JENDL-5 (Neutron sublibrary (activation cs)) Cf-250 0 0 0 0 9.825000+4 2.479280+2 0 0 6 19855 1451 1 0.000000+0 1.000000+0 0 0 0 69855 1451 2 1.000000+0 2.000000+7 0 0 10 59855 1451 3 2.936000+2 0.000000+0 4 0 337 149855 1451 4 98-Cf-250 JAEA+ EVAL-FEB10 O.Iwamoto,T.Nakagawa,+ 9855 1451 5 DIST-DEC21 20100318 9855 1451 6 ----JENDL-5 MATERIAL 9855 9855 1451 7 -----INCIDENT NEUTRON DATA 9855 1451 8 ------ENDF-6 FORMAT 9855 1451 9 9855 1451 10 History 9855 1451 11 06-05 Resonance parameters were evaluated. 9855 1451 12 07-09 New theoretical calculation was done with CCONE code. 9855 1451 13 Data were compiled as JENDL/AC-2008/1/. 9855 1451 14 09-12 New theoretical calculation was done with CCONE code. 9855 1451 15 10-02 Data of prompt gamma rays due to fission were given. 9855 1451 16 10-03 Covariance data were added. 9855 1451 17 9855 1451 18 21-11 revised by O.Iwamoto 9855 1451 19 (MF3/MT19-21,38) deleted 9855 1451 20 (MF8/MT16-18,37,102) JENDL/AD-2017 adopted 9855 1451 21 (MF8/MT4) added 9855 1451 22 9855 1451 23 MF= 1 General information 9855 1451 24 MT=452 Number of Neutrons per fission 9855 1451 25 Sum of MT's = 455 and 456. 9855 1451 26 9855 1451 27 MT=455 Delayed neutron data 9855 1451 28 (same as JENDL-3.3) 9855 1451 29 Semi-empirical formula by Tuttle/2/. 9855 1451 30 9855 1451 31 MT=456 Number of prompt neutrons per fission 9855 1451 32 (same as JENDL-3.3) 9855 1451 33 Semi-empirical formula by Howerton/3/. 9855 1451 34 9855 1451 35 9855 1451 36 MF= 2 Resonance parameters 9855 1451 37 MT=151 9855 1451 38 Resolved resonance parameters (MLBW: 1.0e-5 - 10.0 eV) 9855 1451 39 Measured resonance parameters were reported by Anufriev and 9855 1451 40 Sivukha/4/ and Danon et al./5,6/ The present parameters were 9855 1451 41 determined from these results. A negative resonance was 9855 1451 42 assumed to reproduce thermal cross sections: 9855 1451 43 capture = 2019+-178 /7,8/ 9855 1451 44 fission = 112+-99 /5/ 9855 1451 45 9855 1451 46 Unresolved resonance parameters (10 eV - 100 keV) 9855 1451 47 Parameters (URP) were determined with ASREP code/9/ so as to 9855 1451 48 reproduce the cross sections in this energy region. URP are 9855 1451 49 used only for self-shielding calculations. 9855 1451 50 9855 1451 51 9855 1451 52 Thermal cross sections and resonance integrals (at 300K) 9855 1451 53 ------------------------------------------------------- 9855 1451 54 0.0253 eV reson. integ.(*) 9855 1451 55 (barns) (barns) 9855 1451 56 ------------------------------------------------------- 9855 1451 57 total 2131.9 9855 1451 58 elastic 2.25 9855 1451 59 fission 112.0 133 9855 1451 60 capture 2017.7 11900 9855 1451 61 ------------------------------------------------------- 9855 1451 62 (*) In the energy range from 0.5 eV to 10 MeV. 9855 1451 63 9855 1451 64 9855 1451 65 MF= 3 Neutron cross sections 9855 1451 66 Cross sections above the resolved resonance region were 9855 1451 67 calculated with CCONE code/10/. 9855 1451 68 9855 1451 69 MT= 1 Total cross section 9855 1451 70 The cross section was calculated with CC OMP of Soukhovitskii 9855 1451 71 et al./11/ 9855 1451 72 9855 1451 73 MT=18 Fission cross section 9855 1451 74 The experimental data of Danon et al./5/ were used to 9855 1451 75 determine the parameters in the CCONE calculation. 