IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0
1.90000+ 4 3.87660+ 1 0 0 0 831150 1451 1
0.00000+ 0 0.00000+ 0 0 0 234 01150 1451 2
19-K GGA EVAL-1967 M.K.DRAKE 1150 1451 3
GA-7829 VOL-5 (1967) DIST-MAY74 1150 1451 4
EXTENDED TO 20 MEV FOR ENDF/B VERSION-IV 1150 1451 5
* * * * * * *1150 1451 6
NATURAL POTASSIUM 1150 1451 7
* * * * * * *1150 1451 8
FILE 3 1150 1451 9
TOTAL CROSS SECTION 1150 1451 10
UP TO 10 EV A SMOOTH CURVE WAS DRAWN THROUGH THE DATA OF JOKI(1) 1150 1451 11
FROM 10 EV TO 17 KEV THE TOTAL CROSS SECTION WAS OBTAINED FROM 1150 1451 12
A RESOLVED RESONANCE CALCULATION BASED ON THE TWO PRINCIPLE 1150 1451 13
ISOTOPES. PARAMETERS OF GOOD,ET AL (2) WERE USED 1150 1451 14
BETWEEN 17 KEV AND 315 KEV A SMOOTH CURVE WAS DRAWN THROUGH THE 1150 1451 15
1958 DATA MEASURED BY NEWSON (3). 1150 1451 16
THE TOTAL CROSS SECTION WAS VERY POORLY MEASURED BETWEEN 0.3 1150 1451 17
AND 1.0 MEV. THE RECOMMENDED CURVE WAS DRAWN THROUGH DATA 1150 1451 18
MEASURED BY PETERSON (4). 1150 1451 19
BETWEEN 0.9 AND 2.10 MEV AN AVERAGED WAS TAKEN OF DATA MEASURED 1150 1451 20
BY VAUGHN (5). STRUCTURE IN THE CROSS SECTION IS PRESENT BUT 1150 1451 21
COULD NOT BE ANALYZED FROM VAUGHNS DATA. 1150 1451 22
ABOVE 2.1 MEV DATA MEASURED BY FOSTER (6) AND DECONNINCK (7) 1150 1451 23
WERE USED. 1150 1451 24
RADIATIVE CAPTURE CROSS SECTION 1150 1451 25
THE LOW ENERGY CROSS SECTION WAS MODIFIED TO AGREE WITH THE 1150 1451 26
CSEWG NORMALIZATION AND STANDARDS SUBCOMMITTEE RECOMMENDED 1150 1451 27
2200 M/SEC VALUE OF *(2.10 BARNS)* 1150 1451 28
FROM 1.0-5 EV TO 20 KEV THE CROSS SECTION WAS OBTAINED FROM THE 1150 1451 29
RESOLVED RESONANCE PARAMETERS (SEE GA-7829 VOL-4) PLUS ADDITIONAL1150 1451 30
1/V COMPONENT TO OBTAIN THE DESIRED 0.0253 EV VALUE 1150 1451 31
ABOVE 20KEV THE CROSS SECTION WAS DRAWN THROUGH THE EXPERIMENTAL 1150 1451 32
POINTS AT 30.5 AND 65.0 KEV MEASURED BY MACKLIN ET AL (8). THE 1150 1451 33
SLOPE WAS TAKEN TO BE THE SAME AS WAS MEASURED FOR K-41 1150 1451 34
ACTIVATION BY STUPEGIA (9). 1150 1451 35
INELASTIC SCATTERING 1150 1451 36
THE FIRST THREE LEVEL EXCITATION CROSS SECTIONS WERE BASED ON 1150 1451 37
MEASUREMENTS BY LIND AND DAY (10) AND TOWLE AND GILBOY (11) FOR 1150 1451 38
NEUTRON ENERGIES UP TO 4.0 MEV. OTHER LEVEL EXCITATION CROSS 1150 1451 39
SECTIONS WERE OBTAINED USING THE ABACUS-II CODE (SEE REPORT) 1150 1451 40
CALCULATIONS WERE MADE FOR NEUTRON ENERGIES UP TO 6.8 MEV 1150 1451 41
ABOVE 6.8 MEV THE TOTAL INELASTIC CROSS SECTION WAS TAKEN AS THE 1150 1451 42
