TENDL-2011 gen. purp. file: proton + B - 11 1 MeV - 200 MeV 99 0 0 0 5011.00000 10.9147300 -1 0 0 1 528 1451 1 0.0 0.0 0 0 0 6 528 1451 2 .998620000 200000000. 1 0 10010 0 528 1451 3 0.0 0.0 1 0 271 6 528 1451 4 5-B - 11 NRG EVAL-OCT11 A.J. Koning 528 1451 5 TENDL-2011 DIST- REV1- 528 1451 6 ----TENDL-2011 Material 528 REVISION 1 528 1451 7 -----Incident proton data 528 1451 8 ------ENDF-6 Format 528 1451 9 528 1451 10 TENDL-2011 (TALYS Evaluated Nuclear Data Library) 528 1451 11 528 1451 12 Charged particle transport library made by TALYS 528 1451 13 528 1451 14 Author: A.J. Koning, NRG Petten, The Netherlands 528 1451 15 528 1451 16 ************** G E N E R A L I N F O R M A T I O N ************* 528 1451 17 528 1451 18 This evaluated data file is based primarily on the nuclear model 528 1451 19 code TALYS [kon07], version 1.4. 528 1451 20 It is part of a large collection of isotopic 528 1451 21 evaluations, all created by running TALYS with either default or 528 1451 22 adjusted input parameters. This means that the data in this 528 1451 23 evaluation have been tested in detail for some isotopes against 528 1451 24 individual experimental data, while for other isotopes it is 528 1451 25 only as good as the global quality of TALYS at the present moment. 528 1451 26 The mutual quality of all individual evaluations is however 528 1451 27 consistent: The same set of nuclear models is used and, equally 528 1451 28 important, the same ENDF-6 formatting procedures for each isotope. 528 1451 29 The resulting data file provides a complete representation of 528 1451 30 nuclear data needed for transport, damage, heating, radioactivity, 528 1451 31 and shielding applications over the incident projectile energy 528 1451 32 range from 1.0E-11 to 200 MeV. 528 1451 33 528 1451 34 All transport data for neutrons, other particles, photons and 528 1451 35 residual nuclides are filed using a combination of MF1,3, 528 1451 36 and MF6. This includes cross sections, angular distributions, 528 1451 37 double-differential spectra, production cross sections, 528 1451 38 residual production (activation) cross sections and recoils. 528 1451 39 This evaluation can thus be used as both transport and activation 528 1451 40 library. The data file has been created automatically using the 528 1451 41 ENDF-6 format generator TEFAL. 528 1451 42 528 1451 43 ##### ORIGIN 528 1451 44 528 1451 45 All data < 200 MeV : Produced with TALYS code 528 1451 46 528 1451 47 *************************** T H E O R Y ************************** 528 1451 48 528 1451 49 TALYS is a computer code system for the prediction and analysis 528 1451 50 of nuclear reactions. TALYS simulates reactions that involve 528 1451 51 neutrons, gamma-rays, protons, deuterons, tritons, helions and 528 1451 52 alpha-particles, in the 1 keV - 200 MeV energy range and for 528 1451 53 target nuclides of mass 12 and heavier. This is achieved by 528 1451 54 implementing a suite of nuclear reaction models into a single 528 1451 55 code system. It enables to evaluate nuclear reactions from 528 1451 56 the unresolved resonance region up to intermediate energies. This 528 1451 57 evaluation is based on a theoretical analysis that utilizes the 528 1451 58 optical model, compound nucleus statistical theory, fission, 528 1451 59 direct reactions and pre-equilibrium processes, in combination 528 1451 60 with databases and models for nuclear structure. The following 528 1451 61 output of TALYS is stored in this data file: 528 1451 62 528 1451 63 - Elastic and non-elastic cross sections 528 1451 64 - Elastic scattering angular distributions 528 1451 65 - Residual production cross sections 528 1451 66 - Recoil data 528 1451 67 - Total particle cross sections, e.g. (p,xn), (p,xp),.. 