JENDL-5 (Neutron sublibrary (activation cs)) Np-236 0 0 0 0 9.323600+4 2.340190+2 0 0 6 19343 1451 1 0.000000+0 1.000000+0 0 0 0 69343 1451 2 1.000000+0 2.000000+7 0 0 10 59343 1451 3 2.936000+2 0.000000+0 4 0 350 149343 1451 4 93-Np-236 JAEA+ EVAL-FEB10 O.Iwamoto,T.Nakagawa,K.Furutaka,+9343 1451 5 DIST-DEC21 20100318 9343 1451 6 ----JENDL-5 MATERIAL 9343 9343 1451 7 -----INCIDENT NEUTRON DATA 9343 1451 8 ------ENDF-6 FORMAT 9343 1451 9 9343 1451 10 History 9343 1451 11 07-07 New theoretical calculation was made with CCONE code. 9343 1451 12 07-09 Resolved resonance parameters were replaced. 9343 1451 13 07-10 Theoretical calculation was made with CCONE code. 9343 1451 14 Data were compiled as JENDL/AC-2008/1/. 9343 1451 15 09-02 (3,102) below 0.2 eV, (1,452), (1,455) and (1,456) were 9343 1451 16 revised. 9343 1451 17 10-02 Data of prompt gamma rays due to fission were given. 9343 1451 18 10-03 Covariance data were given. 9343 1451 19 9343 1451 20 21-11 revised by O.Iwamoto 9343 1451 21 (MF3/MT19-21,38) deleted 9343 1451 22 (MF8/MT16-18,37,102) JENDL/AD-2017 adopted 9343 1451 23 (MF8/MT4) added 9343 1451 24 9343 1451 25 MF= 1 General information 9343 1451 26 MT=452 Number of Neutrons per fission 9343 1451 27 Sum of MT's=455 and 456. 9343 1451 28 9343 1451 29 MT=455 Delayed neutron data 9343 1451 30 Determined from systematics by Tuttle/2/, Benedetti et al./3/ 9343 1451 31 and Waldo et al./4/, and partial fission cross sections 9343 1451 32 calculated with CCONE code /5/. 9343 1451 33 9343 1451 34 MT=456 Number of prompt neutrons per fission 9343 1451 35 Based on the data measured by Lindner and Seegmiller/6/ and 9343 1451 36 Ohsawa's systematics/7/. 9343 1451 37 9343 1451 38 9343 1451 39 MF= 2 Resonance parameters 9343 1451 40 MT=151 9343 1451 41 Resolved resonance parameters (MLBW: 1.0e-5 - 21.5 eV) 9343 1451 42 Evaluated by Furutaka /8/ with SAMMY-7 code/9/. 9343 1451 43 Experimental data used are fission cross-section data measured9343 1451 44 by Danon et al./10/ Their data were normalized to 2815 b at 9343 1451 45 0.0253 eV. The capture width was fixed to 40 meV. 9343 1451 46 Doppler as well as resolution broadenings were taken into 9343 1451 47 account in the analysis: temperature was assumed to be 298 K. 9343 1451 48 For resolution broadening, parameters of SAMMY's original 9343 1451 49 resolution-broadening function were chosen to approximately 9343 1451 50 reproduce the experimental resolution function described by 9343 1451 51 equation (11) of ref./10/. 9343 1451 52 9343 1451 53 The 8 fictitious resonances in the energy range 24 to 33 eV 9343 1451 54 were adopted from ENDF/B-VII.0/11/ 9343 1451 55 9343 1451 56 Un-resolved resonance parameters (21.5 eV - 10 keV) 9343 1451 57 Parameters (URP) were determined with ASREP code/12/ so as to 9343 1451 58 reproduce the cross sections in this energy region. URP are 9343 1451 59 used only for self-shielding calculations. 9343 1451 60 9343 1451 61 9343 1451 62 Thermal cross sections and resonance integrals (at 300K) 9343 1451 63 ------------------------------------------------------- 9343 1451 64 0.0253 eV reson. integ.