IRDFF-v1-05_g.zip separated 31.08.15 by O.Gritzay using div-lib 6000 0 0 0 92238.0000 236.005800 0 1 34 19237 1451 1 0.0 1.00000000 0 0 0 69237 1451 2 1.00000000 200000000. 0 0 10 09237 1451 3 300.000000 0.0 1 0 592 139237 1451 4 92-U -238 ORNL,LANL+ EVAL-Feb14 IAEA 9237 1451 5 DIST-Feb14 REV - 9237 1451 6 ----IRDF-0 MATERIAL 9237 9237 1451 7 -----INCIDENT NEUTRON DATA 9237 1451 8 ------ENDF-6 FORMAT 9237 1451 9 ******************************************************************9237 1451 10 IAEA, March 2014 (A. Trkov) 9237 1451 11 A new evaluation of the (n,2n) reaction up to 30 MeV was done by 9237 1451 12 Zolotarev. All reactions were extended to 60 MeV using TENDL-2013.9237 1451 13 9237 1451 14 IAEA, July 2011 (A. Trkov) 9237 1451 15 The dosimetry file prepared by Zolotarev and Pronyaev, which 9237 1451 16 is based on IAEA standards was extended to include the total 9237 1451 17 cross section from the ENDF/B-VII.1b3 library. 9237 1451 18 The original fission cross section evaluation extends to 200 MeV. 9237 1451 19 The data energy range for the other cross sections was extended 9237 1451 20 from 30 to 200 MeV for consistency with the fission cross section 9237 1451 21 using the data from the TENDL-2010 library. 9237 1451 22 9237 1451 23 The extended nu-bar data were taken from the ADS-HE library 9237 1451 24 available from the IAEA "https://www-nds.iaea.org/ads/". 9237 1451 25 9237 1451 26 The capture cross section covariance matrix was processed with 9237 1451 27 NJOY on a customised energy grid to reduce the number of 9237 1451 28 energy groups in order to avoid vers small or slightly negative 9237 1451 29 eigenvalues. 9237 1451 30 ******************************************************************9237 1451 31 ***************************************************************** 9237 1451 32 ------Russian Reactor Dosimetry File BEST-12 20133-10 9237 1451 33 ***************************************************************** 9237 1451 34 Author of evaluation: K.I.Zolotarev 9237 1451 35 ***************************************************************** 9237 1451 36 MF=3 9237 1451 37 MT= 16 - (n,2n) cross section 9237 1451 38 ----------------------------- 9237 1451 39 Microscopic experimental data [1-25] had been analyzed in the 9237 1451 40 process of preparation the input data base for the evaluation of 9237 1451 41 U-238(n,2n)U-237 reaction cross sections and their uncertainty. 9237 1451 42 During this procedure all experimental data if it was possible 9237 1451 43 were corrected for new recommended cross section data for monitor 9237 1451 44 reactions used in the measurements and to a new recommended decay 9237 1451 45 data. Recommended decay data for U-237 was taken from work [26]. 9237 1451 46 Correction for a new standards was applied to the experimental 9237 1451 47 data [1-2], [4-8], [10-25]. 9237 1451 48 Special corrections had been applied for the experimental data 9237 1451 49 [10] and [12-13]. 9237 1451 50 Experimental data of Chou Youpu [10] were renormalized to the 9237 1451 51 cross-section value of 961.1 mb at 14.03 MeV evaluated from the 9237 1451 52 representative experimental data [18-21]. 9237 1451 53 In addition to correction for a new standards data of Frehaut 9237 1451 54 et al. [12] were renormalized to the integral of cross section 9237 1451 55 calculated from experimental data by Filatenkov and Chuvaev [21] 9237 1451 56 in the overlapping energy range 13.47 - 14.86 MeV, Fc = 1.09095. 9237 1451 57 Experimental data by of Frehaut et al. [13] obtained in measure- 9237 1451 58 ments with T(p,n)He3 source in the energy range 6.49 - 13.09 MeV 9237 1451 59 had been multiplied for the same factor. 9237 1451 60 Data base for evaluation of the U-238(n,2n)U-237 reaction exci-9237 1451 61 tation function in the energies region from threshold to 30 MeV 9237 1451 62 was consisted from the experimental cross section data [2], [4-5],9237 1451 63 [7-14], [16-21], [25]. The relative shape of excitation function 9237 1451 64 above 19 MeV was taken the same as in the TENDL-2011 library [27].9237 1451 65 The absolute cross sections in the interval 19-30 MeV were calcu- 9237 1451 66 lated from TENDL-2011 data by normalizing at 19 MeV to a value of 9237 1451 67 273.0 mb measured by Veeser and Arthur [9]. 9237 1451 68 Experimental data of works [1], [3], [6] and Mather et al. [7] 9237 1451 69 at 12.4 MeV were rejected due to inconsistency with the main bulk 9237 1451 70 of experimental data. Experimental data given in the resent publi-9237 1451 71 cations [22-24] were also rejected due to systematically underes- 9237 1451 72 timation of the U-238(n,2n)U-237 reaction cross section in the 9237 1451 73 14-MeV region. 9237 1451 74 Statistical analysis of input database was performed by means 9237 1451 75 of PADE-2 code [28]. Rational function was used as the model 9237 1451 76 function [29]. 9237 1451 77 The evaluated U-238(n,2n)U-237 excitation function averaged 9237 1451 78 over U-235 thermal fission [30] and Cf-252 spontaneous fission 9237 1451 79 neutron spectra [31] are given below in comparison with experi- 9237 1451 80 mental data [32-34]. 9237 1451 81 9237 1451 82 ----------------------+-----------------+----------------------- 9237 1451 83 Type of spectrum | ,mb (calc.) | ,mb (measured) 9237 1451 84 ----------------------+-----------------+----------------------- 9237 1451 85 U-235 neutron fission | 14.708 | 18.16 +- 0.93 [32] 9237 1451 86 | | 18.98 +- 1.70 [33] 9237 1451 87 ----------------------+-----------------+----------------------- 9237 1451 88 CF-252 spont. fission | 20.607 | 20.61 +- 2.02 [34] 9237 1451 89 ----------------------+-----------------+----------------------- 9237 1451 90 9237 1451 91 MF=33 9237 1451 92 MT= 16 - (n,2n) cross section cov. matrix 9237 1451 93 ----------------------------------------- 9237 1451 94 Uncertainties in the evaluated excitation function for the 9237 1451 95 U-238(n,2n)U-237 reaction are given in the form of relative cova- 9237 1451 96 riance matrix for the 49-neutron energy groups (LB=5). Covariance 9237 1451 97 matrix of uncertainties was calculated simultaneously with recom- 9237 1451 98 mended cross section data by means of PADE-2 code [28]. 9237 1451 99 Eigenvalues of the 6-digits relative covariance matrix given 9237 1451 100 in the 33-file are the following: 9237 1451 101 9237 1451 102 3.54537E-07 3.56403E-07 3.60136E-07 3.64977E-07 9237 1451 103 3.70250E-07 3.76599E-07 3.83985E-07 3.92169E-07 9237 1451 104 4.01013E-07 4.10394E-07 4.20574E-07 4.32294E-07 9237 1451 105 4.46724E-07 4.64905E-07 4.88137E-07 5.16198E-07 9237 1451 106 5.47091E-07 5.91668E-07 6.64585E-07 7.58874E-07 9237 1451 107 8.48397E-07 1.06058E-06 1.25714E-06 1.65012E-06 9237 1451 108 1.99413E-06 2.82910E-06 3.48385E-06 4.21256E-06 9237 1451 109 5.47387E-06 6.86460E-06 8.28105E-06 9.67752E-06 9237 1451 110 1.10246E-05 1.23039E-05 1.34765E-05 1.55533E-05 9237 1451 111 2.02276E-05 2.51922E-05 3.04420E-05 8.62659E-04 9237 1451 112 1.29487E-03 1.79071E-03 1.89912E-03 2.62241E-03 9237 1451 113 2.86479E-03 8.38884E-03 3.20631E-02 8.31231E-02 9237 1451 114 1.08298E-01 9237 1451 115 9237 1451 116 References: 9237 1451 117 1. J.A.Phillips, Report AERE-NP/R-2033, Harwell, September 1956 9237 1451 118 2. J.D.Knight, R.K.Smith, B.Warren, Phys. Rev. 112 (1958) 259 9237 1451 119 3. G.P.Antropov et al., Atomnaja Energija, 5 (1958) 456 9237 1451 120 4. J.L.Perkin, R.F.Coleman, J. of Nuclear Energy AB14 (1961) 69 9237 1451 121 5. R.Batchelor, W.B.Gilboy, J.H.Towle, Nucl. Phys. 65 (1965) 236 9237 1451 122 6. D.S.Mather, L.F.Pain, Report AWRE-O-47/69, August 1969 9237 1451 123 7. D.S.Mather, P.F.Bampton, R.E.Coles, G.James, P.J.Nind, 9237 1451 124 Report AWRE-O-72/72, November 1972 9237 1451 125 8. J.H.Landrum, R.J.Nagel, M.Lindner, Phys. Rev. C8 (1973) 1938 9237 1451 126 9. L.R.Veeser, E.D.Arthur, Proc. of Int. Conf. on Neutr. Physics 9237 1451 127 and Nucl. Data for Reactors and Other Applied Purposes, AERE 9237 1451 128 Harwell, UK, 25-29 September 1978, Publ. by OECD/NEA 1978, 9237 1451 129 pp. 1054-1058. 