9855 1451 76 9855 1451 77 9855 1451 78 MF= 4 Angular distributions of secondary neutrons 9855 1451 79 MT=2 Elastic scattering 9855 1451 80 Calculated with CCONE code/10/. 9855 1451 81 9855 1451 82 MT=18 Fission 9855 1451 83 Isotropic distributions in the laboratory system were assumed.9855 1451 84 9855 1451 85 9855 1451 86 MF= 5 Energy distributions of secondary neutrons 9855 1451 87 MT=18 Prompt neutrons 9855 1451 88 Calculated with CCONE code/10/. 9855 1451 89 9855 1451 90 9855 1451 91 MF= 6 Energy-angle distributions 9855 1451 92 Calculated with CCONE code/10/. 9855 1451 93 Distributions from fission (MT=18) are not included. 9855 1451 94 9855 1451 95 9855 1451 96 MF=12 Photon production multiplicities 9855 1451 97 MT=18 Fission 9855 1451 98 Calculated from the total energy released by the prompt 9855 1451 99 gamma-rays due to fission which was estimated from its 9855 1451 100 systematics, and the average energy of gamma-rays. 9855 1451 101 9855 1451 102 9855 1451 103 MF=14 Photon angular distributions 9855 1451 104 MT=18 Fission 9855 1451 105 Isotoropic distributions were assumed. 9855 1451 106 9855 1451 107 9855 1451 108 MF=15 Continuous photon energy spectra 9855 1451 109 MT=18 Fission 9855 1451 110 Experimental data measured by Verbinski et al./12/ for 9855 1451 111 Pu-239 thermal fission were adopted. 9855 1451 112 9855 1451 113 9855 1451 114 MF=31 Covariances of average number of neutrons per fission 9855 1451 115 MT=452 Number of neutrons per fission 9855 1451 116 Sum of covariances for MT=455 and MT=456. 9855 1451 117 9855 1451 118 MT=455 9855 1451 119 Error of 15% was assumed. 9855 1451 120 9855 1451 121 MT=456 9855 1451 122 Covariance was obtained by fitting a linear function to the 9855 1451 123 data at 0.0 and 5.0 MeV with an uncertainty of 10%. 9855 1451 124 9855 1451 125 9855 1451 126 MF=32 Covariances of resonance parameters 9855 1451 127 MT=151 Resolved resonance parameterss 9855 1451 128 Format of LCOMP=0 was adopted. 9855 1451 129 9855 1451 130 Uncertainties of parameters were taken from Mughabghab /13/. 9855 1451 131 For the parameters without any information on uncertainty, 9855 1451 132 the following uncertainties were assumed: 9855 1451 133 Resonance energy 0.1 % 9855 1451 134 Neutron width 10 % 9855 1451 135 Capture width 10 % 9855 1451 136 Fission width 90 % 9855 1451 137 9855 1451 138 They were further modified by considering experimental data 9855 1451 139 of the fission and capture cross sections at the thermal 9855 1451 140 neutron energy. 9855 1451 141 9855 1451 142 9855 1451 143 MF=33 Covariances of neutron cross sections 9855 1451 144 Covariances were given to all the cross sections by using 9855 1451 145 KALMAN code/14/ and the covariances of model parameters 9855 1451 146 used in the cross-section calculations. 9855 1451 147 9855 1451 148 In the resolved resonance region, the following standard 9855 1451 149 deviations were added to the contributions from resonance 9855 1451 150 parameters: 9855 1451 151 Elastic scattering 20 % 9855 1451 152 9855 1451 153 9855 1451 154 MF=34 Covariances for Angular Distributions 9855 1451 155 MT=2 Elastic scattering 9855 1451 156 Covariances were given only to P1 components. 