Retrieved by E4-util: 2010/02/01,11:42:32 1 0 0 0 3.708500+4 8.418240+1 1 0 59 03785 1451 1 0.000000+0 1.0000E+00 0 0 0 63785 1451 2 1.000000+0 2.0000E+07 0 0 10 03785 1451 3 0.000000+0 0.000000+0 0 0 263 463785 1451 4 37-Rb- 85 IPPE EVAL-AUG06 Nikolaev M.N. 3785 1451 5 DIST-DEC06 3785 1451 6 ----RUSFOND Material 3785 3785 1451 7 -----Incident neutron data 3785 1451 8 ------ENDF-6 Format 3785 1451 9 3785 1451 10 RUSFOND DESCRIPTION 3785 1451 11 (See RUSFOND manual for details) 3785 1451 12 3785 1451 13 Data from ENDF/B-VII are adopted 3785 1451 14 ----------------------------------------------------------- 3785 1451 15 3785 1451 16 ENDF/B-VII description 3785 1451 17 3785 1451 18 -------------------------------------------------------- 3785 1451 19 EVAL-MAR90 JNDC FPND WG + S.F. Mughabghab 3785 1451 20 3785 1451 21 ============================================================== 3785 1451 22 File produced by WPEC Subgroup 23 in 2004-2005 3785 1451 23 - WPEC: NEA Working Party on Evaluation Cooperation 3785 1451 24 - SG23: International library of fission product evaluations 3785 1451 25 3785 1451 26 CONVERTED FROM JENDL-3.3 BY NNDC OCT 2004 3785 1451 27 Corrected threshold energy secondary energy distributions 3785 1451 28 in MF=5. 3785 1451 29 Corrected interpolation in MF=5. 3785 1451 30 File obtained by merging: &&3785 1451 31 - Resolved Resonances (MLBW) <8.468 keV : Ref.1 &&3785 1451 32 - Unresolved Resonances 8.468 keV - 100 keV : JENDL 3 &&3785 1451 33 - Fast neutron region >100 keV : JENDL 3 &&3785 1451 34 &&3785 1451 35 Calculated thermal cross sections & resonance integrals: &&3785 1451 36 --------------------------------------------- &&3785 1451 37 Reaction Cross section Res. integral &&3785 1451 38 (barn) (barn) &&3785 1451 39 Total 6.7463E+00 - &&3785 1451 40 Elastic 6.2529E+00 - &&3785 1451 41 Capture 4.9343E-01 7.61E+00 &&3785 1451 42 --------------------------------------------- &&3785 1451 43 3785 1451 44 Reference: 3785 1451 45 1) S.F.Mughabghab: Atlas of Neutron Resonances, to be 3785 1451 46 published by Elsevier, 2006 (5-th edition of BNL-325) 3785 1451 47 3785 1451 48 ============================================================== 3785 1451 49 3785 1451 50 84-10 EVALUATION FOR JENDL-2 WAS MADE BY JNDC FPND W.G./1/ 3785 1451 51 90-03 MODIFICATION FOR JENDL-3 WAS MADE/2/. 