(*) 9343 1451 65 (barns) (barns) 9343 1451 66 ------------------------------------------------------- 9343 1451 67 total 2938.9 9343 1451 68 elastic 9.657 9343 1451 69 fission 2808.0 1170 9343 1451 70 capture 121.3 100 9343 1451 71 ------------------------------------------------------- 9343 1451 72 (*) In the energy range from 0.5 eV to 10 MeV. 9343 1451 73 9343 1451 74 9343 1451 75 MF= 3 Neutron cross sections 9343 1451 76 All the cross-section data above 21.5 eV were calculated with 9343 1451 77 CCONE code/5/. 9343 1451 78 9343 1451 79 MT= 1 Total cross section 9343 1451 80 The cross section was calculated with CC OMP of Soukhovitskii 9343 1451 81 et al./13/. 9343 1451 82 9343 1451 83 MT=18 Fission cross section 9343 1451 84 Calculated with CCONE code. The simulated (n,f) cross section 9343 1451 85 of Britt and Wilhelmy/14/ and the experimental data of 9343 1451 86 Danon et al./10/ and Val'skiy et al./15/ were used to 9343 1451 87 determine the parameters in the CCONE calculation. 9343 1451 88 9343 1451 89 9343 1451 90 MF= 4 Angular distributions of secondary neutrons 9343 1451 91 MT=2 Elastic scattering 9343 1451 92 Calculated with CCONE code. 9343 1451 93 9343 1451 94 MT=18 Fission 9343 1451 95 Isotropic distributions in the laboratory system were assumed.9343 1451 96 9343 1451 97 9343 1451 98 MF= 5 Energy distributions of secondary neutrons 9343 1451 99 MT=18 Prompt neutrons 9343 1451 100 Calculated with CCONE code/5/. 9343 1451 101 9343 1451 102 9343 1451 103 MF= 6 Energy-angle distributions 9343 1451 104 Calculated with CCONE code. 9343 1451 105 Distributions from fission (MT=18) are not included. 9343 1451 106 9343 1451 107 9343 1451 108 MF=12 Photon production multiplicities 9343 1451 109 MT=18 Fission 9343 1451 110 Calculated from the total energy released by the prompt 9343 1451 111 gamma-rays due to fission which was estimated from its 9343 1451 112 systematics, and the average energy of gamma-rays. 9343 1451 113 9343 1451 114 9343 1451 115 MF=14 Photon angular distributions 9343 1451 116 MT=18 Fission 9343 1451 117 Isotoropic distributions were assumed. 9343 1451 118 9343 1451 119 9343 1451 120 MF=15 Continuous photon energy spectra 9343 1451 121 MT=18 Fission 9343 1451 122 Experimental data measured by Verbinski et al./16/ for 9343 1451 123 Pu-239 thermal fission were adopted. 9343 1451 124 9343 1451 125 9343 1451 126 MF=31 Covariances of average number of neutrons per fission 9343 1451 127 MT=452 Number of neutrons per fission 9343 1451 128 Sum of covariances for MT=455 and MT=456. 9343 1451 129 9343 1451 130 MT=455 9343 1451 131 Error of 15% was assumed. 9343 1451 132 9343 1451 133 MT=456 9343 1451 134 Covariance was obtained by fitting a linear function to the 9343 1451 135 data at 0.0 and 5.0 MeV with an uncertainty of 30% which was 9343 1451 136 estimated from the experimental data of Lindner and 9343 1451 137 Seegmiller/6/. 9343 1451 138 9343 1451 139 9343 1451 140 MF=32 Covariances of resonance parameters 9343 1451 141 MT=151 Resolved resonance parameterss 9343 1451 142 Format of LCOMP=1 was adopted. 9343 1451 143 9343 1451 144 Covariances of parameters were taken from the results of SAMMY9343 1451 145 analysis/8/. The covariances were multiplied by a factor 9343 1451 146 of 10 because they were too small. 