DIFFERENCE BETWEEN THE NON-ELASTIC CROSS SECTION AND THE SUM OF 1150 1451 43
(N,P) + (N,NP) + (N,A) + (N,NA) + (N,2N). SEE REPORT FOR THE 1150 1451 44
NON-ELASTIC CROSS SECTION. 1150 1451 45
N,PROTON CROSS SECTIONS 1150 1451 46
UP TO 700 KEV THE (N,P) CROSS SECTION IS 1/V WITH A 2200 M/SEC 1150 1451 47
VALUE OF 0.051 BARNS (NORMALIZATION AND STANDARDS SUBCOMMITTEE 1150 1451 48
RECOMMENDATION).FROM 700 KEV TO 4.0 MEV MEASURED VALUES FOR THE 1150 1451 49
(N,P0) + (N,P1) + (N,P2) CROSS SECTIONS WERE USED, BASED ON 1150 1451 50
MEASUREMENTS BY BASS ET AL (12,13). 1150 1451 51
BETWEEN 4.0 AND 8.0 MEV THE DATA OF BASS ET AL (13) WERE USED 1150 1451 52
THE RECOMMEND CURVE WAS EXTRAPOLATED THROUGH TO DATA MEASURED 1150 1451 53
BY LANGKAU (14) (12.6 TO 19.4 MEV) 1150 1451 54
THE (N,NP) CROSS SECTION WAS BASED ON MEASUREMENTS MADE BY 1150 1451 55
LANGKAU (14) AND BORMANN (15). 1150 1451 56
N,ALPHA CROSS SECTIONS 1150 1451 57
UP TO 1.0 MEV THE CROSS SECTION WAS TAKEN TO BE 1/V WITH A 1150 1451 58
2200 M/SEC VALUE OF 0.0046 BARNS (NORMALIZATION AND STANDARDS 1150 1451 59
SUBCOMMITTEE RECOMMENDATION). FROM 1.0 MEV TO 3.5 MEV THE (N,A) 1150 1451 60
CROSS SECTION WAS BASED ON (N,ALPH-ZERO) MEASUREMENTS OF 1150 1451 61
BASS (12,13). FROM 3.5 TO 8.0 MEV DATA OF BASS (14) WERE USED. 1150 1451 62
ABOVE 8.0 MEV THE DATA OF BORMANN (15,16) WERE USED. 1150 1451 63
THE (N,AN) CROSS SECTION WAS BASED ON DATA MEASURED BY BORMANN(151150 1451 64
N,2N CROSS SECTION 1150 1451 65
THE N,2N CROSS SECTION WAS BASED ON MEASUREMENTS MADE BY 1150 1451 66
BORMANN (17,18) FOR THE K-39(N,2N) K-38G REACTION AND BY 1150 1451 67
ARNOLD (19) AND BORMANN (17) FOR THE K-39 (N,2N) K-38M REACTION 1150 1451 68
* * * * * * *1150 1451 69
FILE 4 (ANGULAR DISTRIBUTIONS) 1150 1451 70
ELASTIC SCATTERING 1150 1451 71
FROM 0.03 TO 1.3 MEV THE DATA OF LANGSDORF, ET AL (20) WERE USED1150 1451 72
FROM 1.5 TO 3.8 MEV THE DATA OF TOWLE AND GILBOY (11) WERE USED1150 1451 73
ABOVE 4.0 MEV THE ABACUS-II CODE WAS USED 1150 1451 74
NON-ELASTIC REACTIONS 1150 1451 75
ANGULAR DISTRIBUTIONS FOR (N,2N), (N,NP), (N,NA), AN (N,INELASTIC1150 1451 76
CONTINUUM) NEUTRONS HAVE BEEN ASSUMED TO BE ISOTROPIC. 1150 1451 77
ANG DISTR. FOR NEUTRONS FROM DISCRETE LEVEL EXCITATION REACTIONS 1150 1451 78
HAVE BEEN CALCULATED USING THE ABACUS-II CODE. 1150 1451 79
* * * * * * *1150 1451 80
FILE 5 (ENERGY DISTRIBUTIONS) 1150 1451 81
AN EVAPORATION MODEL HAS BEEN USED FOR MT=16,22,28, AND 91 1150 1451 82
THE EFFECTIVE NUCLEAR TEMPERATURE WAS BASED ON 1150 1451 83
T(E) = B*SQRT(E/A) 1150 1451 84