9855 1451 157 9855 1451 158 9855 1451 159 MF=35 Covariances for Energy Distributions 9855 1451 160 MT=18 Fission spectra 9855 1451 161 Estimated with CCONE and KALMAN codes. 9855 1451 162 9855 1451 163 9855 1451 164 ***************************************************************** 9855 1451 165 Calculation with CCONE code 9855 1451 166 ***************************************************************** 9855 1451 167 9855 1451 168 Models and parameters used in the CCONE/10/ calculation 9855 1451 169 1) Coupled channel optical model 9855 1451 170 Levels in the rotational band were included. Optical model 9855 1451 171 potential and coupled levels are shown in Table 1. 9855 1451 172 9855 1451 173 2) Two-component exciton model/15/ 9855 1451 174 * Global parametrization of Koning-Duijvestijn/16/ 9855 1451 175 was used. 9855 1451 176 * Gamma emission channel/17/ was added to simulate direct 9855 1451 177 and semi-direct capture reaction. 9855 1451 178 9855 1451 179 3) Hauser-Feshbach statistical model 9855 1451 180 * Moldauer width fluctuation correction/18/ was included. 9855 1451 181 * Neutron, gamma and fission decay channel were included. 9855 1451 182 * Transmission coefficients of neutrons were taken from 9855 1451 183 coupled channel calculation in Table 1. 9855 1451 184 * The level scheme of the target is shown in Table 2. 9855 1451 185 * Level density formula of constant temperature and Fermi-gas 9855 1451 186 model were used with shell energy correction and collective 9855 1451 187 enhancement factor. Parameters are shown in Table 3. 9855 1451 188 * Fission channel: 9855 1451 189 Double humped fission barriers were assumed. 9855 1451 190 Fission barrier penetrabilities were calculated with 9855 1451 191 Hill-Wheler formula/19/. Fission barrier parameters were 9855 1451 192 shown in Table 4. Transition state model was used and 9855 1451 193 continuum levels are assumed above the saddles. The level 9855 1451 194 density parameters for inner and outer saddles are shown in 9855 1451 195 Tables 5 and 6, respectively. 9855 1451 196 * Gamma-ray strength function of Kopecky et al/20/,/21/ 9855 1451 197 was used. The prameters are shown in Table 7. 9855 1451 198 9855 1451 199 9855 1451 200 ------------------------------------------------------------------9855 1451 201 Tables 9855 1451 202 ------------------------------------------------------------------9855 1451 203 9855 1451 204 Table 1. Coupled channel calculation 9855 1451 205 -------------------------------------------------- 9855 1451 206 * rigid rotor model was applied 9855 1451 207 * coupled levels = 0,1,2,3,4 (see Table 2) 9855 1451 208 * optical potential parameters /11/ 9855 1451 209 Volume: 9855 1451 210 V_0 = 49.97 MeV 9855 1451 211 lambda_HF = 0.01004 1/MeV 9855 1451 212 C_viso = 15.9 MeV 9855 1451 213 A_v = 12.04 MeV 9855 1451 214 B_v = 81.36 MeV 9855 1451 215 E_a = 385 MeV 9855 1451 216 r_v = 1.2568 fm 9855 1451 217 a_v = 0.633 fm 9855 1451 218 Surface: 9855 1451 219 W_0 = 17.2 MeV 9855 1451 220 B_s = 11.19 MeV 9855 1451 221 C_s = 0.01361 1/MeV 9855 1451 222 C_wiso = 23.5 MeV 9855 1451 223 r_s = 1.1803 fm 9855 1451 224 a_s = 0.601 fm 9855 1451 225 Spin-orbit: 9855 1451 226 V_so = 5.75 MeV 9855 1451 