9237 1451 130 10. Chou Youpu, "Measurement of U-238(n,2n) Cross-Sections" (in 9237 1451 131 Chinese), Report HSJ-77091, October 1978 9237 1451 132 11. H.Karius, A.Ackermann, W.Scobel, J. of Phys. G 5 (1979) 715 9237 1451 133 12. J.Frehaut, A.Bertin, R.Bois, J.Jary, G.Mosinski, Proc. of Sym-9237 1451 134 posium on Neutron Cross Sections from 10-50 MeV, BNL, Upton, 9237 1451 135 NY, USA, May 12-14, 1980, BNL-NCS-51245, (1), p.399, 1980 9237 1451 136 13. J.Frehaut, A.Bertin, R.Bois, Nucl. Sci. Eng. 74 (1980) 29-33 9237 1451 137 14. T.B.Ryves, P.Kolkowski, Report INDC(UK)-32, p.87, Murch 1980 9237 1451 138 15. N.V.Kornilov, B.V.Zhuravlev, O.A.Sal'nikov, P.Raics, S.Nagy, 9237 1451 139 S.Daroczy, K.Sailer, J.Csikai, Proc. of the 9th Int. Symp. on 9237 1451 140 The Interaction of Fast Neutrons with Nuclei, Gaussig, 26-30 9237 1451 141 November 1977, ZFK-410, p.68, 1980 9237 1451 142 16. P.Raics, S.Daroczy, S.Nagy, N.V.Kornilov, B.V.Zhuravlev, O.A. 9237 1451 143 Salnikov, Proc. of 5th All Union Conf. on Neutron Physics. 9237 1451 144 Kiev, 15-19 September 1980, v.1, p.236, M:CNIIAtominform-1980 9237 1451 145 17. R.Pepelnik, B.Anders, B.M.Bahal, Proc. of Int. Conf. on Nucl. 9237 1451 146 Data for Basic and Applied Physic, Santa Fe, New Mexico,13-17 9237 1451 147 May 1985, v.1, p.211 (JA46) 9237 1451 148 18. V.Ya.Golovnya et al., Proc. of 1st All Union Conf. on Neutron 9237 1451 149 Phys., 14-16 September 1987, Kiev, Moscow-1988, v.3, p.281 9237 1451 150 19. P.Raics, S.Nagy, S.Daroczy, N.V.Kornilov,Report INDC(HUN)-029,9237 1451 151 IAEA, Vienna, October 1990 9237 1451 152 20. C.Konno, Y.Ikeda, K.Oishi, K.Kawade, H.Yamamoto, H.Maekawa, 9237 1451 153 Report JAERI-1329, October 1993 9237 1451 154 21. A.A.Filatenkov, S.V.Chuvaev, Preprit RI-252,M.:CNIIAtominform,9237 1451 155 Moscow 1999 9237 1451 156 22. Xianggao Wang et al., Nucl. Instr. Meth. A 621 (2010) 326 9237 1451 157 23. Xianggao Wang et al., Nucl. Instr. Meth. B 268 (2010) 1949 9237 1451 158 24. Chuanxin Zhu et al., Nucl. Sci. Eng. 169 (2011) 188 9237 1451 159 25. H.Naik et al., J. Radioanal. Nucl. Chem. 293 (2012) 469 9237 1451 160 26. M.S.Basunia, Nuclear Data Sheets, v.107, p.3323,2006 9237 1451 161 27. A.J.Koning, D.Rochman, "Evaluated Nuclear Data Library 9237 1451 162 TENDL-2011". NRG Petten, The Netherlands, 2011 9237 1451 163 28. S.A.Badikov et al., Preprint FEI-1686, Obninsk, 1985 9237 1451 164 29. S.Badikov, N.Rabotnov, K.Zolotarev, Proc. of NEANSC Speciali- 9237 1451 165 st's Meeting on Evaluation and Processing of Covariance Data, 9237 1451 166 Oak Ridge, USA, 7-9 September 1992, OECD, Paris, 1993, p. 105 9237 1451 167 30. P.G.Young et al., Evaluated Neutron Data for Uranium-235, 9237 1451 168 ENDF/B-VII.1 Library, MAT=9228, MF=5, MT=18, eval. Sept. 2006 9237 1451 169 31. W.Mannhart, Report, INDC(NDS)-220/L,p.158, IAEA, Vienna, 1989 9237 1451 170 32. K.Kobayashi et al., Nucl. Sci. Technol. 13 (1976) 531-540 9237 1451 171 33. T.Hashimoto et al., Nucl. Sci. Technol. 15 (1978) 626 9237 1451 172 34. M.V.Blinov et al., Atomnaja Energija (Sov.) 65 (1988) 206 9237 1451 173 ***************************************************************** 9237 1451 174 MF=3 9237 1451 175 MT= 18 - (n,f) cross section 9237 1451 176 MT=102 - (n,g) cross section 9237 1451 177 ----------------------------- 9237 1451 178 U-238(n,f) and U-238(n,g) reactions for neutron dosimetry 9237 1451 179 File was compiled, checked and processed by V. Pronyaev 9237 1451 180 and K. Zolotarev for Neutron Dosimetry Library 9237 1451 181 with evaluations included: 9237 1451 182 9237 1451 183 238U(n,f) and 238U(n,g) cross sections and covariance matrices of 9237 1451 184 uncertainties for neutrons with energy between 1.0e-05 eV and 9237 1451 185 20 KeV (Resolved Resonance Region) were evaluated with code 9237 1451 186 SAMMY. Detailes are described below. 9237 1451 187 9237 1451 188 238U(n,f) cross section and covariance matrix of uncertainty 9237 1451 189 for neutrons with energy between 20 keV and 1 MeV was taken 9237 1451 190 from ENDF/B-VII.0 evaluation. Detailes are given below. 9237 1451 191 9237 1451 192 238U(n,f) cross section and covariance matrix of uncertainty 9237 1451 193 for neutron energy range between 1 MeV and 200 MeV was taken 9237 1451 194 from Standards evaluation [St07]. 9237 1451 195 9237 1451 196 238U(n,g) cross section and covariance matrix of uncertainty 9237 1451 197 for neutrons with energy between 20 keV and 2.2 MeV was taken 9237 1451 198 from Standards evaluation [St07]. 9237 1451 199 9237 1451 200 238U(n,g) cross section and cocovariance matrix of uncertainty 9237 1451 201 for neutrons in energy range 2.2 MeV and 30 MeV was taken from 9237 1451 202 ENDF/B-VII.0 evaluation. Detailes of evaluation are given below. 9237 1451 203 9237 1451 204 No correlations are given between cross sections 9237 1451 205 in the resolved resonance region and at higher energies. 9237 1451 206 9237 1451 207 Cross sections in the resolved resonance region were reconstructed9237 1451 208 in the point-wise form with RECENT code (release 2007) and 9237 1451 209 accuracy 0.2% and Doppler-broadened with T=300K with SIGMA1 code 9237 1451 210 (relase 2007) and following linearization (accuracy 0.2%) 9237 1451 211 9237 1451 212 ***************************************************************** 9237 1451 213 Detailed description 9237 1451 214 ***************************************************************** 9237 1451 215 Resonance parameter covariance was generated in the resolved 9237 1451 216 energy region (1.0-5 eV to 20.0 keV) with the computer code SAMMY 9237 1451 217 at ORNL. Experimental data and uncertainties were used to generate9237 1451 218 covariance data. SAMMY covariance information was converted in 9237 1451 219 the ENDF FILE32 representation. However, because of computer 9237 1451 220 storage concern the FILE32 was converted into the FILE33 (MT=1, 9237 1451 221 2, 18, and 102) representation with reduced computer storage but 9237 1451 222 approximating the features of the FILE32 representation. The full 9237 1451 223 FILE32 matrices can be obtained directly from ORNL. The 9237 1451 224 conversion was done with the PUFF-IV code. Above the resolved 9237 1451 225 resonance region (> 20.0 keV) covariance data were generated at 9237 1451 226 LANL. Uncertainty on nubar was also generated at LANL. 9237 1451 227 9237 1451 228 ***************************************************************** 9237 1451 229 9237 1451 230 ENDF/B-VII EVALUATION 9237 1451 231 9237 1451 232 P.G.Young, M.B.Chadwick, R.E.MacFarlane, W.B.Wilson, D.G.Madland, 9237 1451 233 P.Talou, T. Kawano (LANL) 9237 1451 234 and 9237 1451 235 H. Derrien, A. Courcelle, L. C. Leal, N. Larson (ORNL) 9237 1451 236 9237 1451 237 ----- DETAILED DESCRIPTION ----- 9237 1451 238 9237 1451 239 ----- RESOLVED RESONANCE PARAMETERS (1.e-5 ev - 20 keV) ----- 9237 1451 240 H. Derrien, A. Courcelle, L. C. Leal, N. Larson (ORNL, Oct 2004) 9237 1451 241 9237 1451 242 A new analysis of the resolved resonance region to 20 keV was 9237 1451 243 performed at Oak Ridge National Laboratory, dated October, 2004. 9237 1451 244 This evaluation was performed with the computer code SAMMY (La04) 9237 1451 245 using Reich-Moore formalism. Resonance parameters are obtained 9237 1451 246 from 0 to 20 keV. A description of the present evaluation can be 9237 1451 247 found in (De04). 9237 1451 248 9237 1451 249 1. 1.e-5 eV to 1 keV 9237 1451 250 The thermal capture value was adjusted to sigma0 = 2.683 b 9237 1451 251 (Trkov et al. [Tr04]). The shape of the capture cross-section in 9237 1451 252 the thermal range was checked with the capture measuremements of 9237 1451 253 Corvi et al. [Co87]. For the large s-wave 6.67 eV, 20.8 eV and 9237 1451 254 36.6 eV resonances, the seven transmission spectra of Olsen 9237 1451 255 [Ol77] were fitted with 4 transmission measurements of Meister et 9237 1451 256 al. [Me98] and the capture measurements of De-Saussure et al 9237 1451 257 [De73]. To get a better correction of residual errors in 9237 1451 258 experimental normalizations and backgrounds, SAMMY fits were 9237 1451 259 performed resonance by resonance up to 60 eV. The Crystal Lattice 9237 1451 260 Model of SAMMY for Doppler broadening was used to describe the 9237 1451 261 shape of the 6.67 eV resonance. 