 130
1169 1451 131
1. LOS ALAMOS PHYSICS AND CRYOGENICS GROUPS, NUCL. 1169 1451 132
PHYS. 12, 291 (1959). 1169 1451 133
1169 1451 134
2. J.D. SEAGRAVE, ET AL, PHYS. REV. 119, 1981 (1960). 1169 1451 135
1169 1451 136
3. J.H. COON, ET AL, PHYS. REV. 81, 33 (1951). 1169 1451 137
1169 1451 138
4. T.B. CLEGG, ET AL, NUCL. PHYS. 50, 621 (1964). 1169 1451 139
1169 1451 140
5. W. HAEBERLI, ET AL, PHYS. REV. 133, B1178 (1964). 1169 1451 141
1169 1451 142
6. J.E. BROLLEY, JR., ET AL, PHYS. REV. 117, 1307 1169 1451 143
(1960). DATA AT BACK ANGLES WHERE THE HE3 PARTICLES1169 1451 144
WERE OBSERVED WERE IGNORED IN THIS ANALYSIS. 1169 1451 145
1169 1451 146
7. R.H. LOVBERG, PHYS. REV. 103, 1393 (1956). 1169 1451 147
1169 1451 148
8. R.A. VANETSIAN AND E.D. FEDCHENKO, SOVIET J. OF 1169 1451 149
ATOMIC ENERGY, TRANS. 2, 141 (1957), AND 1169 1451 150
K.P. ARTEMOV, S.P. KALININ AND L.H. SAMOILOV, 1169 1451 151
JETP 10, 474 (1960). THE LATTER DATA WERE NOT 1169 1451 152
USED, SINCE THEY COVERED THE 5- TO 10-MEV ENERGY 1169 1451 153
REGION AND WERE NOT AVAILABLE. 1169 1451 154
1169 1451 155
9. L. ROSEN AND W.T. LELAND, WASH-1064 (EANDC(US)-79 1169 1451 156
U) (OCT. 1966), P. 99. 1169 1451 157
1169 1451 158
10. D. BLANC, F. CAMBOU, M. NIEL, AND G. VEDRENNE, 1169 1451 159
J. DE PHYSIQUE, SUPPLEMENT FASC. 3-4, C1-98 (1966).1169 1451 160
1169 1451 161
11. J.D. SEAGRAVE ET AL., LA-DC-12954 (1971). 1169 1451 162
1169 1451 163
12. J.R. MORALES AND T.A. CAHILL, BULL. AM. PHYS. SOC. 1169 1451 164
14, 554 (1969), AND PRIVATE COMMUNICATION. 1169 1451 165
1169 1451 166
13. R.L. HUTSON ET AL., PHYS. REV. 4, C17 (1971). 1169 1451 167
1169 1451 168
14. D.S. MATHER AND L.F. PAIN, AWRE 047/69 (1969). 1169 1451 169
1169 1451 170
15. JOHN D. ANDERSON, PRIVATE COMMUNICATION, 1965, AND 1169 1451 171
ANDERSON ET AL, PHYS. REV. LETTERS 15, 66 (1965). 1169 1451 172
1169 1451 173
1 451 186 1169 1451 174
1 457 8 1169 1451 175
2 151 4 1169 1451 176
3 1 28 1169 1451 177
3 2 28 1169 1451 178
3 3 13 1169 1451 179
3 16 13 1169 1451 180
3 251 8 1169 1451 181
3 252 8 1169 1451 182
3 253 8 1169 1451 183
4 2 148 1169 1451 184
4 16 140 1169 1451 185
5 16 198 1169 1451 186
1169 1 0 187
1.00300+ 3 2.99014+ 0 0 0 0 11169 1457 188
3.88839+ 8 3.15360+ 5 0 0 4 21169 1457 189
5.72000+ 3 1.00000+ 1 0.00000+ 0 0.00000+ 0 1169 1457 190