9343 1451 147 9343 1451 148 9343 1451 149 MF=33 Covariances of neutron cross sections 9343 1451 150 Covariances were given to all the cross sections by using 9343 1451 151 KALMAN code/17/ and the covariances of model parameters 9343 1451 152 used in the cross-section calculations. 9343 1451 153 9343 1451 154 Covariances of the fission cross section were determined by 9343 1451 155 considering the experimental data (see MF=3). 9343 1451 156 9343 1451 157 In the resolved resonance region, the following standard 9343 1451 158 deviations were added to the contributions from resonance 9343 1451 159 parameters: 9343 1451 160 Elastic scattering 20 % 9343 1451 161 Capture 50 % 9343 1451 162 9343 1451 163 9343 1451 164 MF=34 Covariances for Angular Distributions 9343 1451 165 MT=2 Elastic scattering 9343 1451 166 Covariances were given only to P1 components. 9343 1451 167 9343 1451 168 9343 1451 169 MF=35 Covariances for Energy Distributions 9343 1451 170 MT=18 Fission spectra 9343 1451 171 Estimated with CCONE and KALMAN codes. 9343 1451 172 9343 1451 173 9343 1451 174 ***************************************************************** 9343 1451 175 Calculation with CCONE code 9343 1451 176 ***************************************************************** 9343 1451 177 9343 1451 178 Models and parameters used in the CCONE/5/ calculation 9343 1451 179 1) Coupled channel optical model 9343 1451 180 Levels in the rotational band were included. Optical model 9343 1451 181 potential and coupled levels are shown in Table 1. 9343 1451 182 9343 1451 183 2) Two-component exciton model/18/ 9343 1451 184 * Global parametrization of Koning-Duijvestijn/19/ 9343 1451 185 was used. 9343 1451 186 * Gamma emission channel/20/ was added to simulate direct 9343 1451 187 and semi-direct capture reaction. 9343 1451 188 9343 1451 189 3) Hauser-Feshbach statistical model 9343 1451 190 * Moldauer width fluctuation correction/21/ was included. 9343 1451 191 * Neutron, gamma and fission decay channel were included. 9343 1451 192 * Transmission coefficients of neutrons were taken from 9343 1451 193 coupled channel calculation in Table 1. 9343 1451 194 * The level scheme of the target is shown in Table 2. 9343 1451 195 * Level density formula of constant temperature and Fermi-gas 9343 1451 196 model were used with shell energy correction and collective 9343 1451 197 enhancement factor. Parameters are shown in Table 3. 9343 1451 198 * Fission channel: 9343 1451 199 Double humped fission barriers were assumed. 9343 1451 200 Fission barrier penetrabilities were calculated with 9343 1451 201 Hill-Wheler formula/22/. Fission barrier parameters were 9343 1451 202 shown in Table 4. Transition state model was used and 9343 1451 203 continuum levels are assumed above the saddles. The level 9343 1451 204 density parameters for inner and outer saddles are shown in 9343 1451 205 Tables 5 and 6, respectively. 9343 1451 206 * Gamma-ray strength function of Kopecky et al/23/,/24/ 9343 1451 207 was used. The prameters are shown in Table 7. 