E= INCIDENT NEUTRON ENERGY 1150 1451 85
A= NUCLEAR MASS 1150 1451 86
B= 2.5 FOR MT=91, = 1.59 FOR MT= 16, 22, AND 28 1150 1451 87
(SEE VOL-1 OF GA-7829) 1150 1451 88
* * * * * * *1150 1451 89
FILE 12 AND 13 PHOTON PRODUCTION CROSS SECTIONS 1150 1451 90
GAMMA RAYS FROM THERMAL NEUTRON CAPTURE WERE OBTAINED FROM DATA 1150 1451 91
SUMMARIZED BY ENDT AND VAN DER LEUN (21) AND GROSHEV ET AL (22) 1150 1451 92
AND MEASUREMENTS OF RUDOLPH AND GERSCH (23). 1150 1451 93
SINCE NO EPI-THERMAL MEASUREMENTS WERE AVAILABLE THE SAME SPECTRA1150 1451 94
WAS ASSUMED FOR ALL INCIDENT NEUTRON ENERGIES. 1150 1451 95
1150 1451 96
PHOTONS FROM DISCRETE INELASTIC LEVEL EXCITATION WERE OBTAINED 1150 1451 97
FROM THE LEVEL CROSS SECTION. ALL SIX LEVELS WERE ASSUMED TO 1150 1451 98
DECAY TO THE GROUND STATE. 1150 1451 99
PHOTONS FROM (N,P1), (N,P2) AND (N,A1) REACTIONS WERE OBTAINED 1150 1451 100
BY ANALYZING THE INDIVIDUAL REACTIONS. 1150 1451 101
*1150 1451 102
PHOTONS FROM NEUTRON REACTION ABOVE 7.0 MEV WAS BASED ON 1150 1451 103
A MEASUREMENT BY CALDWELL FOR PHOSPHOROUS. THESE DATA ARE 1150 1451 104
POORLY KNOWN. 1150 1451 105
*1150 1451 106
THE ANGULAR DISTRIBUTIONS FOR DISCRETE PHOTONS WAS CALCULATED 1150 1451 107
USING THE MANDY CODE. 1150 1451 108
THE ANGULAR DISTRIBUTIONS FOR CONTINUUM PHOTONS WAS ASSUMED 1150 1451 109
TO BE ISOTROPIC. 1150 1451 110
* * * * * * *1150 1451 111
REFERENCES 1150 1451 112
(1) E.G.JOKI, ET.AL., PHYS.REV.99,610 (1955) 1150 1451 113
(2) W.M.GOOD, ET.AL., PHYS.REV.109,926 (1958) 1150 1451 114
(3) H.W.NEWSON (DUKE U.) PRI.COMM.(SEE BNL-883,1964) 1150 1451 115
(4) R.E.PETERSON, PHYS.REV. 77, 747 (1950) 1150 1451 116
(5) F.J.VAUGHN, ET.AL., NUCL.SCI.ENG. 17, 325 (1963) 1150 1451 117
(6) D.G.FOSTER,JR. (PRI.COMM 1966) 1150 1451 118
(7) G.DECONNINCK, ET.AL., J.PHYS.(PARIS) 22, 652 (1961) 1150 1451 119
(8) R.L.MACKLIN, ET.AL., PHYS.REV. 129, 2695 (1963) 1150 1451 120
(9) D.C.STUPEGIA, ET.AL., IAEA CONF.ON NUCLEAR DATA (OCT.1966) 1150 1451 121
(10) D.A.LIND AND R.B.DAY, ANN.PHYS. 12, 485 (1961) 1150 1451 122
(11) J.H.TOWLE AND W.B. GILBOY, NUCL.PHYS. 72, 515 (1965) 1150 1451 123
(12) R.BASS, ET.AL., NUCL.PHYS. 28, 478 (1961) 1150 1451 124
(13) R.BASS, ET.AL., ENDC(E)-57, 1965 1150 1451 125
(14) R.LANGKAU, Z.NATURFORSH, 18A, 914 (1963) 1150 1451 126
(15) M.BORMANN, ET.AL., Z.NATURFORSH, 15A, 200 (1960) 1150 1451 127
(16) M.BORMANN, ET.AL., Z.PHYS.166, 477 (1962) 1150 1451 128
(17) M.BORMANN, NUCL.PHYS. 65, 257(1965) 1150 1451 129
(18) M.BORMANN, ET.AL.,NUCL.PHYS. 63, 438 (1965) 1150 1451 130