1.00300+ 3 2.99014+ 0 0 0 6 11169 1457 191
1.00000+ 0 0.00000+ 0 1.86260+ 4 1.10000+ 1 1.00000+ 0 0.00000+ 01169 1457 192
1.00000+ 0 0.00000+ 0 0 0 12 11169 1457 193
1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01169 1457 194
1.86260+ 4 1.10000+ 1 1.00000+ 2 0.00000+ 0 0.00000+ 0 0.00000+ 01169 1457 195
1169 1 0 196
1169 0 0 197
1.00300+ 3 2.99014+ 0 0 0 1 01169 2151 198
1.00300+ 3 1.00000+ 0 0 0 1 01169 2151 199
1.00000- 5 2.00000+ 7 0 0 0 01169 2151 200
5.00000- 1 3.21640- 1 0 0 0 01169 2151 201
1169 2 0 202
1169 0 0 203
1.00300+ 3 2.99014+ 0 0 0 0 01169 3 1 204
0.00000+ 0 0.00000+ 0 0 0 1 741169 3 1 205
74 5 1169 3 1 206
1.00000- 5 1.30000+ 0 2.53000- 2 1.30000+ 0 1.00000+ 2 1.30000+ 01169 3 1 207
1.00000+ 5 1.30000+ 0 1.50000+ 5 1.30000+ 0 2.00000+ 5 1.31500+ 01169 3 1 208
2.50000+ 5 1.32500+ 0 3.00000+ 5 1.35000+ 0 3.50000+ 5 1.37000+ 01169 3 1 209
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5.50000+ 5 1.48000+ 0 6.00000+ 5 1.51000+ 0 6.50000+ 5 1.53000+ 01169 3 1 211
7.00000+ 5 1.56000+ 0 8.00000+ 5 1.61000+ 0 9.00000+ 5 1.65000+ 01169 3 1 212
1.00000+ 6 1.70000+ 0 1.25000+ 6 1.79500+ 0 1.50000+ 6 1.89500+ 01169 3 1 213
1.75000+ 6 2.01500+ 0 2.00000+ 6 2.12000+ 0 2.25000+ 6 2.21000+ 01169 3 1 214
2.50000+ 6 2.29500+ 0 2.75000+ 6 2.35000+ 0 3.00000+ 6 2.40000+ 01169 3 1 215
3.20000+ 6 2.42000+ 0 3.50000+ 6 2.43500+ 0 3.70000+ 6 2.44000+ 01169 3 1 216
4.00000+ 6 2.41000+ 0 4.20000+ 6 2.38000+ 0 4.50000+ 6 2.33500+ 01169 3 1 217
4.70000+ 6 2.30000+ 0 5.00000+ 6 2.24000+ 0 5.20000+ 6 2.20000+ 01169 3 1 218
5.50000+ 6 2.14000+ 0 5.70000+ 6 2.09500+ 0 6.00000+ 6 2.03000+ 01169 3 1 219
6.20000+ 6 1.98500+ 0 6.50000+ 6 1.92500+ 0 6.70000+ 6 1.87000+ 01169 3 1 220
7.00000+ 6 1.81500+ 0 7.50000+ 6 1.70500+ 0 8.00000+ 6 1.61500+ 01169 3 1 221
8.35000+ 6 1.56500+ 0 8.38000+ 6 1.56000+ 0 8.40000+ 6 1.55500+ 01169 3 1 222
8.50000+ 6 1.53500+ 0 8.60000+ 6 1.52800+ 0 8.75000+ 6 1.50300+ 01169 3 1 223
9.00000+ 6 1.46000+ 0 9.25000+ 6 1.42500+ 0 9.50000+ 6 1.39500+ 01169 3 1 224
1.00000+ 7 1.33000+ 0 1.02500+ 7 1.31000+ 0 1.05000+ 7 1.27500+ 01169 3 1 225
1.07500+ 7 1.25000+ 0 1.10000+ 7 1.22000+ 0 1.13000+ 7 1.20000+ 01169 3 1 226
1.15000+ 7 1.17000+ 0 1.20000+ 7 1.12500+ 0 1.25000+ 7 1.07500+ 01169 3 1 227