9237 1451 262 From 250 eV to 1 keV the Macklin et al. capture [Ma88] 9237 1451 263 measurements were included in the fit. The spin of several p-wave 9237 1451 264 resonances have been changed from the original evaluation 9237 1451 265 ([So94]) to account for the spin measurements of Gunsing et al. 9237 1451 266 [Gu97]. Reliable estimates of p-wave neutron widths 9237 1451 267 below 300 eV were given by Crawford et al. [Cr98] with very thick 9237 1451 268 uranium sample transmission measurements and were used as prior 9237 1451 269 parameters in the fit. 9237 1451 270 The fission widths (below 10 keV) are taken from ENDF\B-VI 9237 1451 271 [So94] and were deduced from the Measurements of Defilippo et al. 9237 1451 272 [De80] 9237 1451 273 9237 1451 274 2. 1 keV to 20 keV 9237 1451 275 The Olsen 1979 transmission data [Ol79] were analyzed in the 9237 1451 276 energy range 1 keV to 10 keV and the Harvey transmission data 9237 1451 277 [Ha88] in the energy range 1 keV to 20 keV. The capture data of 9237 1451 278 de Saussure[De73] and Macklin[Ma88] were analyzed in the energy 9237 1451 279 range 1 keV to 10 keV and 1 keV to 20 keV respectively. In 9237 1451 280 general, the thick sample transmissions calculated from the 9237 1451 281 resonance parameters and averaged over 1 keV energy intervals 9237 1451 282 agree within 1% with the experimental values of Harvey and within 9237 1451 283 1.5% with the experimental values of Olsen, in agreement with the 9237 1451 284 quoted experimental errors, The fit to the capture cross sections 9237 1451 285 could not be obtained without large normalization and background 9237 1451 286 corrections. 9237 1451 287 The value of the effective scattering radius, R'=9.48 fm, and 9237 1451 288 of the external resonance parameters, were obtained by assuming 9237 1451 289 that the normalization coefficients in Harvey and Olsen 9237 1451 290 experimental transmission were accurate within 1.0-1.5%. The 9237 1451 291 statistical properties of the resonance parameters were checked 9237 1451 292 against the Wigner distribution of the level spacing and the 9237 1451 293 Porter-Thomas distribution of the reduced neutron widths. 9237 1451 294 >> MF=3 NEUTRON CROSS SECTIONS 9237 1451 295 9237 1451 296 ----- GENERAL INFORMATION ----- 9237 1451 297 The energy range of the evaluation (Yo04) was increased to 30 9237 1451 298 MeV. The evaluation of radiative capture cross section 9237 1451 299 in the energy range 2.2 to 20 MeV was based mainly on experimental9237 1451 300 data, complimented by nuclear model calculations. Model parameters9237 1451 301 for the calculations were obtained by optimization with 9237 1451 302 experimental data. 9237 1451 303 MT=18: FISSION NEUTRON CROSS SECTION 9237 1451 304 20 keV - 1.0 MeV: The fission cross section in this energy 9237 1451 305 range is the same as ENDF/B-VI. That is, it is based on the 9237 1451 306 unresolved resonance parameter analysis of Froehner and Poenitz 9237 1451 307 (Fr88,Po81) and on the ENDF/B-VI standards analysis, which is 9237 1451 308 similar to the ENDF/B-VII analysis at these energies. 9237 1451 309 MT=102: NEUTRON RADIATIVE CAPTURE CROSS SECTION 9237 1451 310 2.2 - 30 MeV: Follows the JENDL-3.0 evaluation. The results 9237 1451 311 in the 8-14 MeV range agree closely with the measurements of 9237 1451 312 McDaniels et al. (Mc82) and Drake et al. (Dr71). 9237 1451 313 9237 1451 314 ***************************************************************** 9237 1451 315 -----------Standards Evaluation-----------------------------------9237 1451 316 9237 1451 317 The evaluation was done in the framework of an IAEA (Vienna, 9237 1451 318 Austria) Coordinated Research Project "On Improvement of the 9237 1451 319 Standard Cross Sections for Light Elements" with contributions by 9237 1451 320 the NEA (Paris,France) WPEC Subgroup 7 on Nuclear Data Standards 9237 1451 321 and the CSEWG (USA). 9237 1451 322 Participants of the Project: 9237 1451 323 Sergei A. Badikov, Institute of Physics and Power Engineering, 9237 1451 324 Russia 9237 1451 325 Chen Zhenpeng, Tsinghua University, China 9237 1451 326 Allan D. Carlson, National Institute of Standards and Technology, 9237 1451 327 USA 9237 1451 328 Evgeny V. Gai, Institute of Physics and Power Engineering, 9237 1451 329 Russia 9237 1451 330 Gerald M. Hale, Los Alamos National Laboratory, USA 9237 1451 331 Franz-Josef Hambsch, Institute for Reference Materials and 9237 1451 332 Measurements, Belgium 9237 1451 333 Hartmut M. Hofmann, Universitat Erlangen-Nurnberg, Germany 9237 1451 334 Nancy M. Larson, Oak Ridge National Laboratory, USA 9237 1451 335 Donald L. Smith, Argonne National Laboratory, USA 9237 1451 336 Soo-Youl Oh, Korea Atomic Energy Research Institute, 9237 1451 337 Republic of Korea 9237 1451 338 Siegfried Tagesen, Institute for Isotopenforschung and 9237 1451 339 Kernphysik der Universitat Wien, Austria 9237 1451 340 Herbert Vonach, Institute for Isotopenforschung and 9237 1451 341 Kernphysik der Universitat Wien, Austria 9237 1451 342 Vladimir G. Pronyaev, International Atomic Energy Agency, 9237 1451 343 Austria 9237 1451 344 9237 1451 345 The methodology of the evaluation, detailed description and 9237 1451 346 the final results are published by the IAEA as an IAEA report 9237 1451 347 [St07]. 9237 1451 348 9237 1451 349 The file presents a version for which all reactions used 9237 1451 350 in the fit are given. Due to the evaluation 9237 1451 351 methodology, the full covariance matrix of the data uncertainty 9237 1451 352 includes blocks describing cross-reaction and cross-material 9237 1451 353 correlations between data used in the fit. Blocks of covariance 9237 1451 354 matrices which contain at least one correlation coefficient 9237 1451 355 higher than 0.2 are given in the file. 9237 1451 356 Data are given for a neutron energy 9237 1451 357 range wider than that recommended for its use as a standard for 9237 1451 358 the (n,f) reaction (2 MeV - 200 MeV). Recommended values and 9237 1451 359 uncertainties representing only diagonal elements of the 9237 1451 360 covariance matrix are shown below: 9237 1451 361 Standard Reaction: 238U(n,f) 9237 1451 362 Neutron Cross Uncertainty Uncertainty 9237 1451 363 energy section (barn) (%) 9237 1451 364 (MeV) (barn) 9237 1451 365 0.1000E+01 0.01355137 1.6347e-4 1.2063e+0 9237 1451 366 0.1100E+01 0.03148451 3.9204e-4 1.2452e+0 9237 1451 367 0.1250E+01 0.03473557 4.4022e-4 1.2674e+0 9237 1451 368 0.1400E+01 0.19119852 1.6659e-3 8.7132e-1 9237 1451 369 0.1600E+01 0.42328233 3.2268e-3 7.6233e-1 9237 1451 370 0.1800E+01 0.48392439 3.5725e-3 7.3823e-1 9237 1451 371 0.2000E+01 0.53402727 3.7840e-3 7.0858e-1 9237 1451 372 0.2200E+01 0.54711402 3.9234e-3 7.1710e-1 9237 1451 373 0.2400E+01 0.54634309 3.9448e-3 7.2205e-1 9237 1451 374 0.2600E+01 0.54108868 3.8127e-3 7.0463e-1 9237 1451 375 0.2800E+01 0.53721997 4.1734e-3 7.7686e-1 9237 1451 376 0.3000E+01 0.52373956 3.6927e-3 7.0507e-1 9237 1451 377 0.3600E+01 0.54692267 3.7823e-3 6.9156e-1 9237 1451 378 0.4000E+01 0.55440109 3.9797e-3 7.1784e-1 9237 1451 379 0.4500E+01 0.55933835 4.1670e-3 7.4498e-1 9237 1451 380 0.4700E+01 0.55813689 4.2737e-3 7.6571e-1 9237 1451 381 0.5000E+01 0.54671151 3.9912e-3 7.3003e-1 9237 1451 382 0.5300E+01 0.54926082 4.5288e-3 8.2452e-1 9237 1451 383 0.5500E+01 0.54633789 4.3601e-3 7.9806e-1 9237 1451 384 0.5800E+01 0.56693575 4.7763e-3 8.4247e-1 9237 1451 385 0.6000E+01 0.61079005 5.3197e-3 8.7096e-1 9237 1451 386 0.6200E+01 0.68170787 6.3320e-3 9.2884e-1 9237 1451 387 0.6500E+01 0.81579519 6.9322e-3 8.4975e-1 9237 1451 388 0.7000E+01 0.93955131 