227 lambda_so = 0.005 1/MeV 9855 1451 228 W_so = -3.1 MeV 9855 1451 229 B_so = 160 MeV 9855 1451 230 r_so = 1.1214 fm 9855 1451 231 a_so = 0.59 fm 9855 1451 232 Coulomb: 9855 1451 233 C_coul = 1.3 9855 1451 234 r_c = 1.2452 fm 9855 1451 235 a_c = 0.545 fm 9855 1451 236 Deformation: 9855 1451 237 beta_2 = 0.213 9855 1451 238 beta_4 = 0.066 9855 1451 239 beta_6 = 0.0015 9855 1451 240 9855 1451 241 * Calculated strength function 9855 1451 242 S0= 1.34e-4 S1= 3.08e-4 R'= 9.14 fm (En=1 keV) 9855 1451 243 -------------------------------------------------- 9855 1451 244 9855 1451 245 Table 2. Level Scheme of Cf-250 9855 1451 246 ------------------- 9855 1451 247 No. Ex(MeV) J PI 9855 1451 248 ------------------- 9855 1451 249 0 0.00000 0 + * 9855 1451 250 1 0.04272 2 + * 9855 1451 251 2 0.14189 4 + * 9855 1451 252 3 0.29623 6 + * 9855 1451 253 4 0.50000 8 + * 9855 1451 254 ------------------- 9855 1451 255 *) Coupled levels in CC calculation 9855 1451 256 9855 1451 257 Table 3. Level density parameters 9855 1451 258 -------------------------------------------------------- 9855 1451 259 Nuclide a* Pair Eshell T E0 Ematch 9855 1451 260 1/MeV MeV MeV MeV MeV MeV 9855 1451 261 -------------------------------------------------------- 9855 1451 262 Cf-251 19.2285 0.7574 1.2773 0.3926 -0.9361 3.0632 9855 1451 263 Cf-250 19.1626 1.5179 1.0208 0.3974 -0.1838 3.8400 9855 1451 264 Cf-249 19.0966 0.7605 0.7689 0.3773 -0.6847 2.7641 9855 1451 265 Cf-248 19.0305 1.5240 0.7495 0.3921 -0.0631 3.7096 9855 1451 266 Cf-247 18.9645 0.7635 0.5924 0.3748 -0.6176 2.6898 9855 1451 267 -------------------------------------------------------- 9855 1451 268 9855 1451 269 Table 4. Fission barrier parameters 9855 1451 270 ---------------------------------------- 9855 1451 271 Nuclide V_A hw_A V_B hw_B 9855 1451 272 MeV MeV MeV MeV 9855 1451 273 ---------------------------------------- 9855 1451 274 Cf-251 6.200 0.800 5.000 0.600 9855 1451 275 Cf-250 6.200 1.040 5.400 0.600 9855 1451 276 Cf-249 6.700 1.200 5.900 0.800 9855 1451 277 Cf-248 6.200 1.040 5.400 0.600 9855 1451 278 Cf-247 6.700 1.000 5.900 0.800 9855 1451 279 ---------------------------------------- 9855 1451 280 9855 1451 281 Table 5. Level density above inner saddle 9855 1451 282 -------------------------------------------------------- 9855 1451 283 Nuclide a* Pair Eshell T E0 Ematch 9855 1451 284 1/MeV MeV MeV MeV MeV MeV 9855 1451 285 -------------------------------------------------------- 9855 1451 286 Cf-251 21.5360 0.8837 2.5000 0.3208 -1.5294 2.8837 9855 1451 287 Cf-250 21.4621 1.7709 2.5000 0.2827 -0.1068 3.2709 9855 1451 288 Cf-249 20.0514 0.8872 2.5000 0.3486 -1.7837 3.0872 9855 1451 289 Cf-248 21.3142 1.7780 2.5000 0.3226 -0.6352 3.7780 9855 1451 290 Cf-247 21.2402 0.8908 2.5000 0.3232 -1.5224 2.8908 9855 1451 291 -------------------------------------------------------- 9855 1451 292 9855 1451 293 Table 6. Level density above outer saddle 9855 1451 294 -------------------------------------------------------- 9855 1451 295 Nuclide a* Pair Eshell T E0 Ematch 9855 1451 296 1/MeV MeV MeV MeV MeV MeV 9855 1451 297 -------------------------------------------------------- 9855 1451 298 Cf-251 21.5360 0.8837 1.0000 0.3488 -0.8268 2.8837 9855 1451 