(19) D.M.ARNOLD, THESIS, U. OF GEORGIA (1965) 1150 1451 131
(20) A.LANGSDORF, ET.AL.,PHYS.REF.107,1077 (1957) 1150 1451 132
(21) P.M.ENDT AND C.VAN DER LEUN, NUCL.PHYS. 34, 1 (1962) 1150 1451 133
(22) L.V.GROSHEV, ET.AL.,ATLAS OF GAMMA-RAY SPECTRA FROM 1150 1451 134
RADIATIVE CAPTURE (TRANS),PERGAMMON PRESS, 1959 1150 1451 135
(23) W.RUDOLPH AND H.V.GERSCH, NUCL.PHYS. 71, 221 (1965) 1150 1451 136
(24) R.L.CALDWELL, ET.AL., NUCL.SCI.ENG. 8, 173 (1960) 1150 1451 137
* * * * * * *1150 1451 138
POTASSIUM--TRANSLATED JUN 69 FROM GA EVALUATION (GA-7829, 1967) 1150 1451 139
PLEASE REFER COMMENTS OR QUESTIONS REGARDING ERRORS IN TRANSLA- 1150 1451 140
TION OR IN FORMAT, OR CONCERNING THE TRANSLATION CODE (LATEX) 1150 1451 141
TO** DONALD J. DUDZIAK, UNIVERSITY OF CALIFORNIA, LOS ALAMOS 1150 1451 142
SCIENTIFIC LABORATORY, LOS ALAMOS, NM 87544 1150 1451 143
ANY COMMENTS REGARDING THE DATA EVALUATION SHOULD BE REFERRED TO 1150 1451 144
M.K. DRAKE, ET AL, THE AUTHORS OF GA-7829 (NDL-TR-89). THE PER- 1150 1451 145
MISSION OF MR. DRAKE TO TRANSLATE HIS EVALUATION IS GRATEFULLY 1150 1451 146
ACKNOWLEDGED.TRANSITION PROBABILITY ARRAYS FOR INELASTIC SCAT- 1150 1451 147
TERING WERE TAKEN FROM DIAGRAMS IN GA-7829,PART V. DATA FOR RTN 1150 1451 148
1032 AND 3032 WERE ASSIGNED MT=28, AS RECOMMENDED BY DRAKE. 1150 1451 149
TRANSLATION COMPLETED JULY, 1969. 1150 1451 150
PHOTON PRODUCTION FILES CONVERTED TO NEW FORMAT IN LA-4549(ENDF-1150 1451 151
102,REVISED,VOL. II) BY DONALD J. DUDZIAK JULY 1970. 1150 1451 152
NEUTRON AND PHOTON PRODUCTION FILES CONVERTED TO ENDF/B-II 1150 1451 153
FORMAT FOR THE RADIATION SHIELDING INFORMATION CENTER BY 1150 1451 154
SINGLETARY, PENNY, AND ROUSSIN. FILE 2 AND FILE 23 ALSO ADDED IN 1150 1451 155
MARCH 1971. 1150 1451 156
1150 1451 157
TABLE OF CONTENTS 1150 1451 158
***** ** ******** 1150 1451 159
** MF=1 ** GENERAL INFORMATION 1150 1451 160
1150 1451 161
1150 1451 162
MT= 1 TOTAL * 0.01 TO 2.0E+07 EV * 1150 1451 163
MT= 2 ELASTIC * SAME ENERGY RANGE AS MT=1 * 1150 1451 164
MT= 3 NONELASTIC * SAME ENERGY RANGE AS MT=1 * 1150 1451 165
MT= 4 TOTAL INELASTIC (N,N-PRIME) GAMMA * Q=-0.03MEV1150 1451 166
MT= 16 (N,2N) * Q= -13.071 MEV 1150 1451 167
MT= 22 (N,N-PRIME)ALPHA * Q= -7.365 MEV 1150 1451 168
MT= 28 (N,N-PRIME)P * Q= -6.424 MEV 1150 1451 169
MT= 51 (N,N-PRIME) TO THE 1ST EXCITED STATE*2.526 MEV1150 1451 170
MT= 52 (N,N-PRIME) TO THE 2ND EXCITED STATE*2.817 MEV1150 1451 171
MT= 53 (N,N-PRIME) TO THE 3RD EXCITED STATE*3.021 MEV1150 1451 172