528 1451 68 - Total particle energy spectra 528 1451 69 - Total particle double-differential spectra 528 1451 70 528 1451 71 Here follows a short description of the used nuclear models: 528 1451 72 528 1451 73 ##### OPTICAL MODEL 528 1451 74 528 1451 75 All optical model calculations are performed by ECIS-06 [ray94], 528 1451 76 in TALYS used as a subroutine. The default optical model 528 1451 77 potentials (OMP) used are the local and global parameterizations 528 1451 78 of Koning and Delaroche [kon03]. These are phenomenological OMPs 528 1451 79 for neutrons and protons which in principle are valid over the 528 1451 80 1 keV - 200 MeV energy range, though the low energy boundary of 528 1451 81 validity may differ from nucleus to nucleus. For neutrons and 528 1451 82 protons, the used parameterization is given in Eq. (7) of 528 1451 83 [kon03]. Revised versions of these potentials (unpublished) are 528 1451 84 used in the case of deformed nuclides. 528 1451 85 To calculate the transmission coefficients and reaction 528 1451 86 cross sections for deuterons, tritons, helions and alpha 528 1451 87 particles, we use OMPs that are directly derived from our nucleon 528 1451 88 potentials using Watanabe's folding approach. 528 1451 89 528 1451 90 ##### DIRECT REACTIONS 528 1451 91 528 1451 92 The built-in ECIS-06 is used for DWBA or coupled-channels 528 1451 93 calculations for rotational or vibrational (or a combination of 528 1451 94 these) nuclides, depending on the information present in the 528 1451 95 nuclear structure database of TALYS. 528 1451 96 In addition, a macroscopic, phenomenological model to describe 528 1451 97 giant resonances in the inelastic channel is used. For each 528 1451 98 multipolarity an energy weighted sum rule applies and a DWBA 528 1451 99 calculation with ECIS-06 is performed for each giant resonance 528 1451 100 state. The cross section is then spread over the continuum with a 528 1451 101 Gaussian distribution. 528 1451 102 528 1451 103 ##### COMPOUND NUCLEUS 528 1451 104 528 1451 105 For compound nucleus reactions we use the the Hauser-Feshbach 528 1451 106 model. The transmission coefficients have been generated 528 1451 107 with the aforementioned OMPs and the full j,l-dependence of the 528 1451 108 transmission coefficients in the Hauser-Feshbach model is used. 528 1451 109 For each nucleus that can be reached through a binary reaction, 528 1451 110 several discrete levels and a continuum described by level 528 1451 111 densities are included simultaneously as competing channels. 528 1451 112 528 1451 113 For each residual nucleus several discrete states 528 1451 114 are included as well as a continuum described by level densities. 528 1451 115 Multiple compound emission is continued until all reaction 528 1451 116 channels are closed and the population distribution of all 528 1451 117 residual nuclides is depleted, through gamma decay, until they 528 1451 118 end up in the ground state or in an isomer. 528 1451 119 528 1451 120 For the level density, we take the Constant Temperature Model 528 1451 121 with level density parameters as given in [kon08]. This employs 528 1451 122 the temperature law at low energies and a Fermi gas expression at 528 1451 123 high energies, and takes into account the damping of shell 528 1451 124 effects at high excitation energy. We have obtained the level 528 1451 125 density parameters from a simultaneous fit to all experimental 528 1451 126 discrete levels and D0 values from the RIPL library [rip09]. 528 1451 127 528 1451 128 Gamma-ray transmission coefficients are generated with the 528 1451 129 Kopecky-Uhl generalized Lorentzian for strength functions, with 528 1451 130 giant dipole resonance parameters taken from the RIPL library 528 1451 131 [rip09], and normalized with experimental radiative widths. 