1.30000+ 7 1.04500+ 0 1.35000+ 7 1.00500+ 0 1.40000+ 7 9.75000- 11169 3 1 228
1.41000+ 7 9.65000- 1 1.45000+ 7 9.37000- 1 1.50000+ 7 9.05000- 11169 3 1 229
1.55000+ 7 8.78000- 1 1.60000+ 7 8.50000- 1 1.75000+ 7 7.75000- 11169 3 1 230
1.94000+ 7 6.95000- 1 2.00000+ 7 6.73000- 1 1169 3 1 231
1169 3 0 232
1.00300+ 3 2.99014+ 0 0 0 0 01169 3 2 233
0.00000+ 0 0.00000+ 0 0 0 1 741169 3 2 234
74 5 1169 3 2 235
1.00000- 5 1.30000+ 0 2.53000- 2 1.30000+ 0 1.00000+ 2 1.30000+ 01169 3 2 236
1.00000+ 5 1.30000+ 0 1.50000+ 5 1.30000+ 0 2.00000+ 5 1.31500+ 01169 3 2 237
2.50000+ 5 1.32500+ 0 3.00000+ 5 1.35000+ 0 3.50000+ 5 1.37000+ 01169 3 2 238
4.00000+ 5 1.40000+ 0 4.50000+ 5 1.42500+ 0 5.00000+ 5 1.45000+ 01169 3 2 239
5.50000+ 5 1.48000+ 0 6.00000+ 5 1.51000+ 0 6.50000+ 5 1.53000+ 01169 3 2 240
7.00000+ 5 1.56000+ 0 8.00000+ 5 1.61000+ 0 9.00000+ 5 1.65000+ 01169 3 2 241
1.00000+ 6 1.70000+ 0 1.25000+ 6 1.79500+ 0 1.50000+ 6 1.89500+ 01169 3 2 242
1.75000+ 6 2.01500+ 0 2.00000+ 6 2.12000+ 0 2.25000+ 6 2.21000+ 01169 3 2 243
2.50000+ 6 2.29500+ 0 2.75000+ 6 2.35000+ 0 3.00000+ 6 2.40000+ 01169 3 2 244
3.20000+ 6 2.42000+ 0 3.50000+ 6 2.43500+ 0 3.70000+ 6 2.44000+ 01169 3 2 245
4.00000+ 6 2.41000+ 0 4.20000+ 6 2.38000+ 0 4.50000+ 6 2.33500+ 01169 3 2 246
4.70000+ 6 2.30000+ 0 5.00000+ 6 2.24000+ 0 5.20000+ 6 2.20000+ 01169 3 2 247
5.50000+ 6 2.14000+ 0 5.70000+ 6 2.09500+ 0 6.00000+ 6 2.03000+ 01169 3 2 248
6.20000+ 6 1.98500+ 0 6.50000+ 6 1.92500+ 0 6.70000+ 6 1.87000+ 01169 3 2 249
7.00000+ 6 1.81500+ 0 7.50000+ 6 1.70500+ 0 8.00000+ 6 1.61500+ 01169 3 2 250
8.35000+ 6 1.56500+ 0 8.38000+ 6 1.55900+ 0 8.40000+ 6 1.55250+ 01169 3 2 251
8.50000+ 6 1.52850+ 0 8.60000+ 6 1.51650+ 0 8.75000+ 6 1.48650+ 01169 3 2 252
9.00000+ 6 1.43600+ 0 9.25000+ 6 1.39400+ 0 9.50000+ 6 1.35950+ 01169 3 2 253
1.00000+ 7 1.28550+ 0 1.02500+ 7 1.26250+ 0 1.05000+ 7 1.22550+ 01169 3 2 254
1.07500+ 7 1.19930+ 0 1.10000+ 7 1.16840+ 0 1.13000+ 7 1.14780+ 01169 3 2 255
1.15000+ 7 1.11750+ 0 1.20000+ 7 1.07250+ 0 1.25000+ 7 1.02280+ 01169 3 2 256
1.30000+ 7 9.93400- 1 1.35000+ 7 9.54100- 1 1.40000+ 7 9.25000- 11169 3 2 257
1.41000+ 7 9.15300- 1 1.45000+ 7 8.88200- 1 1.50000+ 7 8.57400- 11169 3 2 258
1.55000+ 7 8.31600- 1 1.60000+ 7 8.05000- 1 1.75000+ 7 7.34200- 11169 3 2 259