3785 1451 52 3785 1451 53 MF = 1 GENERAL INFORMATION 3785 1451 54 MT=451 COMMENTS AND DICTIONARY 3785 1451 55 3785 1451 56 MF = 2 RESONANCE PARAMETERS 3785 1451 57 MT=151 RESOLVED AND UNRESOLVED RESONANCE PARAMETERS 3785 1451 58 RESOLVED RESONANCE REGION (MLBW FORMULA) : BELOW 8.468 KEV 3785 1451 59 RESONANCE PARAMETERS OF JENDL-2 WERE MODIFIED AS FOLLOWS : 3785 1451 60 EVALUATION OF JENDL-2 WAS PERFORMED ON THE BASIS OF THE DATA 3785 1451 61 MEASURED BY OHKUBO ET AL./3/ AMONG 138 LEVELS MEASURED IN THE 3785 1451 62 ENERGY REGION UP TO 18.6 KEV, 116 RESONANCE LEVELS WERE 3785 1451 63 ASSUMED TO BE S-WAVE, AND REMAINING 22 LEVELS WERE ESTIMATED 3785 1451 64 TO BE P-WAVE. NEUTRON WIDTHS OF ALL LEVELS WERE DETERMINED 3785 1451 65 FROM THE 2G*(NEUTRON WIDTH) MEASURED BY OHKUBO ET AL. 3785 1451 66 HOWEVER, THE VALUE OF TOTAL SPIN J FOR EACH RESONANCE LEVEL 3785 1451 67 WAS UNKNOWN EXCEPT 13 LEVELS ASSIGNED BY OHKUBO ET AL., AND 3785 1451 68 THE TARGET SPIN OF 2.5 WAS ADOPTED AS J FOR J-UNKNOWN LEVELS. 3785 1451 69 RADIATION WIDTHS WERE OBTAINED FOR 10 LEVELS BELOW 2.6 KEV 3785 1451 70 FROM THE MEASUREMENT BY OHKUBO ET AL. AVERAGE RADIATION WIDTH3785 1451 71 WAS ALSO ESTIMATED TO BE 328+-18 MEV BY OHKUBO ET AL., AND WAS3785 1451 72 ADOPTED FOR THE OTHER LEVELS. A NEGATIVE RESONANCE WAS ADDED 3785 1451 73 AT -943 EV SO AS TO REPRODUCE THE THERMAL CAPTURE CROSS 3785 1451 74 SECTION OF 480+-10 MB GIVEN BY MUGHABGHAB ET AL./4/ 3785 1451 75 3785 1451 76 FOR JENDL-3, THE TOTAL SPIN J OF 125 RESONANCE LEVELS WAS 3785 1451 77 TENTATIVELY ESTIMATED WITH A RANDOM NUMBER METHOD. NEUTRON 3785 1451 78 WIDTHS OF THESE LEVELS WERE MODIFIED ON THE BASIS OF THE 3785 1451 79 ESTIMATED J VALUES. NEUTRON AND RADIATION WIDTHS OF THE 3785 1451 80 NEGATIVE RESONANCE LEVEL WERE ALSO MODIFIED SO AS TO REPRODUCE3785 1451 81 THE THERMAL CAPTURE CROSS SECTION ACCORDING TO THE ABOVE 3785 1451 82 MODIFICATION OF THE NEUTRON WIDTHS. SCATTERING RADIUS WAS 3785 1451 83 TAKEN FROM THE GRAPH (FIG. 1, PART A) GIVEN BY MUGHABGHAB ET 3785 1451 84 AL. 3785 1451 85 3785 1451 86 UNRESOLVED RESONANCE REGION : 8.468 KEV - 100 KEV 3785 1451 87 UNRESOLVED RESONANCE PARAMETERS WERE ADOPTED FROM JENDL-2. 3785 1451 88 THE NEUTRON STRENGTH FUNCTION, S0, WAS TAKEN FROM THE 3785 1451 89 RECOMMENDATION IN REF./5/, AND S1 AND S2 WERE CALCULATED WITH 3785 1451 90 OPTICAL MODEL CODE CASTHY/6/. THE OBSERVED LEVEL SPACING WAS 3785 1451 91 DETERMINED TO REPRODUCE THE CAPTURE CROSS SECTION CALCULATED 3785 1451 92 WITH CASTHY. THE EFFECTIVE SCATTERING RADIUS WAS OBTAINED 3785 1451 93 FROM FITTING TO THE CALCULATED TOTAL CROSS SECTION AT 100 KEV.3785 1451 94 3785 1451 95 TYPICAL VALUES OF THE PARAMETERS AT 70 KEV: 3785 1451 96 S0 = 1.000E-4, S1 = 2.920E-4, S2 = 0.650E-4, SG = 21.4E-4, 3785 1451 97 GG = 0.205 EV, R = 6.828 FM. 3785 1451 98 3785 1451 99 3785 1451 100 CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS (BARNS) 3785 1451 101 2200 M/S RES. INTEG. 