528 1451 132 528 1451 133 ##### PRE-EQUILIBRIUM REACTIONS 528 1451 134 528 1451 135 For pre-equilibrium reactions, which become important for 528 1451 136 incident energies above about 10 MeV, we use the two-component 528 1451 137 exciton model [kon04], in which the neutron or proton types of 528 1451 138 particles and holes are followed throughout the reaction. For 528 1451 139 energies above 20 MeV, multiple pre-equilibrium emission up to 528 1451 140 any order of particle emission was included in the calculations. 528 1451 141 A parameterization for the squared matrix element is used that is 528 1451 142 valid for the whole energy range of this evaluation. 528 1451 143 528 1451 144 For deuterons, tritons, helions and alpha-particles, an extra 528 1451 145 contribution was added from the pick/up and knock-out reaction 528 1451 146 model by Kalbach [kal05]. 528 1451 147 528 1451 148 For photons, the model of Akkermans and Gruppelaar [akk85] was 528 1451 149 applied, to simulate the direct and semi-direct capture 528 1451 150 processes. 528 1451 151 528 1451 152 The angular distribution systematics by Kalbach [kal88] were used 528 1451 153 to describe the angular distributions for all continuum 528 1451 154 particles. An isotopic distribution for photons was adopted. 528 1451 155 528 1451 156 ***************** F I L E I N F O R M A T I O N **************** 528 1451 157 528 1451 158 ##### MF1: GENERAL INFORMATION 528 1451 159 528 1451 160 - MT451 : Descriptive data and directory 528 1451 161 528 1451 162 This text and the full directory of used MF/MT sections. 528 1451 163 528 1451 164 ##### MF3: REACTION CROSS SECTIONS 528 1451 165 528 1451 166 All the data present in the following MT-sections have been 528 1451 167 calculated with TALYS. If the maximal cross section in an 528 1451 168 excitation function over the whole energy range does not exceed 528 1451 169 1.e-9 b, the MT-number is not included at all. Cross sections 528 1451 170 lower than 1.e-20 b are assumed to have no physical meaning and 528 1451 171 are set to zero. The minor reaction channels are also present 528 1451 172 but they are stored in MT5 and can be reproduced in combination 528 1451 173 with MF6. All MT numbers extend up to the highest incident energy. 528 1451 174 The following reaction channels/MT numbers are generally included: 528 1451 175 528 1451 176 - MT2 : Elastic scattering cross section: nuclear + 528 1451 177 interference terms 528 1451 178 528 1451 179 Obtained by integrating the "nuclear-plus-interference" angular 528 1451 180 distributions of MF=6. Note that because of the interference 528 1451 181 effect, the tabulations in both MF=6 and MF=3 can be negative at 528 1451 182 some energies and angles. 528 1451 183 528 1451 184 - MT5 : (p,anything) cross section 528 1451 185 528 1451 186 MT5 contains the reactions which can not be stored in any other 528 1451 187 MT-number. As the incident energy increases, the cross section 528 1451 188 of MT5 increases as more reaction channels are no longer stored 528 1451 189 under a specific MT number. The information of MF3/MT5 can be 528 1451 190 combined with MF6/MT5 to obtain residual production cross 528 1451 191 sections particle production cross sections and 528 1451 192 (double-)differential cross sections. 528 1451 193 528 1451 194 ##### MF6: PRODUCT ENERGY-ANGLE DISTRIBUTIONS 528 1451 195 528 1451 196 In MF6 we store all secondary energy, angle, and energy-angle 528 1451 197 distributions, as well as all residual and photon production 528 1451 198 cross sections. All data are generated with TALYS. 528 1451 199 528 1451 200 - MT2 : Elastic scattering angular distribution: nuclear + 528 1451 201 interference terms 528 1451 202 528 1451 203 Relative angular distributions are tabulated on an angular grid. 528 1451 204 They are obtained by using the "nuclear-plus-interference" option 528 1451 205 in MF=6, which corresponds to LAW=5, LTP=12, and the appropriate 528 1451 206 integrated cross section is stored in MF=3. Note that because 528 1451 207 of the interference effect, the tabulations in both MF=6 and 528 1451 208 MF=3 can be negative at some energies and angles. 