7.8828e-3 8.3900e-1 9237 1451 389 0.7500E+01 0.98746213 8.8154e-3 8.9274e-1 9237 1451 390 0.7750E+01 0.98763222 9.8650e-3 9.9885e-1 9237 1451 391 0.8000E+01 1.01109156 8.5129e-3 8.4195e-1 9237 1451 392 0.8500E+01 1.00766137 8.9508e-3 8.8827e-1 9237 1451 393 0.9000E+01 1.00937717 8.8653e-3 8.7829e-1 9237 1451 394 0.1000E+02 1.00133567 9.4376e-3 9.4250e-1 9237 1451 395 0.1100E+02 1.00189688 1.0069e-2 1.0050e+0 9237 1451 396 0.1150E+02 0.99448715 1.0893e-2 1.0953e+0 9237 1451 397 0.1200E+02 0.97188595 9.8296e-3 1.0114e+0 9237 1451 398 0.1300E+02 1.01508870 8.6305e-3 8.5022e-1 9237 1451 399 0.1400E+02 1.14337812 8.1064e-3 7.0899e-1 9237 1451 400 0.1450E+02 1.18439534 7.4802e-3 6.3156e-1 9237 1451 401 0.1500E+02 1.23462382 9.8885e-3 8.0094e-1 9237 1451 402 0.1600E+02 1.30827191 1.2582e-2 9.6175e-1 9237 1451 403 0.1700E+02 1.31415146 1.3445e-2 1.0231e+0 9237 1451 404 0.1800E+02 1.31518690 1.3620e-2 1.0356e+0 9237 1451 405 0.1900E+02 1.35485738 1.3201e-2 9.7435e-1 9237 1451 406 0.2000E+02 1.40508093 1.6740e-2 1.1914e+0 9237 1451 407 0.2100E+02 1.52303967 1.7942e-2 1.1781e+0 9237 1451 408 0.2200E+02 1.55700843 2.7329e-2 1.7552e+0 9237 1451 409 0.2300E+02 1.60853410 2.3972e-2 1.4903e+0 9237 1451 410 0.2400E+02 1.53992995 2.4822e-2 1.6119e+0 9237 1451 411 0.2500E+02 1.58738371 2.2312e-2 1.4056e+0 9237 1451 412 0.2600E+02 1.59398783 2.8481e-2 1.7868e+0 9237 1451 413 0.2700E+02 1.57152519 2.4641e-2 1.5680e+0 9237 1451 414 0.2800E+02 1.62263535 2.9828e-2 1.8382e+0 9237 1451 415 0.2900E+02 1.61977825 2.5477e-2 1.5729e+0 9237 1451 416 0.3000E+02 1.66646769 2.6773e-2 1.6066e+0 9237 1451 417 0.3200E+02 1.70629385 3.1686e-2 1.8570e+0 9237 1451 418 0.3400E+02 1.69270900 3.3224e-2 1.9628e+0 9237 1451 419 0.3600E+02 1.66316121 3.5784e-2 2.1515e+0 9237 1451 420 0.3800E+02 1.64705852 3.7713e-2 2.2897e+0 9237 1451 421 0.4000E+02 1.68559032 3.9563e-2 2.3471e+0 9237 1451 422 0.4200E+02 1.67482055 3.5903e-2 2.1437e+0 9237 1451 423 0.4400E+02 1.65536141 3.8723e-2 2.3392e+0 9237 1451 424 0.4600E+02 1.67419554 3.4671e-2 2.0709e+0 9237 1451 425 0.4800E+02 1.65428673 4.0710e-2 2.4609e+0 9237 1451 426 0.5000E+02 1.62322274 4.1298e-2 2.5442e+0 9237 1451 427 0.5200E+02 1.65580204 4.6284e-2 2.7953e+0 9237 1451 428 0.5400E+02 1.61877514 4.5193e-2 2.7918e+0 9237 1451 429 0.5600E+02 1.63615399 4.6041e-2 2.8140e+0 9237 1451 430 0.5800E+02 1.63340832 4.2344e-2 2.5924e+0 9237 1451 431 0.6000E+02 1.59203041 3.9195e-2 2.4619e+0 9237 1451 432 0.6400E+02 1.57558672 3.4663e-2 2.2000e+0 9237 1451 433 0.6800E+02 1.51199229 3.3580e-2 2.2209e+0 9237 1451 434 0.7200E+02 1.50280613 3.6385e-2 2.4212e+0 9237 1451 435 0.7600E+02 1.52304411 3.8955e-2 2.5577e+0 9237 1451 436 0.8000E+02 1.50702348 4.1528e-2 2.7556e+0 9237 1451 437 0.8400E+02 1.50774895 5.3160e-2 3.5258e+0 9237 1451 438 0.8800E+02 1.45066209 5.1832e-2 3.5730e+0 9237 1451 439 0.9200E+02 1.41977253 5.2522e-2 3.6993e+0 9237 1451 440 0.9600E+02 1.40219671* 5.3027e-2 3.7817e+0 9237 1451 441 0.1000E+03 1.40008093* 5.1398e-2 3.6711e+0 9237 1451 442 0.1040E+03 1.39448546* 5.3965e-2 3.8699e+0 9237 1451 443 0.1080E+03 1.37775279* 6.4604e-2 4.6891e+0 9237 1451 444 0.1120E+03 1.35742035* 6.1120e-2 4.5027e+0 9237 1451 445 0.1160E+03 1.34690512* 6.1431e-2 4.5609e+0 9237 1451 446 0.1200E+03 1.34095378* 6.0619e-2 4.5206e+0 9237 1451 447 0.1280E+03 1.33401941 5.8495e-2 4.3849e+0 9237 1451 448 0.1360E+03 1.32416210 5.7989e-2 4.3793e+0 9237 1451 449 0.1440E+03 1.31035094 5.4479e-2 4.1576e+0 9237 1451 450 0.1520E+03 1.32526144 5.7427e-2 4.3333e+0 9237 1451 451 0.1600E+03 1.30642175 5.8296e-2 4.4622e+0 9237 1451 452 0.1680E+03 1.29838942 5.9764e-2 4.6030e+0 9237 1451 453 0.1760E+03 1.32345065 5.9011e-2 4.4589e+0 9237 1451 454 0.1840E+03 1.32785692 6.5401e-2 4.9253e+0 9237 1451 455 0.1920E+03 1.30440723 5.8605e-2 4.4928e+0 9237 1451 456 0.2000E+03 1.33389620 5.8678e-2 4.3990e+0 9237 1451 457 * - smoothed cross sections 9237 1451 458 9237 1451 459 9237 1451 460 Recommended values (smoothed for En>0.18 MeV) and uncertainties 9237 1451 461 representing only diagonal elements of the covariance matrix for 9237 1451 462 the (n,g) reaction are shown below: 9237 1451 463 Reaction: 238U(n,g), MT=102 9237 1451 464 Neutron Cross Uncertainty Uncertainty 9237 1451 465 energy section (barn) (%) 9237 1451 466 (MeV) (barn) 9237 1451 467 0.2530E-07 2.67705834 0.01227690 0.5 9237 1451 468 0.1500E-03 16.40345905@ 0.10016508 0.6 9237 1451 469 0.2500E-03 8.38157160@ 0.11242939 1.3 9237 1451 470 0.3500E-03 2.86526321@ 0.04914795 1.7 9237 1451 471 0.4500E-03 2.66709032@ 0.02668240 1.0 9237 1451 472 0.5500E-03 4.43917681@ 0.12993952 2.9 9237 1451 473 0.6500E-03 3.40302929@ 0.06569958 1.9 9237 1451 474 0.7500E-03 1.72738697@ 0.03307590 1.9 9237 1451 475 0.8500E-03 2.83678450@ 0.02527669 0.9 9237 1451 476 0.9500E-03 3.70653977@ 0.07778262 2.1 9237 1451 477 0.1500E-02 1.82709885@ 0.02905043 1.6 9237 1451 478 0.2500E-02 1.37138213@ 0.01807938 1.3 9237 1451 479 0.3500E-02 1.12447832@ 0.01801082 1.6 9237 1451 480 0.4500E-02 0.89115124@ 0.01195889 1.3 9237 1451 481 0.5500E-02 0.85164887@ 0.01375318 1.6 9237 1451 482 0.6500E-02 0.76025636@ 0.01654485 2.2 9237 1451 483 0.7500E-02 0.72571914@ 0.01033383 1.4 9237 1451 484 0.8500E-02 0.63323845@ 0.00684449 1.1 9237 1451 485 0.9500E-02 0.66876151@ 0.01039564 1.6 9237 1451 486 0.1500E-01 0.57985893@ 0.00538843 0.9 9237 1451 487 0.2000E-01 0.52571225 0.00929082 1.8 9237 1451 488 0.2400E-01 0.46994887 0.00415725 0.9 9237 1451 489 0.3000E-01 0.43448746 0.00422828 1.0 9237 1451 490 0.4500E-01 0.35900098 0.00411795 1.1 9237 1451 491 0.5500E-01 0.28757234 0.00376471 1.3 9237 1451 492 0.6500E-01 0.24662623 0.00327425 1.3 9237 1451 493 0.7500E-01 0.21587377 0.00298115 1.4 9237 1451 494 0.8500E-01 0.19071497 0.00276572 1.5 9237 1451 495 0.9500E-01 0.18054793 0.00244102 1.4 9237 1451 496 0.1000E+00 0.17961668 0.00265317 1.5 9237 1451 497 0.1200E+00 0.16297159 0.00220029 1.4 9237 1451 498 0.1500E+00 0.14058370 0.00171056 1.2 9237 1451 499 0.1700E+00 0.13747810 0.00222319 1.6 9237 1451 500 0.1800E+00 0.12927828* 0.00418640 3.3 9237 1451 501 0.1900E+00 0.12662137* 0.00243970 1.9 9237 1451 502 0.2000E+00 0.12746494* 0.00234037 1.9 9237 1451 503 0.2100E+00 0.12787819* 0.00290525 2.2 9237 1451 504 0.2200E+00 0.12417342* 0.00271294 2.2 9237 1451 505 0.2300E+00 0.12080753* 0.00205540 1.7 9237 1451 506 0.2350E+00 0.11911300* 0.00534138 4.4 9237 1451 507 0.2400E+00 0.11682643* 0.00286433 2.5 9237 1451 508 0.2450E+00 0.11629365* 0.00246762 2.1 9237 1451 509 0.2500E+00 0.11599478* 0.00259474 2.3 9237 1451 510 0.2600E+00 0.11658732* 0.00207584 1.8 9237 1451 511 0.2700E+00 0.11765405* 0.00723798 6.0 9237 1451 512 0.2800E+00 0.11646769* 0.00267776 2.3 9237 1451 513 0.3000E+00 0.11568992* 0.00200258 1.7 9237 1451 514 0.3250E+00 0.11453138* 0.00331197 2.8 9237 1451 515 0.3500E+00 0.11111003* 0.00223272 2.1 9237 1451 516 0.3750E+00 0.10942991* 0.00235546 2.1 9237 1451 517 0.4000E+00 0.10898173* 0.00151340 1.4 9237 1451 518 0.4250E+00 0.10865831* 0.00595241 5.4 9237 1451 519 0.4500E+00 0.10760785* 0.00197978 1.8 9237 1451 520 0.4750E+00 0.10732578* 0.00565435 5.4 9237 1451 521 0.5000E+00 0.10824353* 0.00146107 1.3 9237 1451 522 0.5200E+00 0.10782893* 0.00204030 1.9 9237 1451 523 0.5400E+00 0.10909529* 0.00184566 1.7 9237 1451 524 0.5700E+00 0.11344814* 0.00181441 1.6 9237 1451 525 0.6000E+00 0.11286867* 0.00153277 1.3 9237 1451 526 0.6500E+00 0.11274003* 0.00328997 3.2 9237 1451 527 0.7000E+00 0.11833885* 0.00213918 1.6 9237 1451 528 0.7500E+00 0.11829182* 0.00326286 2.9 9237 1451 529 0.8000E+00 0.11881469* 0.00164640 1.4 9237 1451 530 0.8500E+00 0.12281274* 0.00581637 4.8 9237 1451 531 0.9000E+00 0.12549621* 0.00288284 2.3 9237 1451 532 0.9400E+00 0.12891020* 0.00291052 2.3 9237 1451 533 0.9600E+00 0.13052439* 0.00280863 2.1 9237 1451 534 0.1000E+01 0.12832436* 0.00264905 2.1 9237 1451 535 0.1100E+01 0.11350049* 0.00220267 1.9 9237 1451 536 0.1250E+01 0.09431692* 0.00166833 1.8 9237 1451 537 0.1400E+01 0.08034129* 0.00161086 2.0 9237 1451 538 0.1600E+01 0.06704474* 0.00127148 1.9 9237 1451 539 0.1800E+01 0.05686464* 0.00168891 3.0 9237 1451 540 0.2000E+01 0.04784651* 0.00125415 2.6 9237 1451 541 0.2200E+01 0.03856413 0.00105892 2.7 9237 1451 542 * - smoothed cross sections; @ - group averaged cross sections. 