MT= 54 (N,N-PRIME) TO THE 4TH EXCITED STATE*3.603 MEV1150 1451 173
MT= 55 (N,N-PRIME) TO THE 5TH EXCITED STATE*3.879 MEV1150 1451 174
MT= 56 (N,N-PRIME) TO THE 6TH EXCITED STATE*3.935 MEV1150 1451 175
MT= 57 (N,N-PRIME) TO THE 7TH EXCITED STATE*4.122 MEV1150 1451 176
MT= 58 (N,N-PRIME) TO THE 8TH EXCITED STATE*4.678 MEV1150 1451 177
MT= 59 (N,N-PRIME) TO THE 9TH EXCITED STATE*5.280 MEV1150 1451 178
MT= 60 (N,N-PRIME) TO THE 10TH EXCITED STATE*5.37 MEV1150 1451 179
MT= 61 (N,N-PRIME) TO THE 11TH EXCITED STATE*5.62 MEV1150 1451 180
MT= 62 (N,N-PRIME) TO THE 12TH EXCITED STATE*5.74 MEV1150 1451 181
MT= 63 (N,N-PRIME) TO THE 13TH EXCITED STATE*5.96 MEV1150 1451 182
MT= 64 (N,N-PRIME) TO THE 14TH EXCITED STATE*6.12 MEV1150 1451 183
MT= 65 (N,N-PRIME) TO THE 15TH EXCITED STATE*6.21 MEV1150 1451 184
MT= 66 (N,N-PRIME) TO THE 16TH EXCITED STATE*6.35 MEV1150 1451 185
MT= 67 (N,N-PRIME) TO THE 17TH EXCITED STATE*6.50 MEV1150 1451 186
MT= 91 (N,N-PRIME) TO THE CONTINIUUM 1150 1451 187
MT=102 (N,GAMMA) 1150 1451 188
MT=103 (N,P) * Q= 0.0 MEV 1150 1451 189
MT=107 (N,ALPHA) * Q= 0.0 MEV 1150 1451 190
MT=251 MU-BAR (L SYSTEM) * SAME ENERGY RANGE AS MT=1*1150 1451 191
1150 1451 192
** MF=4 ** SECONDARY ANGULAR DISTRIBUTIONS * TABULAR * C SYSTEM1150 1451 193
MT= 2 ELASTIC 1150 1451 194
MT= 51 (N,N-PRIME) TO THE 1ST EXCITED STATE 1150 1451 195
MT= 52 (N,N-PRIME) TO THE 2ND EXCITED STATE 1150 1451 196
MT= 53 (N,N-PRIME) TO THE 3RD EXCITED STATE 1150 1451 197
MT= 54 (N,N-PRIME) TO THE 4TH EXCITED STATE 1150 1451 198
MT= 55 (N,N-PRIME) TO THE 5TH EXCITED STATE 1150 1451 199
MT= 56 (N,N-PRIME) TO THE 6TH EXCITED STATE 1150 1451 200
MT= 57 (N,N-PRIME) TO THE 7TH EXCITED STATE 1150 1451 201
MT= 58 (N,N-PRIME) TO THE 8TH EXCITED STATE 1150 1451 202
MT= 59 (N,N-PRIME) TO THE 9TH EXCITED STATE (ISO.) 1150 1451 203
MT= 60 (N,N-PRIME) TO THE 10TH EXCITED STATE (ISO.) 1150 1451 204
1150 1451 205
** MF=5 ** SECONDARY ENERGY DISTRIBUTIONS * ALL LAW 1 (TABULAR)1150 1451 206
MT= 22 (N,N-PRIME)ALPHA 1150 1451 207
MT= 28 (N,N-PRIME)P 1150 1451 208
MT= 91 (N,N-PRIME) TO THE CONTINUUM 1150 1451 209
1150 1451 210
** MF=12 ** MULTIPLICITIES OR TRANSITION PROBABILITIES 1150 1451 211
MT= 51 (N,N-PRIME) TO THE 1ST EXCITED STATE* OPTION2 1150 1451 212
MT= 52 (N,N-PRIME) TO THE 2ND EXCITED STATE* OPTION2 1150 1451 213
MT= 53 (N,N-PRIME) TO THE 3RD EXCITED STATE* OPTION2 1150 1451 214
MT= 54 (N,N-PRIME) TO THE 4TH EXCITED STATE* OPTION2 1150 1451 215
MT= 91 (N,N-PRIME) TO THE CONTINUUM * OPTION 1 1150 1451 216
MT=102 (N,GAMMA) * OPTION 1 1150 1451 217