1.94000+ 7 6.59400- 1 2.00000+ 7 6.39200- 1 1169 3 2 260
1169 3 0 261
1.00300+ 3 2.99014+ 0 0 0 0 01169 3 3 262
0.00000+ 0-6.25760+ 6 0 0 2 291169 3 3 263
2 2 29 5 1169 3 3 264
8.35000+ 6 0.00000+ 0 8.38000+ 6 1.00000- 3 8.40000+ 6 2.50000- 31169 3 3 265
8.50000+ 6 6.50000- 3 8.60000+ 6 1.15000- 2 8.75000+ 6 1.65000- 21169 3 3 266
9.00000+ 6 2.40000- 2 9.25000+ 6 3.10000- 2 9.50000+ 6 3.55000- 21169 3 3 267
1.00000+ 7 4.45000- 2 1.02500+ 7 4.75000- 2 1.05000+ 7 4.95000- 21169 3 3 268
1.07500+ 7 5.07000- 2 1.10000+ 7 5.16000- 2 1.13000+ 7 5.22000- 21169 3 3 269
1.15000+ 7 5.25000- 2 1.20000+ 7 5.25000- 2 1.25000+ 7 5.22000- 21169 3 3 270
1.30000+ 7 5.16000- 2 1.35000+ 7 5.09000- 2 1.40000+ 7 5.00000- 21169 3 3 271
1.41000+ 7 4.97000- 2 1.45000+ 7 4.88000- 2 1.50000+ 7 4.76000- 21169 3 3 272
1.55000+ 7 4.64000- 2 1.60000+ 7 4.50000- 2 1.75000+ 7 4.08000- 21169 3 3 273
1.94000+ 7 3.56000- 2 2.00000+ 7 3.38000- 2 1169 3 3 274
1169 3 0 275
1.00300+ 3 2.99014+ 0 0 0 0 01169 3 16 276
0.00000+ 0-6.25760+ 6 0 0 2 291169 3 16 277
2 2 29 5 1169 3 16 278
8.35000+ 6 0.00000+ 0 8.38000+ 6 1.00000- 3 8.40000+ 6 2.50000- 31169 3 16 279
8.50000+ 6 6.50000- 3 8.60000+ 6 1.15000- 2 8.75000+ 6 1.65000- 21169 3 16 280
9.00000+ 6 2.40000- 2 9.25000+ 6 3.10000- 2 9.50000+ 6 3.55000- 21169 3 16 281
1.00000+ 7 4.45000- 2 1.02500+ 7 4.75000- 2 1.05000+ 7 4.95000- 21169 3 16 282
1.07500+ 7 5.07000- 2 1.10000+ 7 5.16000- 2 1.13000+ 7 5.22000- 21169 3 16 283
1.15000+ 7 5.25000- 2 1.20000+ 7 5.25000- 2 1.25000+ 7 5.22000- 21169 3 16 284
1.30000+ 7 5.16000- 2 1.35000+ 7 5.09000- 2 1.40000+ 7 5.00000- 21169 3 16 285
1.41000+ 7 4.97000- 2 1.45000+ 7 4.88000- 2 1.50000+ 7 4.76000- 21169 3 16 286
1.55000+ 7 4.64000- 2 1.60000+ 7 4.50000- 2 1.75000+ 7 4.08000- 21169 3 16 287
1.94000+ 7 3.56000- 2 2.00000+ 7 3.38000- 2 1169 3 16 288
1169 3 0 289
1.00300+ 3 2.99014+ 0 0 0 0 01169 3251 290
0.00000+ 0 0.00000+ 0 0 0 1 151169 3251 291
15 2 1169 3251 292
1.00000- 5 2.22950- 1 1.00000+ 5 2.22950- 1 5.00000+ 5 6.04600- 21169 3251 293
1.00000+ 6-9.57110- 2 1.50000+ 6-6.38390- 2 2.00000+ 6-4.56900- 21169 3251 294
3.50000+ 6 2.25340- 1 6.00000+ 6 4.37160- 1 8.50000+ 6 4.95000- 11169 3251 295
9.50000+ 6 5.14450- 1 1.04000+ 7 5.28560- 1 1.15000+ 7 5.52990- 11169 3251 296
1.40000+ 7 5.72630- 1 1.62300+ 7 6.19100- 1 2.00000+ 7 6.44900- 11169 3251 297