9343 1451 208 9343 1451 209 9343 1451 210 ------------------------------------------------------------------9343 1451 211 Tables 9343 1451 212 ------------------------------------------------------------------9343 1451 213 9343 1451 214 Table 1. Coupled channel calculation 9343 1451 215 -------------------------------------------------- 9343 1451 216 * rigid rotor model was applied 9343 1451 217 * coupled levels = 0,1,5 (see Table 2) 9343 1451 218 * optical potential parameters /13/ 9343 1451 219 Volume: 9343 1451 220 V_0 = 49.97 MeV 9343 1451 221 lambda_HF = 0.01004 1/MeV 9343 1451 222 C_viso = 15.9 MeV 9343 1451 223 A_v = 12.04 MeV 9343 1451 224 B_v = 81.36 MeV 9343 1451 225 E_a = 385 MeV 9343 1451 226 r_v = 1.2568 fm 9343 1451 227 a_v = 0.633 fm 9343 1451 228 Surface: 9343 1451 229 W_0 = 17.2 MeV 9343 1451 230 B_s = 11.19 MeV 9343 1451 231 C_s = 0.01361 1/MeV 9343 1451 232 C_wiso = 23.5 MeV 9343 1451 233 r_s = 1.1803 fm 9343 1451 234 a_s = 0.601 fm 9343 1451 235 Spin-orbit: 9343 1451 236 V_so = 5.75 MeV 9343 1451 237 lambda_so = 0.005 1/MeV 9343 1451 238 W_so = -3.1 MeV 9343 1451 239 B_so = 160 MeV 9343 1451 240 r_so = 1.1214 fm 9343 1451 241 a_so = 0.59 fm 9343 1451 242 Coulomb: 9343 1451 243 C_coul = 1.3 9343 1451 244 r_c = 1.2452 fm 9343 1451 245 a_c = 0.545 fm 9343 1451 246 Deformation: 9343 1451 247 beta_2 = 0.213 9343 1451 248 beta_4 = 0.066 9343 1451 249 beta_6 = 0.0015 9343 1451 250 9343 1451 251 * Calculated strength function 9343 1451 252 S0= 0.90e-4 S1= 2.70e-4 R'= 9.46 fm (En=1 keV) 9343 1451 253 -------------------------------------------------- 9343 1451 254 9343 1451 255 Table 2. Level Scheme of Np-236 9343 1451 256 ------------------- 9343 1451 257 No. Ex(MeV) J PI 9343 1451 258 ------------------- 9343 1451 259 0 0.00000 6 - * 9343 1451 260 1 0.05600 7 - * 9343 1451 261 2 0.06000 1 + 9343 1451 262 3 0.07600 2 + 9343 1451 263 4 0.10000 3 + 9343 1451 264 5 0.12000 8 - * 9343 1451 265 6 0.13200 4 + 9343 1451 266 ------------------- 9343 1451 267 *) Coupled levels in CC calculation 9343 1451 268 9343 1451 269 Table 3. Level density parameters 9343 1451 270 -------------------------------------------------------- 9343 1451 271 Nuclide a* Pair Eshell T E0 Ematch 9343 1451 272 1/MeV MeV MeV MeV MeV MeV 9343 1451 273 -------------------------------------------------------- 9343 1451 274 Np-237 18.3022 0.7795 2.4371 0.3963 -0.9739 3.1569 9343 1451 275 Np-236 18.2358 0.0000 2.1332 0.2999 -0.7994 1.1664 9343 1451 276 Np-235 18.1694 0.7828 2.2924 0.3973 -0.9417 3.1303 9343 1451 277 Np-234 18.1029 0.0000 2.1332 0.2844 -0.6773 1.0000 9343 1451 278 Np-233 18.0364 0.7861 2.3620 0.4163 -1.1454 3.3864 9343 1451 279 -------------------------------------------------------- 9343 1451 280 9343 1451 281 Table 4. Fission barrier parameters 9343 1451 282 ---------------------------------------- 9343 1451 283 Nuclide V_A hw_A V_B hw_B 9343 1451 284 MeV MeV MeV MeV 9343 1451 285 ---------------------------------------- 9343 1451 286 Np-237 6.000 0.950 5.570 0.600 9343 1451 287 Np-236 6.100 0.600 6.080 0.600 9343 1451 288 Np-235 6.250 0.950 5.630 0.600 9343 1451 289 Np-234 6.200 0.460 5.850 0.370 9343 1451 290 Np-233 4.300 0.800 3.300 0.520 9343 1451 291 ---------------------------------------- 9343 1451 292 9343 1451 293 Table 5. Level density above inner saddle 9343 1451 294 -------------------------------------------------------- 9343 1451 295 Nuclide a* Pair Eshell T E0 Ematch 9343 1451 296 1/MeV MeV MeV MeV MeV MeV 9343 1451 297 -------------------------------------------------------- 9343 1451 298 Np-237 21.9626 0.9094 2.6000 0.3162 -1.4591 2.9094 9343 1451 299 Np-236 22.2477 0.0000 2.6000 0.3139 -2.3586 2.0000 9343 1451 300 Np-235 20.3497 0.9133 2.6000 0.3299 -1.4981 2.9133 9343 1451 301 Np-234 20.2753 0.0000 2.6000 0.3306 -2.4114 2.0000 9343 1451 302 Np-233 20.2008 0.9172 2.6000 0.3312 -1.4942 2.9172 9343 1451 303 -------------------------------------------------------- 9343 1451 304 9343 1451 305 Table 6. Level density above outer saddle 9343 1451 306 -------------------------------------------------------- 9343 1451 307 Nuclide a* Pair Eshell T E0 Ematch 9343 1451 308 1/MeV MeV MeV MeV MeV MeV 9343 1451 309 -------------------------------------------------------- 9343 1451 310 Np-237 22.3287 0.9094 0.2400 0.3268 -0.5253 2.6094 9343 1451 311 Np-236 22.2477 0.0000 0.2000 0.3977 -2.2734 2.7000 9343 1451 312 Np-235 22.1666 0.9133 0.1600 0.3517 -0.7691 2.9133 9343 1451 313 Np-234 20.2753 0.0000 0.1200 0.3712 -1.6997 2.0000 9343 1451 314 Np-233 20.2008 0.9172 0.0800 0.3724 -0.7819 2.9172 9343 1451 315 -------------------------------------------------------- 9343 1451 316 9343 1451 317 Table 7. Gamma-ray strength function for Np-237 9343 1451 318 -------------------------------------------------------- 9343 1451 319 K0 = 1.300 E0 = 4.500 (MeV) 9343 1451 320 * E1: ER = 10.98 (MeV) EG = 2.17 (MeV) SIG = 311.00 (mb) 9343 1451 321 ER = 14.08 (MeV) EG = 4.66 (MeV) SIG = 540.00 (mb) 9343 1451 322 * M1: ER = 6.63 (MeV) EG = 4.00 (MeV) SIG = 2.08 (mb) 9343 1451 323 * E2: ER = 10.18 (MeV) EG = 3.27 (MeV) SIG = 6.65 (mb) 9343 1451 324 -------------------------------------------------------- 9343 1451 325 9343 1451 326 9343 1451 327 References 9343 1451 328 1) O.Iwamoto et al.: J. Nucl. Sci. Technol., 46, 510 (2009). 9343 1451 329 2) R.J.Tuttle: INDC(NDS)-107/G+Special, p.29 (1979). 9343 1451 330 3) G.Benedetti et al.: Nucl. Sci. Eng., 80, 379 (1982). 9343 1451 331 4) R.Waldo et al.: Phys. Rev., C23, 1113 (1981). 9343 1451 332 5) O.Iwamoto: J. Nucl. Sci. Technol., 44, 687 (2007). 9343 1451 333 6) M.Lindner, D.W.Seegmiller: Radiochimica Acta, 49, 1(1990). 9343 1451 334 7) T.Ohsawa: J.Nucl. Radiochem. Sci., 9, 19 (2008). 9343 1451 335 8) K.Furutaka: Private communication (2007). 9343 1451 336 9) N.M.Larson: PSR-158 (2006), ORNL/TM-9179/R7 (2006) 9343 1451 337 10) Y.Danon et al.: Nucl. Sci. Eng., 124, 482 (1996). 9343 1451 338 11) M.B.Chadwick et al.: Nucl. Data Sheets, 102, 2931 (2006). 9343 1451 339 12) Y.Kikuchi et al.: JAERI-Data/Code 99-025 (1999) in Japanese. 9343 1451 340 13) E.Sh.Soukhovitskii et al.: Phys. Rev. C72, 024604 (2005). 9343 1451 341 14) H.C.Britt, J.B.Wilhelmy: Nucl. Sci. Eng., 72, 222 (1979). 9343 1451 342 15) G.V.Val'skiy et al.: 1987 Kiev, Vol.3, p.99 (1987). 9343 1451 343 16) V.V.Verbinski et al.: Phys. Rev., C7, 1173 (1973). 9343 1451 344 17) T.Kawano, K.Shibata, JAERI-Data/Code 97-037 (1997) in 9343 1451 345 Japanese. 9343 1451 346 18) C.Kalbach: Phys. Rev. C33, 818 (1986). 9343 1451 347 19) A.J.Koning, M.C.Duijvestijn: Nucl. Phys. A744, 15 (2004). 9343 1451 348 20) J.M.Akkermans, H.Gruppelaar: Phys. Lett. 157B, 95 (1985). 9343 1451 349 21) P.A.Moldauer: Nucl. Phys. A344, 185 (1980). 