3785 1451 102 TOTAL 6.334 - 3785 1451 103 ELASTIC 5.854 - 3785 1451 104 CAPTURE 0.4800 8.73 3785 1451 105 3785 1451 106 MF = 3 NEUTRON CROSS SECTIONS 3785 1451 107 BELOW 100 KEV, RESONANCE PARAMETERS WERE GIVEN. 3785 1451 108 ABOVE 100 KEV, THE SPHERICAL OPTICAL AND STATISTICAL MODEL 3785 1451 109 CALCULATION WAS PERFORMED WITH CASTHY, BY TAKING ACCOUNT OF 3785 1451 110 COMPETING REACTIONS, OF WHICH CROSS SECTIONS WERE CALCULATED 3785 1451 111 WITH PEGASUS/7/ STANDING ON A PREEQUILIBRIUM AND MULTI-STEP 3785 1451 112 EVAPORATION MODEL. THE OMP'S FOR NEUTRON GIVEN IN TABLE 1 WERE 3785 1451 113 DETERMINED TO REPRODUCE A SYSTEMATIC TREND OF THE TOTAL CROSS 3785 1451 114 SECTION BY CHANGING R0, RS AND RSO OF IIJIMA-KAWAI POTENTIAL/8/.3785 1451 115 THE OMP'S FOR CHARGED PARTICLES ARE AS FOLLOWS: 3785 1451 116 PROTON = PEREY/9/ 3785 1451 117 ALPHA = HUIZENGA AND IGO/10/ 3785 1451 118 DEUTERON = LOHR AND HAEBERLI/11/ 3785 1451 119 HELIUM-3 AND TRITON = BECCHETTI AND GREENLEES/12/ 3785 1451 120 PARAMETERS FOR THE COMPOSITE LEVEL DENSITY FORMULA OF GILBERT 3785 1451 121 AND CAMERON/13/ WERE EVALUATED BY IIJIMA ET AL./14/ MORE 3785 1451 122 EXTENSIVE DETERMINATION AND MODIFICATION WERE MADE IN THE 3785 1451 123 PRESENT WORK. TABLE 2 SHOWS THE LEVEL DENSITY PARAMETERS USED 3785 1451 124 IN THE PRESENT CALCULATION. ENERGY DEPENDENCE OF SPIN CUT-OFF 3785 1451 125 PARAMETER IN THE ENERGY RANGE BELOW E-JOINT IS DUE TO GRUPPELAAR3785 1451 126 /15/. 3785 1451 127 3785 1451 128 MT = 1 TOTAL 3785 1451 129 SPHERICAL OPTICAL MODEL CALCULATION WAS ADOPTED. 3785 1451 130 3785 1451 131 MT = 2 ELASTIC SCATTERING 3785 1451 132 CALCULATED AS (TOTAL - SUM OF PARTIAL CROSS SECTIONS). 3785 1451 133 3785 1451 134 MT = 4, 51 - 91 INELASTIC SCATTERING 3785 1451 135 SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WAS 3785 1451 136 ADOPTED. THE LEVEL SCHEME WAS TAKEN FROM REF./16/. 3785 1451 137 3785 1451 138 NO. ENERGY(MEV) SPIN-PARITY 3785 1451 139 GR. 0.0 5/2 - 3785 1451 140 1 0.1513 3/2 - 3785 1451 141 2 0.2810 1/2 - 3785 1451 142 3 0.5140 9/2 + 3785 1451 143 4 0.7350 3/2 - 3785 1451 144 5 0.8685 7/2 - 3785 1451 145 6 0.8830 1/2 - 3785 1451 146 7 0.9500 5/2 + 3785 1451 147 8 1.1750 7/2 + 3785 1451 148 LEVELS ABOVE 1.294 MEV WERE ASSUMED TO BE OVERLAPPING. 3785 1451 149 3785 1451 150 MT = 102 CAPTURE 3785 1451 151 SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WITH 3785 1451 152 CASTHY WAS ADOPTED. DIRECT AND SEMI-DIRECT CAPTURE CROSS 3785 1451 153 SECTIONS WERE ESTIMATED ACCORDING TO THE PROCEDURE OF BENZI 3785 1451 154 AND REFFO/17/ AND NORMALIZED TO 1 MILLI-BARN AT 14 MEV. 3785 1451 155 3785 1451 156 THE GAMMA-RAY STRENGTH FUNCTION (22.0E-04) WAS ADJUSTED TO 3785 1451 157 REPRODUCE THE CAPTURE CROSS