9237 1451 543 9237 1451 544 References 9237 1451 545 Co87 F. Corvi, G. Fioni, Proc. Conf. Nuc. Data for Sci. and 9237 1451 546 Tech., Mito, Japan, (1988). 9237 1451 547 Cr98 B. E. Crawford et al., Phys. Rev. C, 58, Num 2 (1998). 9237 1451 548 De73 G. De Saussure, E. G. Silver, R. B. Perez ,R. Ingle and H. 9237 1451 549 Weaver, Nucl. Sci. and Eng., 5, 385 (1973). 9237 1451 550 De80 F.C. Difilippo et al, Phys.Rev.C 21, 1400 (1980). 9237 1451 551 De04 H. Derrien, A. Courcelle, L. C. Leal, A.Santamarina Proc. 9237 1451 552 Int. Conf. on Nuc. Data for Sci. and Tech., Santa-Fe, USA 9237 1451 553 (2004). 9237 1451 554 Dr71 D. Drake, M. I. Bergqvist, and D. K. McDaniels, Phys. Lett. 9237 1451 555 B36, 557 (1971). 9237 1451 556 Fr88 F. H. Frohner, Nucl. Sci. and Eng.,103 (1988); F. H. 9237 1451 557 Frohner, Proc. Int. Conf. on Reactor Phys., Jackson Hole, 9237 1451 558 Wyoming (1988) Vol. III, p. 171. 9237 1451 559 Gu97 F. Gunsing, K. Athanassopulos, and F. Corvi, Phys. Rev. C, 9237 1451 560 56, Num 3 (1997). 9237 1451 561 Ha88 Harvey J. A., Hill N. W., Perey F. G., Tweed G. L. and Leal 9237 1451 562 L. C, Proc. Int. Conf. on nuclear data for Science and 9237 1451 563 Technology, Mito, Japan (1988). 9237 1451 564 La04 N. M. Larson, ORNL/TM-9179/R6 ENDF-364. 9237 1451 565 Ma88 Macklin Roger L., Perez R. B., De Saussure G. and Ingle 9237 1451 566 R. W., Proc. Int. Conf. on nuclear data for Science and 9237 1451 567 Technology, Mito, Japan (1988). 9237 1451 568 Mc82 D. K. McDaniels, P. Varghese, D. M. Drake, E. Arthur, A. 9237 1451 569 Lindholm, M. I. Bergqvist, and J. Krumlinde, Nuc. Phys. 9237 1451 570 A384, 88 (1982). 9237 1451 571 Me98 A. Meister et al., Proc. Conf. Nuc. Data, Long Island, 9237 1451 572 October 5-8, (1998). 9237 1451 573 Ol77 D.K. Olsen, G. De Saussure, R.B. Perez, F.C. Difilippo, R.W. 9237 1451 574 Ingle, and H. Weaver, Nucl. Sci. and Eng., 62, 479 (1977). 9237 1451 575 Ol79 D.K. Olsen, G. De Saussure, R.B. Perez, F.C. Difilippo, R.W. 9237 1451 576 Ingle, and H. Weaver, Nucl. Sci. and Eng., 69, 202-222 9237 1451 577 (1979). 9237 1451 578 Po81 W. P. Poenitz, L.R. Fawcett Jr and D.L. Smith, Nucl. Sci. 9237 1451 579 Eng., 78, (1981) 239-247. 9237 1451 580 So94 M. Moxon and M. Sowerby, NEA-OECD report (1994). 9237 1451 581 St07 International Evaluation of Neutron Cross-Section Standards, 9237 1451 582 STI/PUB/1291, IAEA, Vienna, Austria 92007) 9237 1451 583 Tr04 A. Trkov et al., personal communication, submitted to Nucl. 9237 1451 584 Sci. Eng. (2004). 9237 1451 585 Yo04 P. G. Young, M. B. Chadwick, R. E. MacFarlane, P. Talou, T. 9237 1451 586 Kawano, D. G. Madland, and W. B. Wilson, "Analysis and 9237 1451 587 Evaluation of Neutron Reactions on 238U," Los Alamos 9237 1451 588 National Laboratory report LA-UR-04-6456 (2004). 9237 1451 589 ***************************************************************** 9237 1451 590 ***************** Program LINEAR (VERSION 2012-1) ***************9237 1451 591 For All Data Greater than 1.0000D-10 barns in Absolute Value 9237 1451 592 Data Linearized to Within an Accuracy of .100000000 per-cent 9237 1451 593 ***************** Program GROUPIE (VERSION 2012-1) **************9237 1451 594 Unshielded Group Averages Using 640 Groups 9237 1451 595 Weighting Spectrum: Flat (Constant) Spectrum 9237 1451 596 1 451 603 19237 1451 597 1 452 27 19237 1451 598 1 455 7 19237 1451 599 1 456 27 19237 1451 600 1 458 5 19237 1451 601 2 151 4 19237 1451 602 3 1 67804 19237 1451 603 3 16 66 19237 1451 604 3 18 5471 19237 1451 605 3 102 221824 19237 1451 606 33 16 233 19237 1451 607 33 18 755 19237 1451 608 33 102 172 19237 1451 609 9237 1 0 610 92238.0000 236.005800 0 2 0 09237 1452 611 0.0 0.0 0 0 1 729237 1452 612 72 2 9237 1452 613 1.00000E-5 2.49208800 .025300000 2.49208800 .025300000 2.492088009237 1452 614 2900000.00 2.69876900 4000000.00 2.90860400 5150000.00 3.123837009237 1452 615 6000000.00 3.24999100 8000000.00 3.54028900 9000000.00 3.688423009237 1452 616 15850000.0 4.72780100 30000000.0 6.41410900 30000100.0 6.414109009237 1452 617 31000000.0 6.50730900 32000000.0 6.59920900 33000000.0 6.689609009237 1452 618 34000000.0 6.77881000 35000000.0 6.86661000 36000000.0 6.953110009237 1452 619 37000000.0 7.03831000 38000000.0 7.12221000 39000000.0 7.204910009237 1452 620 40000000.0 7.28631000 42000000.0 7.44561000 44000000.0 7.600211009237 1452 621 46000000.0 7.75021100 48000000.0 7.89581100 50000000.0 8.037111009237 1452 622 52000000.0 8.17421100 54000000.0 8.30721200 56000000.0 8.436312009237 1452 623 58000000.0 8.56161200 60000000.0 8.68321200 62000000.0 8.801212009237 1452 624 64000000.0 8.91581300 66000000.0 9.02691300 68000000.0 9.134713009237 1452 625 70000000.0 9.23941300 72000000.0 9.34101300 74000000.0 9.439513009237 1452 626 76000000.0 9.53521300 78000000.0 9.62801400 80000000.0 9.718114009237 1452 627 82000000.0 9.80551400 84000000.0 9.89031400 86000000.0 9.972714009237 1452 628 88000000.0 10.0530100 90000000.0 10.1300100 92000000.0 10.20501009237 1452 629 94000000.0 10.2780100 96000000.0 10.3490100 98000000.0 10.41801009237 1452 630 100000000. 10.4850100 105000000. 10.6430100 110000000. 10.79002009237 1452 631 115000000. 10.9260200 120000000. 11.0530200 125000000. 11.17002009237 1452 632 130000000. 11.2790200 135000000. 11.3800200 140000000. 11.47302009237 1452 633 145000000. 11.5600200 150000000. 11.6410200 155000000. 11.71602009237 1452 634 160000000. 11.7850200 165000000. 11.8490200 170000000. 11.90902009237 1452 635 175000000. 11.9650200 180000000. 12.0160200 185000000. 12.06402009237 1452 636 190000000. 12.1080200 195000000. 12.1490200 200000000. 12.18702009237 1452 637 9237 1 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18 1781 1.216000-5 1.176000-5 1.173000-5 1.178000-5 1.172000-5 1.183000-5923733 18 1782 1.181000-5 1.134000-5 1.116000-5 1.124000-5 1.112000-5 1.104000-5923733 18 1783 1.101000-5 1.081000-5 1.091000-5 1.099000-5 1.085000-5 1.092000-5923733 18 1784 1.098000-5 1.096000-5 1.034000-5 4.314000-5 2.014000-5 1.948000-5923733 18 1785 1.579000-5 1.507000-5 1.458000-5 1.415000-5 1.406000-5 1.381000-5923733 18 1786 1.388000-5 1.382000-5 1.401000-5 1.471000-5 1.443000-5 1.449000-5923733 18 1787 1.455000-5 1.469000-5 1.456000-5 1.440000-5 1.455000-5 1.467000-5923733 18 1788 1.451000-5 1.428000-5 1.371000-5 1.321000-5 1.168000-5 8.531000-6923733 18 1789 7.083000-6 1.019000-5 1.236000-5 1.334000-5 1.396000-5 1.407000-5923733 18 1790 1.477000-5 1.464000-5 1.448000-5 1.484000-5 1.507000-5 1.480000-5923733 18 1791 1.445000-5 1.485000-5 1.433000-5 1.473000-5 1.437000-5 1.328000-5923733 18 1792 1.289000-5 1.301000-5 1.285000-5 1.251000-5 1.257000-5 1.223000-5923733 18 1793 1.196000-5 1.237000-5 1.224000-5 1.210000-5 1.211000-5 1.211000-5923733 18 1794 1.213000-5 1.143000-5 1.229000-5 1.236000-5 1.251000-5 1.269000-5923733 18 1795 1.284000-5 1.243000-5 1.240000-5 1.246000-5 1.240000-5 1.251000-5923733 18 1796 1.249000-5 1.200000-5 1.182000-5 1.189000-5 1.176000-5 1.166000-5923733 18 1797 1.162000-5 1.140000-5 1.152000-5 1.160000-5 1.145000-5 1.153000-5923733 18 1798 1.158000-5 1.156000-5 1.091000-5 4.065000-5 2.131000-5 1.694000-5923733 18 1799 1.378000-5 1.381000-5 1.390000-5 1.370000-5 1.373000-5 1.356000-5923733 18 1800 1.344000-5 1.363000-5 1.431000-5 1.413000-5 1.422000-5 1.441000-5923733 18 1801 1.459000-5 1.450000-5 1.459000-5 1.472000-5 1.450000-5 1.416000-5923733 18 1802 1.382000-5 1.327000-5 1.280000-5 1.146000-5 8.404000-6 7.199000-6923733 18 1803 1.008000-5 1.217000-5 1.316000-5 1.380000-5 1.412000-5 1.451000-5923733 18 1804 1.435000-5 1.421000-5 1.460000-5 1.484000-5 1.452000-5 1.413000-5923733 18 1805 1.459000-5 1.402000-5 1.446000-5 1.412000-5 1.297000-5 1.256000-5923733 18 1806 1.267000-5 1.249000-5 1.214000-5 1.220000-5 1.185000-5 1.159000-5923733 