MT=103 (N,N-PRIME)P *OPTION 1* 1150 1451 218
MT=107 (N,N-PRIME)ALPHA *OPTION 1* 1150 1451 219
** MF=13 ** PHOTON PRODUCTION CROSS SECTIONS 1150 1451 220
MT= 51 PHOTONS FROM DE-EXCITATION OF 1ST STATE 1150 1451 221
MT= 52 PHOTONS FROM DE-EXCITATION OF 2ND STATE 1150 1451 222
MT= 53 PHOTONS FROM DE-EXCITATION OF 3RD STATE 1150 1451 223
MT= 54 PHOTONS FROM DE-EXCITATION OF 4TH STATE 1150 1451 224
MT= 55 PHOTONS FROM DE-EXCITATION OF 5TH STATE 1150 1451 225
MT= 56 PHOTONS FROM DE-EXCITATION OF 6TH STATE 1150 1451 226
** MF=14 ** PHOTON ANGULAR DISTRIBUTIONS * TABULAR 1150 1451 227
MT= 51 (N,N-PRIME) TO THE 1ST EXCITED STATE (ISO.) 1150 1451 228
MT= 52 (N,N-PRIME) TO THE 2ND EXCITED STATE 1150 1451 229
MT= 53 (N,N-PRIME) TO THE 3RD EXCITED STATE 1150 1451 230
MT= 54 (N,N-PRIME) TO THE 4TH EXCITED STATE 1150 1451 231
MT= 55 (N,N-PRIME) TO THE 5TH EXCITED STATE 1150 1451 232
MT= 56 (N,N-PRIME) TO THE 6TH EXCITED STATE 1150 1451 233
MT=103 (N,P-GAMMA) (ISO.) 1150 1451 234
* * * * * * *1150 1451 235
* * * * * * *1150 1451 236
1 451 319 1150 1451 237
2 151 4 1150 1451 238
3 1 247 1150 1451 239
3 2 237 1150 1451 240
3 4 87 1150 1451 241
3 16 8 1150 1451 242
3 22 14 1150 1451 243
3 28 16 1150 1451 244
3 51 18 1150 1451 245
3 52 18 1150 1451 246
3 53 17 1150 1451 247
3 54 15 1150 1451 248
3 55 14 1150 1451 249
3 56 14 1150 1451 250
3 57 13 1150 1451 251
3 58 11 1150 1451 252
3 59 9 1150 1451 253
3 60 9 1150 1451 254
3 61 8 1150 1451 255
3 62 7 1150 1451 256
3 63 7 1150 1451 257
3 64 6 1150 1451 258
3 65 6 1150 1451 259
3 66 5 1150 1451 260
3 67 5 1150 1451 261
3 91 66 1150 1451 262
3 102 26 1150 1451 263
3 103 87 1150 1451 264
3 107 74 1150 1451 265
3 251 26 1150 1451 266
3 252 26 1150 1451 267
3 253 26 1150 1451 268
4 2 1099 1150 1451 269
4 16 10 1150 1451 270
4 22 10 1150 1451 271
4 28 10 1150 1451 272
4 51 94 1150 1451 273
4 52 94 1150 1451 274
4 53 85 1150 1451 275
4 54 76 1150 1451 276
4 55 76 1150 1451 277
4 56 76 1150 1451 278
4 57 67 1150 1451 279
4 58 58 1150 1451 280
4 59 10 1150 1451 281
4 60 10 1150 1451 282
4 61 10 1150 1451 283
4 62 10 1150 1451 284
4 63 10 1150 1451 285
4 64 10 1150 1451 286
4 65 10 1150 1451 287
4 66 10 1150 1451 288
4 67 10 1150 1451 289
4 91 10 1150 1451 290
5 16 7 1150 1451 291
5 22 7 1150 1451 292
5 28 7 1150 1451 293
5 91 7 1150 1451 294
12 51 3 1150 1451 295
12 52 3 1150 1451 296
12 53 3 1150 1451 297
12 54 3 1150 1451 298
12 91 6 1150 1451 299
12 102 145 1150 1451 300
12 103 39 1150 1451 301
12 107 9 1150 1451 302
13 51 16 1150 1451 303
13 52 16 1150 1451 304