SECTION OF 335 MILLI-BARNS AT 25 3785 1451 158 KEV MEASURED BY LAKSHMANA ET AL./18/ 3785 1451 159 3785 1451 160 MT = 16 (N,2N) CROSS SECTION 3785 1451 161 MT = 17 (N,3N) CROSS SECTION 3785 1451 162 MT = 22 (N,N'A) CROSS SECTION 3785 1451 163 MT = 28 (N,N'P) CROSS SECTION 3785 1451 164 MT = 32 (N,N'D) CROSS SECTION 3785 1451 165 MT =103 (N,P) CROSS SECTION 3785 1451 166 MT =104 (N,D) CROSS SECTION 3785 1451 167 MT =105 (N,T) CROSS SECTION 3785 1451 168 MT =106 (N,HE3) CROSS SECTION 3785 1451 169 MT =107 (N,ALPHA) CROSS SECTION 3785 1451 170 THESE REACTION CROSS SECTIONS WERE CALCULATED WITH THE 3785 1451 171 PREEQUILIBRIUM AND MULTI-STEP EVAPORATION MODEL CODE PEGASUS. 3785 1451 172 3785 1451 173 THE KALBACH'S CONSTANT K (= 281.4) WAS ESTIMATED BY THE 3785 1451 174 FORMULA DERIVED FROM KIKUCHI-KAWAI'S FORMALISM/19/ AND LEVEL 3785 1451 175 DENSITY PARAMETERS. 3785 1451 176 3785 1451 177 FINALLY, THE (N,2N), (N,P) AND (N,ALPHA) CROSS SECTIONS WERE 3785 1451 178 NORMALIZED TO THE FOLLOWING VALUES AT 14.5 MEV: 3785 1451 179 (N,2N) 1050.00 MB (RECOMMENDED BY BYCHKOV+/20/) 3785 1451 180 (N,P) 17.40 MB (SYSTEMATICS OF FORREST/21/) 3785 1451 181 (N,ALPHA) 6.65 MB (RECOMMENDED BY FORREST/21/) 3785 1451 182 3785 1451 183 MT = 251 MU-BAR 3785 1451 184 CALCULATED WITH CASTHY. 3785 1451 185 3785 1451 186 MF = 4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 3785 1451 187 LEGENDRE POLYNOMIAL COEFFICIENTS FOR ANGULAR DISTRIBUTIONS ARE 3785 1451 188 GIVEN IN THE CENTER-OF-MASS SYSTEM FOR MT=2 AND DISCRETE INELAS-3785 1451 189 TIC LEVELS, AND IN THE LABORATORY SYSTEM FOR MT=91. THEY WERE 3785 1451 190 CALCULATED WITH CASTHY. FOR OTHER REACTIONS, ISOTROPIC DISTRI- 3785 1451 191 BUTIONS IN THE LABORATORY SYSTEM WERE ASSUMED. 3785 1451 192 3785 1451 193 MF = 5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS 3785 1451 194 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS WERE CALCULATED WITH 3785 1451 195 PEGASUS FOR INELASTIC SCATTERING TO OVERLAPPING LEVELS AND FOR 3785 1451 196 OTHER NEUTRON EMITTING REACTIONS. 3785 1451 197 3785 1451 198 TABLE 1 NEUTRON OPTICAL POTENTIAL PARAMETERS 3785 1451 199 3785 1451 200 DEPTH (MEV) RADIUS(FM) DIFFUSENESS(FM) 3785 1451 201 ---------------------- ------------ --------------- 3785 1451 202 V = 46.0-0.25E R0 = 5.7 A0 = 0.62 3785 1451 203 WS = 7.0 RS = 6.2 AS = 0.35 3785 1451 204 VSO= 7.0 RSO= 5.7 ASO= 0.62 3785 1451 205 THE FORM OF SURFACE ABSORPTION PART IS DER. WOODS-SAXON TYPE. 3785 1451 206 3785 1451 207 TABLE 2 LEVEL DENSITY PARAMETERS 3785 1451 208 3785 1451 209 NUCLIDE SYST A(1/MEV) T(MEV) C(1/MEV) EX(MEV) PAIRING 3785 1451 210 --------------------------------------------------------------- 