18 1807 1.200000-5 1.186000-5 1.173000-5 1.174000-5 1.174000-5 1.177000-5923733 18 1808 1.105000-5 1.193000-5 1.200000-5 1.215000-5 1.233000-5 1.248000-5923733 18 1809 1.206000-5 1.204000-5 1.210000-5 1.205000-5 1.214000-5 1.212000-5923733 18 1810 1.164000-5 1.146000-5 1.153000-5 1.139000-5 1.130000-5 1.124000-5923733 18 1811 1.103000-5 1.115000-5 1.123000-5 1.109000-5 1.116000-5 1.121000-5923733 18 1812 1.119000-5 1.056000-5 5.135000-5 2.399000-5 1.658000-5 1.549000-5923733 18 1813 1.516000-5 1.512000-5 1.476000-5 1.502000-5 1.487000-5 1.522000-5923733 18 1814 1.573000-5 1.580000-5 1.584000-5 1.587000-5 1.560000-5 1.557000-5923733 18 1815 1.533000-5 1.568000-5 1.571000-5 1.579000-5 1.545000-5 1.476000-5923733 18 1816 1.424000-5 1.207000-5 8.659000-6 7.201000-6 1.043000-5 1.271000-5923733 18 1817 1.378000-5 1.441000-5 1.452000-5 1.504000-5 1.498000-5 1.514000-5923733 18 1818 1.528000-5 1.535000-5 1.536000-5 1.528000-5 1.532000-5 1.520000-5923733 18 1819 1.524000-5 1.465000-5 1.388000-5 1.362000-5 1.389000-5 1.379000-5923733 18 1820 1.342000-5 1.349000-5 1.308000-5 1.277000-5 1.325000-5 1.305000-5923733 18 1821 1.291000-5 1.292000-5 1.292000-5 1.295000-5 1.213000-5 1.314000-5923733 18 1822 1.322000-5 1.339000-5 1.359000-5 1.375000-5 1.318000-5 1.316000-5923733 18 1823 1.322000-5 1.317000-5 1.327000-5 1.325000-5 1.260000-5 1.241000-5923733 18 1824 1.247000-5 1.233000-5 1.222000-5 1.216000-5 1.192000-5 1.206000-5923733 18 1825 1.214000-5 1.200000-5 1.207000-5 1.211000-5 1.209000-5 1.142000-5923733 18 1826 4.072000-5 2.163000-5 1.664000-5 1.679000-5 1.690000-5 1.644000-5923733 18 1827 1.691000-5 1.655000-5 1.707000-5 1.721000-5 1.740000-5 1.769000-5923733 18 1828 1.775000-5 1.731000-5 1.739000-5 1.706000-5 1.750000-5 1.761000-5923733 18 1829 1.791000-5 1.746000-5 1.676000-5 1.602000-5 1.325000-5 9.324000-6923733 18 1830 7.650000-6 1.138000-5 1.399000-5 1.520000-5 1.589000-5 1.591000-5923733 18 1831 1.646000-5 1.650000-5 1.707000-5 1.698000-5 1.685000-5 1.725000-5923733 18 1832 1.756000-5 1.710000-5 1.753000-5 1.707000-5 1.611000-5 1.570000-5923733 18 1833 1.561000-5 1.610000-5 1.608000-5 1.565000-5 1.575000-5 1.520000-5923733 18 1834 1.481000-5 1.543000-5 1.512000-5 1.494000-5 1.494000-5 1.494000-5923733 18 1835 1.502000-5 1.396000-5 1.527000-5 1.536000-5 1.557000-5 1.581000-5923733 18 1836 1.601000-5 1.517000-5 1.517000-5 1.524000-5 1.518000-5 1.528000-5923733 18 1837 1.526000-5 1.433000-5 1.412000-5 1.417000-5 1.401000-5 1.386000-5923733 18 1838 1.377000-5 1.348000-5 1.366000-5 1.374000-5 1.360000-5 1.367000-5923733 18 1839 1.371000-5 1.369000-5 1.292000-5 3.883000-5 2.545000-5 1.941000-5923733 18 1840 1.752000-5 1.660000-5 1.748000-5 1.712000-5 1.729000-5 1.720000-5923733 18 1841 1.730000-5 1.752000-5 1.748000-5 1.707000-5 1.716000-5 1.684000-5923733 18 1842 1.730000-5 1.741000-5 1.774000-5 1.728000-5 1.655000-5 1.585000-5923733 18 1843 1.310000-5 9.302000-6 7.618000-6 1.126000-5 1.382000-5 1.501000-5923733 18 1844 1.568000-5 1.572000-5 1.625000-5 1.629000-5 1.688000-5 1.674000-5923733 18 1845 1.658000-5 1.701000-5 1.734000-5 1.684000-5 1.732000-5 1.683000-5923733 18 1846 1.590000-5 1.557000-5 1.549000-5 1.599000-5 1.598000-5 1.558000-5923733 18 1847 1.567000-5 1.515000-5 1.476000-5 1.536000-5 1.507000-5 1.489000-5923733 18 1848 1.489000-5 1.489000-5 1.497000-5 1.394000-5 1.521000-5 1.529000-5923733 18 1849 1.549000-5 1.573000-5 1.593000-5 1.512000-5 1.511000-5 1.518000-5923733 18 1850 1.512000-5 1.523000-5 1.520000-5 1.430000-5 1.409000-5 1.415000-5923733 18 1851 1.399000-5 1.385000-5 1.377000-5 1.349000-5 1.365000-5 1.374000-5923733 18 1852 1.359000-5 1.366000-5 1.371000-5 1.369000-5 1.292000-5 4.253000-5923733 18 1853 2.598000-5 2.304000-5 1.942000-5 1.675000-5 1.695000-5 1.727000-5923733 18 1854 1.733000-5 1.751000-5 1.772000-5 1.749000-5 1.705000-5 1.715000-5923733 18 1855 1.696000-5 1.738000-5 1.743000-5 1.770000-5 1.722000-5 1.652000-5923733 18 1856 1.579000-5 1.304000-5 9.261000-6 7.591000-6 1.124000-5 1.383000-5923733 18 1857 1.503000-5 1.573000-5 1.596000-5 1.631000-5 1.632000-5 1.690000-5923733 18 1858 1.671000-5 1.652000-5 1.694000-5 1.730000-5 1.676000-5 1.728000-5923733 18 1859 1.676000-5 1.585000-5 1.554000-5 1.548000-5 1.600000-5 1.600000-5923733 18 1860 1.560000-5 1.569000-5 1.518000-5 1.480000-5 1.539000-5 1.510000-5923733 18 1861 1.490000-5 1.491000-5 1.491000-5 1.499000-5 1.397000-5 1.523000-5923733 18 1862 1.531000-5 1.551000-5 1.575000-5 1.595000-5 1.515000-5 1.513000-5923733 18 1863 1.520000-5 1.514000-5 1.525000-5 1.523000-5 1.433000-5 1.411000-5923733 18 1864 1.418000-5 1.402000-5 1.388000-5 1.380000-5 1.352000-5 1.369000-5923733 18 1865 1.377000-5 1.362000-5 1.369000-5 1.375000-5 1.372000-5 1.295000-5923733 18 1866 4.650000-5 3.003000-5 2.551000-5 2.340000-5 2.112000-5 1.817000-5923733 18 1867 1.625000-5 1.712000-5 1.764000-5 1.769000-5 1.732000-5 1.743000-5923733 18 1868 1.756000-5 1.764000-5 1.753000-5 1.759000-5 1.703000-5 1.630000-5923733 18 1869 1.560000-5 1.294000-5 9.207000-6 7.378000-6 1.112000-5 1.380000-5923733 18 1870 1.507000-5 1.586000-5 1.638000-5 1.649000-5 1.644000-5 1.696000-5923733 18 1871 1.676000-5 1.657000-5 1.690000-5 1.720000-5 1.674000-5 1.719000-5923733 18 1872 1.674000-5 1.589000-5 1.551000-5 1.542000-5 1.592000-5 1.590000-5923733 18 1873 1.551000-5 1.560000-5 1.509000-5 1.472000-5 1.530000-5 1.503000-5923733 18 1874 1.485000-5 1.486000-5 1.486000-5 1.492000-5 1.392000-5 1.516000-5923733 18 1875 1.524000-5 1.543000-5 1.567000-5 1.586000-5 1.509000-5 1.507000-5923733 18 1876 1.514000-5 1.508000-5 1.519000-5 1.517000-5 1.431000-5 1.409000-5923733 18 1877 1.416000-5 1.399000-5 1.386000-5 1.379000-5 1.351000-5 1.367000-5923733 18 1878 1.376000-5 1.360000-5 1.368000-5 1.373000-5 1.371000-5 1.293000-5923733 18 1879 4.963000-5 2.817000-5 2.621000-5 2.320000-5 2.067000-5 1.910000-5923733 18 1880 1.709000-5 1.751000-5 1.790000-5 1.772000-5 1.783000-5 1.776000-5923733 18 1881 1.798000-5 1.793000-5 1.798000-5 1.750000-5 1.688000-5 1.611000-5923733 18 1882 1.353000-5 9.642000-6 8.082000-6 1.182000-5 1.457000-5 1.579000-5923733 18 1883 1.667000-5 1.760000-5 1.738000-5 1.710000-5 1.756000-5 1.740000-5923733 18 1884 1.725000-5 1.753000-5 1.775000-5 1.738000-5 1.771000-5 1.737000-5923733 18 1885 1.650000-5 1.597000-5 1.583000-5 1.630000-5 1.626000-5 1.583000-5923733 18 1886 1.593000-5 1.539000-5 1.500000-5 1.561000-5 1.532000-5 1.516000-5923733 18 1887 1.517000-5 1.516000-5 1.522000-5 1.417000-5 1.547000-5 1.556000-5923733 18 1888 1.577000-5 1.601000-5 1.621000-5 1.540000-5 1.539000-5 1.546000-5923733 18 1889 1.541000-5 1.551000-5 1.549000-5 1.459000-5 1.438000-5 1.444000-5923733 18 1890 1.427000-5 1.413000-5 1.404000-5 1.375000-5 1.392000-5 1.401000-5923733 18 1891 1.386000-5 1.393000-5 1.398000-5 1.396000-5 1.317000-5 4.429000-5923733 18 1892 3.000000-5 2.674000-5 2.334000-5 2.140000-5 1.995000-5 1.808000-5923733 18 1893 1.763000-5 1.781000-5 1.793000-5 1.797000-5 1.816000-5 1.796000-5923733 18 1894 1.782000-5 1.735000-5 1.667000-5 1.597000-5 1.379000-5 9.844000-6923733 18 1895 8.526000-6 1.217000-5 1.492000-5 1.626000-5 1.728000-5 1.878000-5923733 18 1896 1.807000-5 1.766000-5 1.799000-5 1.778000-5 1.769000-5 1.778000-5923733 18 1897 1.786000-5 1.767000-5 1.778000-5 1.764000-5 1.690000-5 1.615000-5923733 18 1898 1.589000-5 1.630000-5 1.620000-5 1.573000-5 1.582000-5 1.528000-5923733 18 1899 1.489000-5 1.551000-5 1.524000-5 1.502000-5 1.503000-5 1.503000-5923733 18 1900 1.513000-5 1.407000-5 1.539000-5 1.548000-5 1.569000-5 1.593000-5923733 18 1901 1.613000-5 1.537000-5 1.537000-5 1.544000-5 1.538000-5 1.549000-5923733 18 1902 1.547000-5 1.461000-5 1.440000-5 1.445000-5 1.428000-5 1.413000-5923733 18 1903 1.404000-5 1.375000-5 1.393000-5 1.401000-5 1.386000-5 1.393000-5923733 18 1904 1.398000-5 1.396000-5 1.317000-5 5.899000-5 3.394000-5 2.958000-5923733 18 1905 2.533000-5 2.399000-5 2.226000-5 1.802000-5 1.793000-5 1.822000-5923733 18 1906 1.815000-5 1.855000-5 1.837000-5 1.844000-5 1.801000-5 