528 1451 209 528 1451 210 - MT5 : (p,anything) yields and energy-angle distributions 528 1451 211 528 1451 212 MT5 contains the production yields of particles and residual 528 1451 213 products. It also contains the secondary energy-angle 528 1451 214 distributions for all particles and photons. First, the yields 528 1451 215 for neutrons are given for the whole energy range. Next, on a 528 1451 216 secondary energy grid the relative emission spectra are given 528 1451 217 together with the parameters for the Kalbach systematics for 528 1451 218 angular distributions. Inelastic scattering cross sections for 528 1451 219 discrete states have been broadened and added to the continuum 528 1451 220 spectra. This procedure is repeated for protons, deuterons, 528 1451 221 tritons, Helium-3, alpha particles and photons. Finally, the 528 1451 222 residual production yields are given per final product. All these 528 1451 223 yields and relative distributions can be multiplied with the 528 1451 224 cross sections given in MF3/MT5 to get the production cross 528 1451 225 sections and (double-)differential cross sections. 528 1451 226 528 1451 227 ***** F I L E C H E C K I N G A N D P R O C E S S I N G **** 528 1451 228 528 1451 229 This file has been checked successfully by the BNL checking 528 1451 230 codes CHECKR-8.0, FIZCON-8.0 and PSYCHE-8.0 [her08] and has 528 1451 231 been processed successfully into an MCNP library by the 528 1451 232 processing code NJOY99.90 [mac00]. 528 1451 233 528 1451 234 *********************** R E F E R E N C E S ********************** 528 1451 235 528 1451 236 [akk85] J.M. Akkermans and H. Gruppelaar, Phys. Lett. 157B, 95 528 1451 237 (1985). 528 1451 238 [her08] M. Herman, ENDF Utility Codes Release 8.0, (2008). 528 1451 239 [kal88] C. Kalbach, Phys. Rev. C37, 2350 (1988). 528 1451 240 [kal05] C. Kalbach, Phys. Rev. C71, 034606 (2005). 528 1451 241 [kon03] A.J. Koning and J.P. Delaroche, Nucl. Phys. A713, 231 528 1451 242 (2003). 528 1451 243 [kon04] A.J. Koning and M.C. Duijvestijn, Nucl. Phys. A744, 15 528 1451 244 (2004). 528 1451 245 [kon07] A.J. Koning, S. Hilaire and M.C. Duijvestijn, TALYS-1.0, 528 1451 246 Proceedings of the International Conference on Nuclear 528 1451 247 Data for Science and Technology - ND-2007, 528 1451 248 April 22-27, 2007, Nice, France 528 1451 249 [kon08] A.J. Koning, S. Hilaire and S. Goriely, ``Global and 528 1451 250 local level density models'', Nucl Phys. A810, 528 1451 251 13-76 (2008). 528 1451 252 [mac00] R.E. Macfarlane, NJOY99 - Code system for producing 528 1451 253 pointwise and multigroup neutron and photon cross 528 1451 254 sections from ENDF/B Data, RSIC PSR-480 (2000). 528 1451 255 [ray94] J. Raynal, Notes on ECIS94, CEA Saclay Report 528 1451 256 No. CEA-N-2772, 1994. 528 1451 257 [rip09] R. Capote, M. Herman, P. Oblozinsky, P.G. Young, 528 1451 258 S. Goriely, T. Belgya, A.V. Ignatyuk, A.J. Koning, 528 1451 259 S. Hilaire, V. Plujko, M. Avrigeanu, O. Bersillon, 528 1451 260 M.B. Chadwick, T. Fukahori, S. Kailas, J. Kopecky, 528 1451 261 V.M. Maslov, G. Reffo, M. Sin, E. Soukhovitskii, 528 1451 262 P. Talou, H. Yinlu, and G. Zhigang, 528 1451 263 RIPL - Reference Input Parameter Library for calculation 528 1451 264 of nuclear reactions and nuclear data evaluation, 528 1451 265 Nucl. Data Sheets 110, 3107 (2009). 528 1451 266 528 1451 267 ************************* C O N T E N T S ************************ 528 1451 268 528 1451 269 *************** PROGRAM ACTIVATE (VERSION 2010-1) *************** 528 1451 270 MF=10 Activation Cross Sections Defined by Combining MF=3 528 1451 271 Cross Sections and MF=9 Multipliers. MF=9 Deleted. 