3785 1451 211 35-BR- 81 1.290E+01 8.310E-01 3.275E+00 7.733E+00 1.570E+00 3785 1451 212 35-BR- 82 1.266E+01 6.900E-01 5.789E+00 3.665E+00 0.0 3785 1451 213 35-BR- 83 1.324E+01 7.830E-01 2.683E+00 6.978E+00 1.460E+00 3785 1451 214 35-BR- 84 * 1.302E+01 7.738E-01 1.393E+01 5.216E+00 0.0 3785 1451 215 3785 1451 216 36-KR- 82 1.319E+01 7.810E-01 4.961E-01 8.191E+00 2.740E+00 3785 1451 217 36-KR- 83 1.483E+01 6.700E-01 2.532E+00 5.589E+00 1.170E+00 3785 1451 218 36-KR- 84 9.970E+00 9.600E-01 4.942E-01 8.590E+00 2.630E+00 3785 1451 219 36-KR- 85 1.024E+01 8.900E-01 1.570E+00 6.261E+00 1.170E+00 3785 1451 220 3785 1451 221 37-RB- 83 * 1.400E+01 7.831E-01 3.730E+00 7.579E+00 1.570E+00 3785 1451 222 37-RB- 84 1.106E+01 8.060E-01 5.598E+00 4.438E+00 0.0 3785 1451 223 37-RB- 85 1.190E+01 8.690E-01 2.827E+00 7.561E+00 1.460E+00 3785 1451 224 37-RB- 86 1.002E+01 8.500E-01 3.954E+00 4.312E+00 0.0 3785 1451 225 --------------------------------------------------------------- 3785 1451 226 SYST: * = LDP'S WERE DETERMINED FROM SYSTEMATICS. 3785 1451 227 3785 1451 228 SPIN CUTOFF PARAMETERS WERE CALCULATED AS 0.146*SQRT(A)*A**(2/3).3785 1451 229 IN THE CASTHY CALCULATION, SPIN CUTOFF FACTORS AT 0 MEV WERE 3785 1451 230 ASSUMED TO BE 4.75 FOR RB- 85 AND 5.0 FOR RB- 86. 3785 1451 231 3785 1451 232 REFERENCES 3785 1451 233 1) AOKI, T. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR BASIC 3785 1451 234 AND APPLIED SCIENCE, SANTA FE., VOL. 2, P.1627 (1985). 3785 1451 235 2) KAWAI, M. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR SCIENCE3785 1451 236 AND TECHNOLOGY, MITO, P. 569 (1988). 3785 1451 237 3) OHKUBO, M., MIZUMOTO, M., AND KAWARASAKI, Y.: 3785 1451 238 NUCL. SCI. TECH. 21, 254 (1984). 3785 1451 239 4) MUGHABGHAB, S.F. ET AL.: "NEUTRON CROSS SECTIONS, VOL. I, 3785 1451 240 PART A", ACADEMIC PRESS (1981). 3785 1451 241 5) MUGHABGHAB, S.F. AND GARBER, D.I.: "NEUTRON CROSS SECTIONS, 3785 1451 242 VOL. 1, RESONANCE PARAMETERS", BNL 325, 3RD ED., VOL. 1(1973).3785 1451 243 6) IGARASI, S.: J. NUCL. SCI. TECHNOL., 12, 67 (1975). 3785 1451 244 7) IIJIMA, S. ET AL.: JAERI-M 87-025, P. 337 (1987). 3785 1451 245 8) IIJIMA, S. AND KAWAI, M.: J. NUCL. SCI. TECHNOL., 20, 77 3785 1451 246 (1983). 3785 1451 247 9) PEREY, F.G: PHYS. REV. 131, 745 (1963). 3785 1451 248 10) HUIZENGA, J.R. AND IGO, G.: NUCL. PHYS. 29, 462 (1962). 3785 1451 249 11) LOHR, J.M. AND HAEBERLI, W.: NUCL. PHYS. A232, 381 (1974). 3785 1451 250 12) BECCHETTI, F.D., JR. AND GREENLEES, G.W.: POLARIZATION 3785 1451 251 PHENOMENA IN NUCLEAR REACTIONS ((EDS) H.H. BARSHALL AND 3785 1451 252 W. HAEBERLI), P. 682, THE UNIVERSITY OF WISCONSIN PRESS. 3785 1451 253 (1971). 