1.728000-5923733 18 1907 1.646000-5 1.376000-5 9.829000-6 8.196000-6 1.199000-5 1.476000-5923733 18 1908 1.602000-5 1.686000-5 1.761000-5 1.752000-5 1.741000-5 1.793000-5923733 18 1909 1.774000-5 1.754000-5 1.790000-5 1.822000-5 1.773000-5 1.819000-5923733 18 1910 1.773000-5 1.683000-5 1.636000-5 1.625000-5 1.679000-5 1.676000-5923733 18 1911 1.631000-5 1.641000-5 1.585000-5 1.545000-5 1.608000-5 1.579000-5923733 18 1912 1.546000-5 1.547000-5 1.547000-5 1.566000-5 1.455000-5 1.595000-5923733 18 1913 1.602000-5 1.623000-5 1.649000-5 1.671000-5 1.587000-5 1.586000-5923733 18 1914 1.593000-5 1.588000-5 1.598000-5 1.597000-5 1.501000-5 1.479000-5923733 18 1915 1.485000-5 1.467000-5 1.452000-5 1.443000-5 1.413000-5 1.431000-5923733 18 1916 1.440000-5 1.424000-5 1.431000-5 1.437000-5 1.434000-5 1.352000-5923733 18 1917 5.469000-5 3.078000-5 2.680000-5 2.497000-5 2.312000-5 1.945000-5923733 18 1918 1.733000-5 1.759000-5 1.769000-5 1.798000-5 1.787000-5 1.781000-5923733 18 1919 1.739000-5 1.674000-5 1.598000-5 1.352000-5 9.777000-6 8.018000-6923733 18 1920 1.180000-5 1.449000-5 1.567000-5 1.647000-5 1.703000-5 1.723000-5923733 18 1921 1.701000-5 1.744000-5 1.739000-5 1.729000-5 1.750000-5 1.766000-5923733 18 1922 1.738000-5 1.761000-5 1.736000-5 1.657000-5 1.592000-5 1.572000-5923733 18 1923 1.617000-5 1.611000-5 1.566000-5 1.576000-5 1.523000-5 1.484000-5923733 18 1924 1.545000-5 1.517000-5 1.495000-5 1.496000-5 1.495000-5 1.506000-5923733 18 1925 1.401000-5 1.532000-5 1.540000-5 1.561000-5 1.586000-5 1.606000-5923733 18 1926 1.528000-5 1.527000-5 1.534000-5 1.529000-5 1.539000-5 1.537000-5923733 18 1927 1.450000-5 1.428000-5 1.434000-5 1.417000-5 1.403000-5 1.394000-5923733 18 1928 1.365000-5 1.382000-5 1.391000-5 1.376000-5 1.383000-5 1.388000-5923733 18 1929 1.386000-5 1.307000-5 6.197000-5 3.466000-5 3.275000-5 3.006000-5923733 18 1930 2.502000-5 2.023000-5 1.782000-5 1.850000-5 1.917000-5 1.921000-5923733 18 1931 1.905000-5 1.838000-5 1.777000-5 1.683000-5 1.412000-5 9.972000-6923733 18 1932 8.180000-6 1.222000-5 1.509000-5 1.638000-5 1.719000-5 1.747000-5923733 18 1933 1.786000-5 1.783000-5 1.839000-5 1.837000-5 1.825000-5 1.856000-5923733 18 1934 1.882000-5 1.843000-5 1.878000-5 1.841000-5 1.750000-5 1.688000-5923733 18 1935 1.672000-5 1.724000-5 1.718000-5 1.669000-5 1.680000-5 1.621000-5923733 18 1936 1.579000-5 1.645000-5 1.615000-5 1.578000-5 1.579000-5 1.579000-5923733 18 1937 1.602000-5 1.486000-5 1.633000-5 1.640000-5 1.662000-5 1.690000-5923733 18 1938 1.713000-5 1.626000-5 1.626000-5 1.634000-5 1.628000-5 1.639000-5923733 18 1939 1.637000-5 1.539000-5 1.516000-5 1.521000-5 1.504000-5 1.488000-5923733 18 1940 1.477000-5 1.446000-5 1.465000-5 1.474000-5 1.458000-5 1.465000-5923733 18 1941 1.471000-5 1.468000-5 1.384000-5 6.685000-5 3.798000-5 3.204000-5923733 18 1942 2.632000-5 2.222000-5 2.038000-5 1.819000-5 1.910000-5 1.938000-5923733 18 1943 1.903000-5 1.842000-5 1.774000-5 1.700000-5 1.470000-5 1.024000-5923733 18 1944 8.329000-6 1.266000-5 1.566000-5 1.705000-5 1.789000-5 1.794000-5923733 18 1945 1.866000-5 1.860000-5 1.894000-5 1.924000-5 1.940000-5 1.930000-5923733 18 1946 1.914000-5 1.930000-5 1.904000-5 1.921000-5 1.846000-5 1.724000-5923733 18 1947 1.683000-5 1.718000-5 1.706000-5 1.660000-5 1.668000-5 1.612000-5923733 18 1948 1.566000-5 1.641000-5 1.597000-5 1.686000-5 1.680000-5 1.678000-5923733 18 1949 1.599000-5 1.492000-5 1.611000-5 1.634000-5 1.665000-5 1.683000-5923733 18 1950 1.694000-5 1.607000-5 1.603000-5 1.610000-5 1.604000-5 1.615000-5923733 18 1951 1.613000-5 1.520000-5 1.498000-5 1.503000-5 1.486000-5 1.470000-5923733 18 1952 1.460000-5 1.430000-5 1.449000-5 1.458000-5 1.442000-5 1.449000-5923733 18 1953 1.454000-5 1.451000-5 1.370000-5 7.727000-5 3.996000-5 3.075000-5923733 18 1954 2.529000-5 2.310000-5 2.060000-5 1.900000-5 1.959000-5 1.979000-5923733 18 1955 1.904000-5 1.827000-5 1.744000-5 1.477000-5 1.027000-5 8.342000-6923733 18 1956 1.269000-5 1.570000-5 1.708000-5 1.789000-5 1.793000-5 1.856000-5923733 18 1957 1.856000-5 1.915000-5 1.909000-5 1.917000-5 1.920000-5 1.919000-5923733 18 1958 1.915000-5 1.910000-5 1.910000-5 1.832000-5 1.732000-5 1.694000-5923733 18 1959 1.734000-5 1.727000-5 1.684000-5 1.690000-5 1.634000-5 1.584000-5923733 18 1960 1.666000-5 1.611000-5 1.777000-5 1.767000-5 1.764000-5 1.622000-5923733 18 1961 1.517000-5 1.622000-5 1.656000-5 1.692000-5 1.705000-5 1.709000-5923733 18 1962 1.612000-5 1.606000-5 1.612000-5 1.606000-5 1.617000-5 1.615000-5923733 18 1963 1.516000-5 1.493000-5 1.499000-5 1.482000-5 1.466000-5 1.457000-5923733 18 1964 1.426000-5 1.445000-5 1.454000-5 1.438000-5 1.445000-5 1.451000-5923733 18 1965 1.448000-5 1.366000-5 6.320000-5 3.767000-5 2.996000-5 2.754000-5923733 18 1966 2.416000-5 2.030000-5 1.964000-5 2.070000-5 1.993000-5 1.903000-5923733 18 1967 1.809000-5 1.518000-5 1.052000-5 8.565000-6 1.302000-5 1.611000-5923733 18 1968 1.754000-5 1.836000-5 1.843000-5 1.898000-5 1.898000-5 1.963000-5923733 18 1969 1.964000-5 1.956000-5 1.987000-5 2.009000-5 1.976000-5 2.004000-5923733 18 1970 1.973000-5 1.873000-5 1.797000-5 1.774000-5 1.827000-5 1.822000-5923733 18 1971 1.773000-5 1.783000-5 1.719000-5 1.670000-5 1.749000-5 1.705000-5923733 18 1972 1.752000-5 1.749000-5 1.747000-5 1.702000-5 1.581000-5 1.722000-5923733 18 1973 1.741000-5 1.771000-5 1.794000-5 1.810000-5 1.710000-5 1.708000-5923733 18 1974 1.715000-5 1.709000-5 1.720000-5 1.718000-5 1.609000-5 1.586000-5923733 18 1975 1.590000-5 1.572000-5 1.555000-5 1.544000-5 1.510000-5 1.531000-5923733 18 1976 1.540000-5 1.524000-5 1.531000-5 1.537000-5 1.534000-5 1.446000-5923733 18 1977 6.139000-5 3.737000-5 3.419000-5 2.950000-5 2.629000-5 2.193000-5923733 18 1978 2.083000-5 2.069000-5 1.978000-5 1.870000-5 1.561000-5 1.080000-5923733 18 1979 8.877000-6 1.343000-5 1.665000-5 1.807000-5 1.894000-5 1.922000-5923733 18 1980 1.957000-5 1.943000-5 2.030000-5 2.019000-5 2.005000-5 2.046000-5923733 18 1981 2.075000-5 2.034000-5 2.072000-5 2.032000-5 1.928000-5 1.860000-5923733 18 1982 1.838000-5 1.893000-5 1.885000-5 1.828000-5 1.839000-5 1.772000-5923733 18 1983 1.724000-5 1.799000-5 1.765000-5 1.731000-5 1.732000-5 1.731000-5923733 18 1984 1.753000-5 1.621000-5 1.787000-5 1.796000-5 1.821000-5 1.851000-5923733 18 1985 1.876000-5 1.777000-5 1.778000-5 1.786000-5 1.780000-5 1.791000-5923733 18 1986 1.789000-5 1.678000-5 1.654000-5 1.658000-5 1.639000-5 1.621000-5923733 18 1987 1.608000-5 1.573000-5 1.595000-5 1.605000-5 1.589000-5 1.595000-5923733 18 1988 1.601000-5 1.598000-5 1.507000-5 7.069000-5 4.367000-5 3.539000-5923733 18 1989 3.137000-5 2.738000-5 1.953000-5 2.076000-5 1.985000-5 1.880000-5923733 18 1990 1.598000-5 1.107000-5 9.168000-6 1.388000-5 1.730000-5 1.869000-5923733 18 1991 1.963000-5 2.015000-5 2.035000-5 2.011000-5 2.067000-5 2.084000-5923733 18 1992 2.090000-5 2.094000-5 2.087000-5 2.093000-5 2.078000-5 2.084000-5923733 18 1993 1.997000-5 1.878000-5 1.836000-5 1.875000-5 1.859000-5 1.799000-5923733 18 1994 1.810000-5 1.745000-5 1.698000-5 1.773000-5 1.739000-5 1.716000-5923733 18 1995 1.716000-5 1.716000-5 1.729000-5 1.601000-5 1.761000-5 1.771000-5923733 18 1996 1.797000-5 1.825000-5 1.849000-5 1.759000-5 1.760000-5 1.768000-5923733 18 1997 1.762000-5 1.773000-5 1.771000-5 1.669000-5 1.646000-5 1.649000-5923733 18 1998 1.631000-5 1.612000-5 1.600000-5 1.565000-5 1.587000-5 1.596000-5923733 18 1999 1.580000-5 1.587000-5 1.592000-5 1.589000-5 1.500000-5 9.077000-5923733 18 2000 4.071000-5 3.479000-5 3.041000-5 2.260000-5 2.073000-5 2.045000-5923733 18 2001 1.917000-5 1.607000-5 1.115000-5 9.370000-6 1.401000-5 1.745000-5923733 18 2002 1.886000-5 1.983000-5 2.063000-5 2.048000-5 2.029000-5 2.097000-5923733 18 2003 2.074000-5 2.066000-5 2.090000-5 2.105000-5 2.079000-5 2.097000-5923733 18 2004 2.075000-5 1.976000-5 1.891000-5 1.858000-5 1.907000-5 1.894000-5923733 18 2005 1.834000-5 1.845000-5 1.778000-5 1.729000-5 1.806000-5 1.770000-5923733 18 2006 1.746000-5 1.746000-5 1.745000-5 1.759000-5 1.628000-5 