13 53 16 1150 1451 305
13 54 15 1150 1451 306
13 55 14 1150 1451 307
13 56 14 1150 1451 308
14 51 1 1150 1451 309
14 52 96 1150 1451 310
14 53 87 1150 1451 311
14 54 24 1150 1451 312
14 55 78 1150 1451 313
14 56 69 1150 1451 314
14 91 1 1150 1451 315
14 102 1 1150 1451 316
14 103 1 1150 1451 317
14 107 1 1150 1451 318
15 91 90 1150 1451 319
1150 1 0 320
1150 0 0 321
1.90000+ 4 3.87660+ 1 0 0 1 01150 2151 322
1.90390+ 4 1.00000+ 0 0 0 1 01150 2151 323
1.00000- 5 1.00000+ 5 0 0 0 01150 2151 324
1.50000+ 0 3.45000- 1 0 0 0 01150 2151 325
1150 2 0 326
1150 0 0 327
1.90000+ 4 3.87660+ 1 0 99 0 01150 3 1 328
0.00000+ 0 0.00000+ 0 0 0 1 7311150 3 1 329
731 5 1150 3 1 330
1.00000- 5 1.10627+ 2 1.00000- 4 3.64874+ 1 1.00000- 3 1.30427+ 11150 3 1 331
1.00000- 2 5.62864+ 0 2.00000- 2 4.62444+ 0 2.53000- 2 4.35560+ 01150 3 1 332
4.00000- 2 3.90436+ 0 6.00000- 2 3.55977+ 0 1.00000- 1 3.23427+ 01150 3 1 333
2.00000- 1 2.82669+ 0 4.00000- 1 2.57213+ 0 6.00000- 1 2.47265+ 01150 3 1 334
1.00000+ 0 2.35287+ 0 2.00000+ 0 2.30045+ 0 4.00000+ 0 2.21944+ 01150 3 1 335
6.00000+ 0 2.16098+ 0 1.00000+ 1 2.06043+ 0 2.00000+ 1 1.96867+ 01150 3 1 336
4.00000+ 1 1.84921+ 0 6.00000+ 1 1.78926+ 0 1.00000+ 2 1.68149+ 01150 3 1 337
2.00000+ 2 1.53084+ 0 4.00000+ 2 1.42054+ 0 6.00000+ 2 1.36040+ 01150 3 1 338
1.00000+ 3 1.27034+ 0 1.50000+ 3 1.18018+ 0 2.00000+ 3 1.12035+ 01150 3 1 339
2.50000+ 3 1.08018+ 0 3.00000+ 3 1.05916+ 0 3.10000+ 3 9.44359- 11150 3 1 340
3.20000+ 3 8.01156- 1 3.30000+ 3 9.23154- 1 3.35000+ 3 1.56802+ 11150 3 1 341
3.40000+ 3 3.40200+ 2 3.45000+ 3 1.20502+ 1 3.50000+ 3 4.43015+ 01150 3 1 342
3.60000+ 3 2.87565+ 0 3.70000+ 3 2.52375+ 0 3.80000+ 3 2.28154+ 01150 3 1 343
3.90000+ 3 2.07614+ 0 4.00000+ 3 1.92554+ 0 4.20000+ 3 1.71534+ 01150 3 1 344
4.40000+ 3 1.56513+ 0 4.60000+ 3 1.46503+ 0 4.80000+ 3 1.38493+ 01150 3 1 345
5.00000+ 3 1.32483+ 0 5.20000+ 3 1.38472+ 0 5.30000+ 3 1.80532+ 01150 3 1 346
5.35000+ 3 2.87212+ 0 5.40000+ 3 1.69351+ 1 5.45000+ 3 4.05212+ 01150 3 1 347
5.50000+ 3 2.75322+ 0 5.60000+ 3 1.99452+ 0 5.80000+ 3 1.52442+ 01150 3 1 348
6.00000+ 3 1.32431+ 0 7.00000+ 3 1.18411+ 0 8.00000+ 3 1.05390+ 01150 3 1 349
8.20000+ 3 9.73798- 1 8.40000+ 3 8.83796- 1 8.60000+ 3 7.86395- 11150 3 1 350
8.80000+ 3 7.14194- 1 9.00000+ 3 1.64509+ 0 9.10000+ 3 8.00309+ 01150 3 1 351
9.15000+ 3 3.19601+ 1 9.20000+ 3 1.45380+ 2 9.25000+ 3 5.06501+ 11150 3 1 352
9.30000+ 3 2.05601+ 1 9.40000+ 3 7.09609+ 0 9.60000+ 3 3.44059+ 01150 3 1 353
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