528 1451 272 ***************** Program GROUPIE (VERSION 2011-1) ************** 528 1451 273 Unshielded Group Averages Using 162 Groups 528 1451 274 Weighting Spectrum: 1/E Spectrum 528 1451 275 1 451 275 1 528 1451 276 3 2 18 1 528 1451 277 3 5 18 1 528 1451 278 6 2 1401 1 528 1451 279 6 5 11903 1 528 1451 280 8 5 23 1 528 1451 281 528 1 0 282 528 0 0 283 5011.00000 10.9147300 0 0 0 0 528 3 2 284 0.0 0.0 0 0 1 67 528 3 2 285 67 1 528 3 2 286 7000000.00-.016826877 7200000.00-.012536252 7400000.00-.008245642 528 3 2 287 7600000.00-.003955045 7800000.00 3.35539E-4 8000000.00 .004094255 528 3 2 288 8200000.00 .007316656 8400000.00 .010539049 8600000.00 .013761435 528 3 2 289 8800000.00 .016983815 9000000.00 .019803763 9200000.00 .022218288 528 3 2 290 9400000.00 .024632809 9600000.00 .027047326 9800000.00 .029461840 528 3 2 291 10000000.0 .035200552 11000000.0 .043430834 12000000.0 .049974587 528 3 2 292 13000000.0 .055331684 14000000.0 .059813485 15000000.0 .063606634 528 3 2 293 16000000.0 .066823113 17000000.0 .069533824 18000000.0 .071791713 528 3 2 294 19000000.0 .073640990 20000000.0 .075602254 22000000.0 .077345106 528 3 2 295 24000000.0 .078090087 26000000.0 .078060877 28000000.0 .077436314 528 3 2 296 30000000.0 .075169183 35000000.0 .070820260 40000000.0 .065588760 528 3 2 297 45000000.0 .060067931 50000000.0 .055126499 54000000.0 .052418762 528 3 2 298 55000000.0 .049397630 60000000.0 .042410946 70000000.0 .034311709 528 3 2 299 80000000.0 .027859768 90000000.0 .022667200 100000000. .017067460 528 3 2 300 120000000. .011983534 140000000. .008907897 160000000. .007091180 528 3 2 301 180000000. .005950000 200000000. .005515377 240000000. .005515377 528 3 2 302 280000000. .005515377 320000000. .005515377 360000000. .005515377 528 3 2 303 400000000. .005515377 440000000. .005515377 480000000. .005515377 528 3 2 304 520000000. .005515377 560000000. .005515377 600000000. .005515377 528 3 2 305 640000000. .005515377 680000000. .005515377 720000000. .005515377 528 3 2 306 760000000. .005515377 800000000. .005515377 840000000. .005515377 528 3 2 307 880000000. .005515377 920000000. .005515377 960000000. .005515377 528 3 2 308 1.00000E+9 0.0 528 3 2 309 528 3 0 310 5011.00000 10.9147300 0 0 0 0 528 3 5 311 0.0 0.0 0 0 1 106 528 3 5 312 106 1 528 3 5 313 1000000.00 .435780240 1125000.00 .436393373 1250000.00 .437006386 528 3 5 314 1375000.00 .437619309 1500000.00 .438232165 1625000.00 .438844968 528 3 5 315 1750000.00 .439457729 1875000.00 .440070456 2000000.00 .441712648 528 3 5 316 2125000.00 .444405926 2250000.00 .447099119 2375000.00 .449792242 528 3 5 317 2500000.00 .452485303 2625000.00 .455178312 2750000.00 .457871276 528 3 5 318 2875000.00 .460564201 3000000.00 .466093908 3125000.00 .474500030 528 3 5 319 3250000.00 .482906067 3375000.00 .491312028 3500000.00 .499717922 528 3 5 320 3625000.00 .508123755 3750000.00 .516529534 3875000.00 .524935263 528 3 5 321 4000000.00 .532660304 4200000.00 .539719639 4400000.00 .546778856 528 3 5 322 4600000.00 .553837969 4800000.00 .560896991 5000000.00 .568095017 528 3 5 323 5200000.00 .575433922 5400000.00 .582772762 5600000.00 .590111542 528 3 5 324 5800000.00 .597450270 6000000.00 .602655672 6200000.00 .605703936 528 3 5 325 6400000.00 .608752184 6600000.00 .611800417 6800000.00 .614848637 528 3 5 326 7000000.00 .616771155 7200000.00 .617557205 7400000.00 .618343253 528 3 5 327 7600000.00 .619129299 7800000.00 .619915342 8000000.00 .620616732 528 3 5 328 8200000.00 .621232763 8400000.00 .621848792 8600000.00 .622464820 528 3 5 329 8800000.00 .623080846 9000000.00 .623182772 9200000.00 .622766776 528 3 5 330 9400000.00 .622350780 9600000.00 .621934785 9800000.00 .621518790 528 3 5 331 10000000.0 .623416111 11000000.0 .631355225 12000000.0 .636900269 528 3 5 332 13000000.0 .636949381 14000000.0 .636648853 15000000.0 .633530487 528 3 5 333 16000000.0 .627843695 17000000.0 .620542915 18000000.0 .612244072 528 3 5 334 19000000.0 .603393732 20000000.0 .589751517 22000000.0 .571431661 528 3 5 335 24000000.0 .553601516 26000000.0 .536537692 28000000.0 .520330603 528 3 5 336 30000000.0 .494856370 35000000.0 .461040193 40000000.0 .431435544 528 3 5 337 45000000.0 .405507174 50000000.0 .384830863 54000000.0 .374118489 528 3 5 338 55000000.0 .362790358 60000000.0 .337711931 70000000.0 .309925196 528 3 5 339 80000000.0 .288176844 90000000.0 .270453611 100000000. .250428838 528 3 5 340 120000000. .230457214 140000000. .216202377 160000000. .205671261 528 3 5 341 180000000. .197245838 200000000. .193430000 240000000. .193430000 528 3 5 342 280000000. .193430000 320000000. .193430000 360000000. .193430000 528 3 5 343 400000000. .193430000 440000000. .193430000 480000000. .193430000 528 3 5 344 520000000. .193430000 560000000. .193430000 600000000. .193430000 528 3 5 345 640000000. .193430000 680000000. .193430000 720000000. .193430000 528 3 5 346 760000000. .193430000 800000000. .193430000 840000000. .193430000 528 3 5 347 880000000. .193430000 920000000. .193430000 960000000. .193430000 528 3 5 348 1.00000E+9 0.0 528 3 5 349 528 3 0 350 528 0 0 351 5011.00000 10.9147300 0 0 23 0 52810 5 352 0.0 0.0 1 0 1 90 52810 5 353 90 1 52810 5 354 3000000.00 .003814711 3125000.00 .011497419 3250000.00 .019180050 52810 5 355 3375000.00 .026862612 3500000.00 .034545112 3625000.00 .042227557 52810 5 356 3750000.00 .049909952 3875000.00 .057592302 4000000.00 .063289127 52810 5 357 4200000.00 .066991244 4400000.00 .070693298 4600000.00 .074395299 52810 5 358 4800000.00 .078097251 5000000.00 .082548392 5200000.00 .087758772 52810 5 359 5400000.00 .092969105 5600000.00 .098179396 5800000.00 .103389650 52810 5 360 6000000.00 .106865808 6200000.00 .108588515 6400000.00 .110311213 52810 5 361 6600000.00 .112033903 6800000.00 .113756585 7000000.00 .116478055 52810 5 362 7200000.00 .120207867 7400000.00 .123937665 7600000.00 .127667452 52810 5 363 7800000.00 .131397228 8000000.00 .134624800 8200000.00 .137345968 52810 5 364 8400000.00 .140067129 8600000.00 .142788285 8800000.00 .145509436 52810 5 365 9000000.00 .147192382 9200000.00 .147829409 9400000.00 .148466435 52810 5 366 9600000.00 .149103460 9800000.00 .149740485 10000000.0 .155796225 52810 5 367 11000000.0 .146266537 12000000.0 .131229115 13000000.0 .132976816 52810 5 368 14000000.0 .141058859 15000000.0 .156954980 16000000.0 .171340715 52810 5 369 17000000.0 .180619511 18000000.0 .186061850 19000000.0 .189001340 52810 5 370 20000000.0 .192559869 22000000.0 .198532697 24000000.0 .206893402 52810 5 371 26000000.0 .216452986 28000000.0 .227404140 30000000.0 .246976771 52810 5 372 35000000.0 .271441170 40000000.0 .286845810 45000000.0 .295247384 52810 5 373 50000000.0 .299953962 54000000.0 .300723104 55000000.0 .302771202 52810 5 374 60000000.0 .305325481 70000000.0 .301764524 80000000.0 .299362969 52810 5 375 90000000.0 .300152366 100000000. .299201854 120000000. .295948731 52810 5 376 140000000. .295009626 160000000. .295320877 180000000. .295878342 52810 5 377 200000000. .295508814 240000000. .295508814 280000000. .295508814 52810 5 378 320000000. .295508814 360000000. .295508814 400000000. .295508814 52810 5 379 440000000. .295508814 480000000. .295508814 520000000. .295508814 52810 5 380 560000000. .295508814 600000000. .295508814 640000000. .295508814 52810 5 381 680000000. .295508814 720000000. .295508814 760000000. .295508814 52810 5 382 800000000. .295508814 840000000. .295508814 880000000. .295508814 52810 5 383 920000000. .295508814 960000000. .295508814 1.00000E+9 0.0 52810 5 384 0.0 0.0 1001 0 1 106 52810 5 385 106 1 52810 5 386 1000000.00 2.4220E-11 1125000.00 7.3681E-11 1250000.00 1.2313E-10 52810 5 387 1375000.00 1.7258E-10 1500000.00 2.2202E-10 1625000.00 2.7145E-10 52810 5 388 1750000.00 3.2088E-10 1875000.00 3.7031E-10 2000000.00 4.99927E-4 52810 5 389 2125000.00 .001510276 2250000.00 .002520593 2375000.00 .003530884 52810 5 390 2500000.00 .004541152 2625000.00 .005551400 2750000.00 .006561632 52810 5 391 2875000.00 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