1.793000-5923733 18 2007 1.803000-5 1.829000-5 1.858000-5 1.882000-5 1.785000-5 1.786000-5923733 18 2008 1.794000-5 1.788000-5 1.799000-5 1.797000-5 1.688000-5 1.665000-5923733 18 2009 1.668000-5 1.649000-5 1.630000-5 1.617000-5 1.582000-5 1.604000-5923733 18 2010 1.614000-5 1.599000-5 1.605000-5 1.610000-5 1.606000-5 1.517000-5923733 18 2011 6.189000-5 3.645000-5 3.123000-5 2.439000-5 1.976000-5 1.972000-5923733 18 2012 1.884000-5 1.618000-5 1.123000-5 9.827000-6 1.420000-5 1.762000-5923733 18 2013 1.914000-5 2.034000-5 2.218000-5 2.108000-5 2.058000-5 2.103000-5923733 18 2014 2.086000-5 2.081000-5 2.087000-5 2.085000-5 2.081000-5 2.076000-5923733 18 2015 2.073000-5 1.983000-5 1.874000-5 1.835000-5 1.877000-5 1.861000-5923733 18 2016 1.801000-5 1.812000-5 1.746000-5 1.698000-5 1.774000-5 1.739000-5923733 18 2017 1.719000-5 1.719000-5 1.718000-5 1.730000-5 1.601000-5 1.762000-5923733 18 2018 1.773000-5 1.799000-5 1.827000-5 1.850000-5 1.757000-5 1.759000-5923733 18 2019 1.766000-5 1.760000-5 1.771000-5 1.769000-5 1.664000-5 1.642000-5923733 18 2020 1.644000-5 1.626000-5 1.607000-5 1.594000-5 1.559000-5 1.582000-5923733 18 2021 1.590000-5 1.576000-5 1.582000-5 1.586000-5 1.583000-5 1.497000-5923733 18 2022 6.990000-5 4.120000-5 3.179000-5 2.271000-5 1.980000-5 1.918000-5923733 18 2023 1.594000-5 1.111000-5 9.376000-6 1.381000-5 1.715000-5 1.855000-5923733 18 2024 1.954000-5 2.052000-5 2.019000-5 1.989000-5 2.052000-5 2.031000-5923733 18 2025 2.010000-5 2.052000-5 2.084000-5 2.037000-5 2.081000-5 2.035000-5923733 18 2026 1.927000-5 1.867000-5 1.848000-5 1.904000-5 1.898000-5 1.844000-5923733 18 2027 1.855000-5 1.788000-5 1.740000-5 1.815000-5 1.779000-5 1.758000-5923733 18 2028 1.759000-5 1.758000-5 1.769000-5 1.640000-5 1.801000-5 1.811000-5923733 18 2029 1.837000-5 1.865000-5 1.888000-5 1.788000-5 1.789000-5 1.797000-5923733 18 2030 1.791000-5 1.802000-5 1.800000-5 1.688000-5 1.665000-5 1.669000-5923733 18 2031 1.650000-5 1.632000-5 1.620000-5 1.585000-5 1.606000-5 1.616000-5923733 18 2032 1.600000-5 1.607000-5 1.612000-5 1.609000-5 1.520000-5 6.814000-5923733 18 2033 3.936000-5 2.897000-5 2.398000-5 1.865000-5 1.621000-5 1.132000-5923733 18 2034 9.312000-6 1.406000-5 1.741000-5 1.887000-5 1.980000-5 2.021000-5923733 18 2035 2.045000-5 2.024000-5 2.143000-5 2.096000-5 2.079000-5 2.116000-5923733 18 2036 2.144000-5 2.104000-5 2.138000-5 2.099000-5 1.992000-5 1.920000-5923733 18 2037 1.894000-5 1.948000-5 1.939000-5 1.880000-5 1.891000-5 1.822000-5923733 18 2038 1.773000-5 1.851000-5 1.814000-5 1.792000-5 1.792000-5 1.792000-5923733 18 2039 1.802000-5 1.669000-5 1.835000-5 1.846000-5 1.872000-5 1.902000-5923733 18 2040 1.926000-5 1.825000-5 1.826000-5 1.834000-5 1.828000-5 1.839000-5923733 18 2041 1.838000-5 1.724000-5 1.699000-5 1.704000-5 1.683000-5 1.665000-5923733 18 2042 1.653000-5 1.616000-5 1.638000-5 1.649000-5 1.631000-5 1.638000-5923733 18 2043 1.645000-5 1.642000-5 1.546000-5 7.983000-5 4.294000-5 3.609000-5923733 18 2044 3.025000-5 1.707000-5 1.107000-5 9.129000-6 1.407000-5 1.751000-5923733 18 2045 1.878000-5 1.953000-5 1.947000-5 2.004000-5 1.987000-5 2.194000-5923733 18 2046 2.066000-5 2.023000-5 2.100000-5 2.168000-5 2.075000-5 2.166000-5923733 18 2047 2.076000-5 1.944000-5 1.928000-5 1.922000-5 1.991000-5 1.991000-5923733 18 2048 1.934000-5 1.945000-5 1.873000-5 1.821000-5 1.904000-5 1.858000-5923733 18 2049 1.837000-5 1.837000-5 1.836000-5 1.849000-5 1.709000-5 1.884000-5923733 18 2050 1.895000-5 1.922000-5 1.951000-5 1.975000-5 1.859000-5 1.862000-5923733 18 2051 1.869000-5 1.862000-5 1.874000-5 1.871000-5 1.742000-5 1.721000-5923733 18 2052 1.724000-5 1.705000-5 1.685000-5 1.671000-5 1.635000-5 1.658000-5923733 18 2053 1.668000-5 1.653000-5 1.658000-5 1.663000-5 1.660000-5 1.571000-5923733 18 2054 9.201000-5 5.061000-5 4.220000-5 2.417000-5 1.264000-5 9.197000-6923733 18 2055 1.388000-5 1.783000-5 1.937000-5 1.996000-5 1.920000-5 1.997000-5923733 18 2056 2.001000-5 2.260000-5 2.104000-5 2.068000-5 2.125000-5 2.181000-5923733 18 2057 2.107000-5 2.177000-5 2.107000-5 1.989000-5 1.953000-5 1.935000-5923733 18 2058 1.997000-5 1.995000-5 1.939000-5 1.947000-5 1.878000-5 1.824000-5923733 18 2059 1.906000-5 1.858000-5 1.863000-5 1.858000-5 1.854000-5 1.863000-5923733 18 2060 1.727000-5 1.899000-5 1.912000-5 1.940000-5 1.960000-5 1.978000-5923733 18 2061 1.860000-5 1.874000-5 1.876000-5 1.862000-5 1.879000-5 1.871000-5923733 18 2062 1.742000-5 1.741000-5 1.731000-5 1.722000-5 1.702000-5 1.680000-5923733 18 2063 1.650000-5 1.675000-5 1.676000-5 1.679000-5 1.674000-5 1.672000-5923733 18 2064 1.668000-5 1.622000-5 1.110000-4 4.815000-5 2.678000-5 1.433000-5923733 18 2065 1.041000-5 1.422000-5 1.644000-5 1.860000-5 1.962000-5 1.890000-5923733 18 2066 1.933000-5 1.998000-5 2.158000-5 2.038000-5 2.006000-5 2.069000-5923733 18 2067 2.127000-5 2.046000-5 2.122000-5 2.046000-5 1.926000-5 1.898000-5923733 18 2068 1.885000-5 1.949000-5 1.948000-5 1.893000-5 1.903000-5 1.834000-5923733 18 2069 1.782000-5 1.862000-5 1.817000-5 1.812000-5 1.809000-5 1.806000-5923733 18 2070 1.816000-5 1.683000-5 1.851000-5 1.863000-5 1.890000-5 1.913000-5923733 18 2071 1.932000-5 1.818000-5 1.827000-5 1.831000-5 1.820000-5 1.835000-5923733 18 2072 1.829000-5 1.703000-5 1.695000-5 1.689000-5 1.678000-5 1.658000-5923733 18 2073 1.639000-5 1.608000-5 1.632000-5 1.636000-5 1.632000-5 1.631000-5923733 18 2074 1.632000-5 1.628000-5 1.568000-5 9.329000-5 3.054000-5 1.585000-5923733 18 2075 1.149000-5 1.565000-5 1.329000-5 1.692000-5 1.861000-5 1.824000-5923733 18 2076 1.852000-5 1.857000-5 1.943000-5 1.898000-5 1.884000-5 1.934000-5923733 18 2077 1.978000-5 1.918000-5 1.973000-5 1.914000-5 1.807000-5 1.768000-5923733 18 2078 1.753000-5 1.807000-5 1.805000-5 1.754000-5 1.763000-5 1.701000-5923733 18 2079 1.654000-5 1.728000-5 1.685000-5 1.678000-5 1.676000-5 1.674000-5923733 18 2080 1.683000-5 1.562000-5 1.715000-5 1.725000-5 1.750000-5 1.771000-5923733 18 2081 1.789000-5 1.687000-5 1.695000-5 1.699000-5 1.689000-5 1.703000-5923733 18 2082 1.697000-5 1.584000-5 1.575000-5 1.572000-5 1.560000-5 1.543000-5923733 18 2083 1.526000-5 1.497000-5 1.518000-5 1.523000-5 1.518000-5 1.517000-5923733 18 2084 1.519000-5 1.516000-5 1.457000-5 6.329000-5 1.992000-5 1.529000-5923733 18 2085 2.104000-5 1.808000-5 1.496000-5 1.590000-5 1.654000-5 1.702000-5923733 18 2086 1.660000-5 1.679000-5 1.715000-5 1.732000-5 1.719000-5 1.702000-5923733 18 2087 1.729000-5 1.694000-5 1.717000-5 1.663000-5 1.545000-5 1.500000-5923733 18 2088 1.521000-5 1.504000-5 1.457000-5 1.464000-5 1.418000-5 1.380000-5923733 18 2089 1.439000-5 1.408000-5 1.405000-5 1.403000-5 1.402000-5 1.407000-5923733 18 2090 1.312000-5 1.432000-5 1.441000-5 1.461000-5 1.478000-5 1.492000-5923733 18 2091 1.425000-5 1.432000-5 1.435000-5 1.426000-5 1.438000-5 1.433000-5923733 18 2092 1.356000-5 1.349000-5 1.347000-5 1.337000-5 1.323000-5 1.310000-5923733 18 2093 1.285000-5 1.303000-5 1.307000-5 1.303000-5 1.302000-5 1.304000-5923733 18 2094 1.302000-5 1.252000-5 4.127000-5 1.635000-5 1.946000-5 1.689000-5923733 18 2095 1.431000-5 1.222000-5 1.073000-5 1.195000-5 1.189000-5 1.194000-5923733 18 2096 1.186000-5 1.188000-5 1.182000-5 1.173000-5 1.184000-5 1.165000-5923733 18 2097 1.175000-5 1.143000-5 1.076000-5 1.048000-5 1.062000-5 1.052000-5923733 18 2098 1.025000-5 1.029000-5 1.002000-5 9.789000-6 1.013000-5 9.980000-6923733 18 2099 9.947000-6 9.937000-6 9.925000-6 9.955000-6 9.382000-6 1.010000-5923733 18 2100 1.016000-5 1.028000-5 1.039000-5 1.047000-5 1.008000-5 1.012000-5923733 18 2101 1.014000-5 1.006000-5 1.017000-5 1.013000-5 9.663000-6 9.613000-6923733 18 2102 9.623000-6 9.554000-6 9.474000-6 9.404000-6 9.248000-6 9.354000-6923733 18 2103 9.390000-6 9.344000-6 9.349000-6 9.373000-6 9.359000-6 9.009000-6923733 18 2104 3.089000-5 1.949000-5 1.461000-5 1.264000-5 1.108000-5 9.005000-6923733 18 2105 8.895000-6 9.333000-6 9.537000-6 9.458000-6 9.462000-6 9.371000-6923733 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