9343 1451 350 22) D.L.Hill, J.A.Wheeler: Phys. Rev. 89, 1102 (1953). 9343 1451 351 23) J.Kopecky, M.Uhl: Phys. Rev. C41, 1941 (1990). 9343 1451 352 24) J.Kopecky, M.Uhl, R.E.Chrien: Phys. Rev. C47, 312 (1990). 9343 1451 353 9343 1451 354 1 451 368 19343 1451 355 2 151 4 19343 1451 356 3 4 27 19343 1451 357 3 16 13 19343 1451 358 3 17 8 19343 1451 359 3 18 313 19343 1451 360 3 37 4 19343 1451 361 3 102 407 19343 1451 362 8 4 2 19343 1451 363 8 16 2 19343 1451 364 8 17 2 19343 1451 365 8 18 2 19343 1451 366 8 37 2 19343 1451 367 8 102 2 19343 1451 368 9343 1 099999 9343 0 0 0 9.323600+4 2.340190+2 0 0 1 09343 2151 1 9.323600+4 1.000000+0 0 0 1 09343 2151 2 1.000000-5 2.150000+1 0 0 0 09343 2151 3 6.000000+0 9.500000-1 0 0 0 09343 2151 4 9343 2 099999 9343 0 0 0 9.323600+4 2.340190+2 0 0 0 09343 3 4 1 0.000000+0-5.600000+4 0 0 1 709343 3 4 2 70 2 9343 3 4 3 5.623930+4 0.000000+0 6.025640+4 4.038780-3 7.000000+4 1.014480-29343 3 4 4 7.632480+4 1.422380-2 1.000000+5 2.975203-2 1.004270+5 3.004167-29343 3 4 5 1.111580+5 3.718397-2 1.200000+5 4.306924-2 1.205130+5 4.340747-29343 3 4 6 1.325640+5 5.266170-2 1.400000+5 5.998954-2 1.700000+5 8.838006-29343 3 4 7 2.000000+5 1.157304-1 2.500000+5 1.933570-1 3.000000+5 2.210031-19343 3 4 8 4.000000+5 3.476750-1 5.000000+5 4.995879-1 6.000000+5 6.231149-19343 3 4 9 7.000000+5 7.472744-1 8.000000+5 8.462291-1 9.000000+5 9.394777-19343 3 4 10 1.000000+6 1.034999+0 1.100000+6 1.114168+0 1.200000+6 1.188168+09343 3 4 11 1.300000+6 1.257314+0 1.400000+6 1.321833+0 1.500000+6 1.379819+09343 3 4 12 1.600000+6 1.432695+0 1.700000+6 1.477240+0 1.800000+6 1.517284+09343 3 4 13 1.900000+6 1.548997+0 2.000000+6 1.577112+0 2.300000+6 1.630173+09343 3 4 14 2.500000+6 1.648278+0 2.700000+6 1.658798+0 3.000000+6 1.664195+09343 3 4 15 3.500000+6 1.662604+0 4.000000+6 1.650822+0 4.500000+6 1.633620+09343 3 4 16 5.000000+6 1.622814+0 5.500000+6 1.608128+0 6.000000+6 1.567530+09343 3 4 17 6.500000+6 1.331060+0 7.000000+6 1.056372+0 7.500000+6 8.373618-19343 3 4 18 8.000000+6 6.874712-1 8.500000+6 5.845708-1 9.000000+6 5.171295-19343 3 4 19 9.500000+6 4.696693-1 1.000000+7 4.355240-1 1.050000+7 4.091185-19343 3 4 20 1.100000+7 3.880087-1 1.150000+7 3.702531-1 1.200000+7 3.540660-19343 3 4 21 1.250000+7 3.399438-1 1.300000+7 3.268168-1 1.350000+7 3.145717-19343 3 4 22 1.400000+7 3.024970-1 1.450000+7 2.917943-1 1.500000+7 2.811409-19343 3 4 23 1.550000+7 2.710937-1 1.600000+7 2.615506-1 1.650000+7 2.527938-19343 3 4 24 1.700000+7 2.441789-1 1.750000+7 2.362501-1 1.800000+7 2.284974-19343 3 4 25 1.850000+7 2.213415-1 1.900000+7 2.144128-1 1.950000+7 2.080357-19343 3 4 26 2.000000+7 2.020089-1 9343 3 4 27 9343 3 099999 9.323600+4 2.340190+2 0 0 0 09343 3 16 1 -5.736680+6-5.736680+6 0 0 1 309343 3 16 2 30 2 9343 3 16 3 5.761200+6 0.000000+0 6.000000+6 3.361740-3 6.500000+6 4.970070-29343 3 16 4 7.000000+6 1.062690-1 7.500000+6 1.550500-1 8.000000+6 1.938270-19343 3 16 5 8.500000+6 2.214090-1 9.000000+6 2.420740-1 9.500000+6 2.569710-19343 3 16 6 1.000000+7 2.701630-1 1.050000+7 2.823090-1 1.100000+7 2.923820-19343 3 16 7 1.150000+7 3.027530-1 1.200000+7 3.127260-1 1.250000+7 3.117320-19343 3 16 8 1.300000+7 2.973910-1 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