299 Cf-250 21.4621 1.7709 0.9600 0.3499 0.0610 3.7709 9855 1451 300 Cf-249 20.0514 0.8872 0.9200 0.3794 -1.0059 3.0872 9855 1451 301 Cf-248 21.3142 1.7780 0.8800 0.3522 0.0693 3.7780 9855 1451 302 Cf-247 21.2402 0.8908 0.8400 0.3533 -0.8173 2.8908 9855 1451 303 -------------------------------------------------------- 9855 1451 304 9855 1451 305 Table 7. Gamma-ray strength function for Cf-251 9855 1451 306 -------------------------------------------------------- 9855 1451 307 K0 = 1.700 E0 = 4.500 (MeV) 9855 1451 308 * E1: ER = 11.36 (MeV) EG = 2.69 (MeV) SIG = 256.28 (mb) 9855 1451 309 ER = 14.26 (MeV) EG = 4.16 (MeV) SIG = 512.55 (mb) 9855 1451 310 * M1: ER = 6.50 (MeV) EG = 4.00 (MeV) SIG = 2.02 (mb) 9855 1451 311 * E2: ER = 9.99 (MeV) EG = 3.10 (MeV) SIG = 7.35 (mb) 9855 1451 312 -------------------------------------------------------- 9855 1451 313 9855 1451 314 9855 1451 315 References 9855 1451 316 1) O.Iwamoto et al.: J. Nucl. Sci. Technol., 46, 510 (2009). 9855 1451 317 2) R.J.Tuttle: INDC(NDS)-107/G+Special, p.29 (1979). 9855 1451 318 3) R.J.Howerton: Nucl. Sci. Eng., 62, 438 (1977). 9855 1451 319 4) V.A.Anufriev, V.I.Sivukha: Sov. At. Energy, 74, 69 (1993). 9855 1451 320 5) Y.Danon et al.: Nucl. Sci. Eng., 109, 341 (1991). 9855 1451 321 6) Y.Danon et al.: 1994 Gatlinburg, Vol. 1, p.245 (1994). 9855 1451 322 7) J.Halperin et al.: ORNL-4706, p.47 (1971). 9855 1451 323 8) V.D.Gavrilov, V.A.Goncharov: Sov. At. Energy, 22, 274 9855 1451 324 (1978). 9855 1451 325 9) Y.Kikuchi et al.: JAERI-Data/Code 99-025 (1999) in Japanese. 9855 1451 326 10) O.Iwamoto: J. Nucl. Sci. Technol., 44, 687 (2007). 9855 1451 327 11) E.Sh.Soukhovitskii et al.: Phys. Rev. C72, 024604 (2005). 9855 1451 328 12) V.V.Verbinski et al.: Phys. Rev., C7, 1173 (1973). 9855 1451 329 13) S.F.Mughabghab: "Atlas of Neutron Resonances," Elsevier 9855 1451 330 (2006). 9855 1451 331 14) T.Kawano, K.Shibata, JAERI-Data/Code 97-037 (1997) in 9855 1451 332 Japanese. 9855 1451 333 15) C.Kalbach: Phys. Rev. C33, 818 (1986). 9855 1451 334 16) A.J.Koning, M.C.Duijvestijn: Nucl. Phys. A744, 15 (2004). 9855 1451 335 17) J.M.Akkermans, H.Gruppelaar: Phys. Lett. 157B, 95 (1985). 9855 1451 336 18) P.A.Moldauer: Nucl. Phys. A344, 185 (1980). 9855 1451 337 19) D.L.Hill, J.A.Wheeler: Phys. Rev. 89, 1102 (1953). 9855 1451 338 20) J.Kopecky, M.Uhl: Phys. Rev. C41, 1941 (1990). 9855 1451 339 21) J.Kopecky, M.Uhl, R.E.Chrien: Phys. Rev. C47, 312 (1990). 9855 1451 340 9855 1451 341 1 451 355 19855 1451 342 2 151 4 19855 1451 343 3 4 27 19855 1451 344 3 16 13 19855 1451 345 3 17 9 19855 1451 346 3 18 364 19855 1451 347 3 37 4 19855 1451 348 3 102 377 19855 1451 349 8 4 2 19855 1451 350 8 16 2 19855 1451 351 8 17 2 19855 1451 352 8 18 2 19855 1451 353 8 37 2 19855 1451 354 8 102 2 19855 1451 355 9855 1 099999 9855 0 0 0 9.825000+4 2.479280+2 0 0 1 09855 2151 1 9.825000+4 1.000000+0 0 0 1 09855 2151 2 1.000000-5 1.000000+1 0 0 0 09855 2151 3 0.000000+0 9.250000-1 0 0 0 09855 2151 4 9855 2 099999 9855 0 0 0 9.825000+4 2.479280+2 0 0 0 09855 3 4 1 0.000000+0-4.272200+4 0 0 1 709855 3 4 2 70 2 9855 3 4 3 4.289430+4 0.000000+0 5.000000+4 1.353580-1 7.000000+4 4.515330-19855 3 4 4 1.000000+5 7.537570-1 1.100000+5 8.189570-1 1.200000+5 