1169 3 0 298
1.00300+ 3 2.99014+ 0 0 0 0 01169 3252 299
0.00000+ 0 0.00000+ 0 0 0 1 151169 3252 300
15 2 1169 3252 301
1.00000- 5 5.39300- 1 1.00000+ 5 5.39300- 1 5.00000+ 5 6.52960- 11169 3252 302
1.00000+ 6 7.62040- 1 1.50000+ 6 7.39480- 1 2.00000+ 6 7.25990- 11169 3252 303
3.50000+ 6 5.36110- 1 6.00000+ 6 3.88010- 1 8.50000+ 6 3.47660- 11169 3252 304
9.50000+ 6 3.33940- 1 1.04000+ 7 3.23680- 1 1.15000+ 7 3.06350- 11169 3252 305
1.40000+ 7 2.92150- 1 1.62300+ 7 2.61750- 1 2.00000+ 7 2.43680- 11169 3252 306
1169 3 0 307
1.00300+ 3 2.99014+ 0 0 0 0 01169 3253 308
0.00000+ 0 0.00000+ 0 0 0 1 151169 3253 309
15 2 1169 3253 310
1.00000- 5 4.05760- 1 1.00000+ 5 4.05760- 1 5.00000+ 5 4.48740- 11169 3253 311
1.00000+ 6 4.77960- 1 1.50000+ 6 4.84320- 1 2.00000+ 6 4.92700- 11169 3253 312
3.50000+ 6 4.71830- 1 6.00000+ 6 4.26610- 1 8.50000+ 6 4.06490- 11169 3253 313
9.50000+ 6 3.97000- 1 1.04000+ 7 3.89510- 1 1.15000+ 7 3.86790- 11169 3253 314
1.40000+ 7 3.82120- 1 1.62300+ 7 3.56170- 1 2.00000+ 7 3.42330- 11169 3253 315
1169 3 0 316
1169 0 0 317
1.00300+ 3 2.99014+ 0 0 2 0 01169 4 2 318
0.00000+ 0 2.99014+ 0 0 2 0 01169 4 2 319
0.00000+ 0 0.00000+ 0 0 0 1 151169 4 2 320
15 2 1169 4 2 321
0.00000+ 0 1.00000- 5 0 0 1 21169 4 2 322
2 2 1169 4 2 323
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1 1169 4 2 324
0.00000+ 0 1.00000+ 5 0 0 1 21169 4 2 325
2 2 1169 4 2 326
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1 1169 4 2 327
0.00000+ 0 5.00000+ 5 0 0 1 211169 4 2 328
21 2 1169 4 2 329
-1.00000+ 0 8.51600- 1-9.00000- 1 7.98800- 1-8.00000- 1 7.44600- 11169 4 2 330
-7.00000- 1 6.95600- 1-6.00000- 1 6.49100- 1-5.00000- 1 6.06400- 11169 4 2 331
-4.00000- 1 5.69300- 1-3.00000- 1 5.35200- 1-2.00000- 1 5.04900- 11169 4 2 332
-1.00000- 1 4.76400- 1 0.00000+ 0 4.50800- 1 1.00000- 1 4.29000- 11169 4 2 333
2.00000- 1 4.09000- 1 3.00000- 1 3.91900- 1 4.00000- 1 3.77800- 11169 4 2 334
5.00000- 1 3.66300- 1 6.00000- 1 3.56900- 1 7.00000- 1 3.49300- 11169 4 2 335
8.00000- 1 3.46700- 1 9.00000- 1 3.44600- 1 1.00000+ 0 3.43700- 11169 4 2 336
0.00000+ 0 1.00000+ 6 0 0 1 211169 4 2 337
21 2 1169 4 2 338
-1.00000+ 0 1.19000+ 0-9.00000- 1 1.08600+ 0-8.00000- 1 9.79700- 11169 4 2 339
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