3785 1451 254 13) GILBERT, A. AND CAMERON, A.G.W.: CAN. J. PHYS., 43, 1446 3785 1451 255 (1965). 3785 1451 256 14) IIJIMA, S., ET AL.: J. NUCL. SCI. TECHNOL. 21, 10 (1984). 3785 1451 257 15) GRUPPELAAR, H.: ECN-13 (1977). 3785 1451 258 16) MATSUMOTO, J.: PRIVATE COMMUNICATION (1981). 3785 1451 259 17) BENZI, V. AND REFFO, G.: CCDN-NW/10 (1969). 3785 1451 260 18) LAKSHMANA, RAO, A., ET AL.: "PROC. SYMPOSIUM ON NUCLEAR 3785 1451 261 PHYSICS, MADURAI, INDIA 1970", VOL.2, 19. 3785 1451 262 19) KIKUCHI, K. AND KAWAI, M.: "NUCLEAR MATTER AND NUCLEAR 3785 1451 263 REACTIONS", NORTH HOLLAND (1968). 3785 1451 264 20) BYCHKOV, V.M. ET AL.: INDC(CCP)-146/LJ (1980). 3785 1451 265 21) FORREST, R.A.: AERE-R 12419 (1986). 3785 1451 266 3785 1451 267 1 451 313 03785 1451 268 2 151 458 03785 1451 269 3 1 25 03785 1451 270 3 2 25 03785 1451 271 3 4 15 03785 1451 272 3 16 9 03785 1451 273 3 17 4 03785 1451 274 3 22 11 03785 1451 275 3 28 11 03785 1451 276 3 32 6 03785 1451 277 3 51 15 03785 1451 278 3 52 14 03785 1451 279 3 53 13 03785 1451 280 3 54 12 03785 1451 281 3 55 12 03785 1451 282 3 56 11 03785 1451 283 3 57 11 03785 1451 284 3 58 10 03785 1451 285 3 91 9 03785 1451 286 3 102 19 03785 1451 287 3 103 15 03785 1451 288 3 104 12 03785 1451 289 3 105 10 03785 1451 290 3 106 9 03785 1451 291 3 107 15 03785 1451 292 4 2 160 03785 1451 293 4 16 10 03785 1451 294 4 17 10 03785 1451 295 4 22 10 03785 1451 296 4 28 10 03785 1451 297 4 32 10 03785 1451 298 4 51 25 03785 1451 299 4 52 25 03785 1451 300 4 53 24 03785 1451 301 4 54 24 03785 1451 302 4 55 24 03785 1451 303 4 56 24 03785 1451 304 4 57 24 03785 1451 305 4 58 22 03785 1451 306 4 91 22 03785 1451 307 5 16 47 03785 1451 308 5 17 13 03785 1451 309 5 22 136 03785 1451 310 5 28 107 03785 1451 311 5 32 35 03785 1451 312 5 91 126 03785 1451 313 0.000000+0 0.000000+0 0 0 0 03785 1 099999 0.000000+0 0.000000+0 0 0 0 03785 0 0 0 3.708500+4 8.418240+1 0 0 1 03785 2151 1 3.708500+4 1.000000+0 0 0 2 03785 2151 2 1.000000-5 8.468000+3 1 2 0 03785 2151 3 2.500000+0 7.200000-1 0 0 2 03785 2151 4 8.418240+1 0.000000+0 0 0 450 753785 2151 5 -1.545000+3 3.000000+0 3.416000+1 3.391000+1 2.500000-1 0.000000+03785 2151 6 2.350000+2 3.000000+0 2.733715-1 1.337143-2 2.600000-1 0.000000+03785 2151 7 4.740000+2 2.000000+0 3.176000-1 5.760000-2 2.600000-1 0.000000+03785 2151 8 5.267000+2 3.000000+0 1.639571+0 1.400571+0 2.390000-1 0.000000+03785 2151 9 6.549000+2 2.000000+0 6.084000-1 3.504000-1 2.580000-1 0.000000+03785 2151 10 1.007000+3 2.000000+0 4.196000-1 1.596000-1 2.600000-1 0.000000+03785 2151 11 1.042000+3 3.000000+0 9.778572-1 7.628571-1 2.150000-1 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