8.841665-19855 3 4 5 1.400000+5 9.960066-1 1.424570+5 1.009231+0 1.700000+5 1.137861+09855 3 4 6 2.000000+5 1.276672+0 2.500000+5 1.419131+0 2.974250+5 1.540761+09855 3 4 7 3.000000+5 1.547727+0 4.000000+5 1.655657+0 5.000000+5 1.797166+09855 3 4 8 5.020170+5 1.798272+0 6.000000+5 1.851941+0 7.000000+5 1.940282+09855 3 4 9 8.000000+5 2.023944+0 9.000000+5 2.087767+0 1.000000+6 2.118288+09855 3 4 10 1.100000+6 2.107575+0 1.200000+6 2.078168+0 1.300000+6 2.044084+09855 3 4 11 1.400000+6 2.019377+0 1.500000+6 1.992520+0 1.600000+6 1.972086+09855 3 4 12 1.700000+6 1.944694+0 1.800000+6 1.919399+0 1.900000+6 1.886090+09855 3 4 13 2.000000+6 1.853302+0 2.100000+6 1.813983+0 2.300000+6 1.735991+09855 3 4 14 2.500000+6 1.653458+0 2.700000+6 1.573515+0 3.000000+6 1.461443+09855 3 4 15 3.500000+6 1.321383+0 4.000000+6 1.226011+0 4.500000+6 1.191559+09855 3 4 16 5.000000+6 1.183380+0 5.500000+6 1.190614+0 6.000000+6 1.172657+09855 3 4 17 6.500000+6 1.093764+0 7.000000+6 9.847172-1 7.500000+6 8.639023-19855 3 4 18 8.000000+6 7.710047-1 8.500000+6 6.966995-1 9.000000+6 6.426381-19855 3 4 19 9.500000+6 5.997236-1 1.000000+7 5.660581-1 1.050000+7 5.379814-19855 3 4 20 1.100000+7 5.136867-1 1.150000+7 4.921934-1 1.200000+7 4.719861-19855 3 4 21 1.250000+7 4.538703-1 1.300000+7 4.363522-1 1.350000+7 4.202865-19855 3 4 22 1.400000+7 4.045933-1 1.450000+7 3.902788-1 1.500000+7 3.758902-19855 3 4 23 1.550000+7 3.634591-1 1.600000+7 3.507812-1 1.650000+7 3.395343-19855 3 4 24 1.700000+7 3.286851-1 1.750000+7 3.189399-1 1.800000+7 3.090775-19855 3 4 25 1.850000+7 3.004024-1 1.900000+7 2.918726-1 1.950000+7 2.841571-19855 3 4 26 2.000000+7 2.767848-1 9855 3 4 27 9855 3 099999 9.825000+4 2.479280+2 0 0 0 09855 3 16 1 -6.625150+6-6.625150+6 0 0 1 289855 3 16 2 28 2 9855 3 16 3 6.651870+6 0.000000+0 7.000000+6 1.420250-2 7.500000+6 9.865370-29855 3 16 4 8.000000+6 2.017500-1 8.500000+6 2.768480-1 9.000000+6 3.198330-19855 3 16 5 9.500000+6 3.372840-1 1.000000+7 3.439620-1 1.050000+7 3.439400-19855 3 16 6 1.100000+7 3.468830-1 1.150000+7 3.520560-1 1.200000+7 3.593480-19855 3 16 7 1.250000+7 3.639840-1 1.300000+7 3.650310-1 1.350000+7 3.571020-19855 3 16 8 1.400000+7 3.392640-1 1.450000+7 3.157990-1 1.500000+7 2.911010-19855 3 16 9 1.550000+7 2.647460-1 1.600000+7 2.433420-1 1.650000+7 2.238020-19855 3 16 10 1.700000+7 2.067820-1 1.750000+7 1.930200-1 1.800000+7 1.849200-19855 3 16 11 1.850000+7 1.755450-1 1.900000+7 1.676280-1 1.950000+7 1.613720-19855 3 16 12 2.000000+7 1.526100-1 9855 3 16 13 9855 3 099999 9.825000+4 2.479280+2 0 0 0 09855 3 17 1 -1.221060+7-1.221060+7 0 0 1 169855 3 17 2 16 2 9855 3 17 3 1.225990+7 0.000000+0 1.300000+7 1.649340-3 1.350000+7 8.906070-39855 3 17 4 1.400000+7 2.151670-2 1.450000+7 3.539470-2 1.500000+7 4.875180-29855 3 17 5 1.550000+7 6.095330-2 1.600000+7 7.433590-2 1.650000+7 8.145670-29855 3 17 6 1.700000+7 9.147370-2 1.750000+7 9.737010-2 1.800000+7 1.022070-19855 3 17 7 1.850000+7 1.071760-1 1.900000+7 1.116490-1 1.950000+7 1.126100-19855 3 17 8 2.000000+7 1.148080-1 9855 3 17 9 9855 3 099999 9.825000+4 2.479280+2 0 0 0 09855 3 18 1 2.144000+8 2.144000+8 0 0 1 10829855 3 18 2 1082 2 9855 3 18 3 1.000000-5 9.095563+3 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