TENDL-2011 gen. purp. file: deuteron + Be- 7 1 MeV - 200 MeV 99 0 0 0 4007.00000 6.95665100 -1 0 0 1 419 1451 1 0.0 0.0 0 0 0 6 419 1451 2 1.99626000 200000000. 1 0 10020 0 419 1451 3 0.0 0.0 1 0 268 6 419 1451 4 4-Be- 7 NRG EVAL-NOV11 A.J. Koning 419 1451 5 TENDL-2011 DIST- REV1- 419 1451 6 ----TENDL-2011 Material 419 REVISION 1 419 1451 7 -----Incident deuteron data 419 1451 8 ------ENDF-6 Format 419 1451 9 419 1451 10 TENDL-2011 (TALYS Evaluated Nuclear Data Library) 419 1451 11 419 1451 12 Charged particle transport library made by TALYS 419 1451 13 419 1451 14 Author: A.J. Koning, NRG Petten, The Netherlands 419 1451 15 419 1451 16 ************** G E N E R A L I N F O R M A T I O N ************* 419 1451 17 419 1451 18 This evaluated data file is based primarily on the nuclear model 419 1451 19 code TALYS [kon07], version 1.4. 419 1451 20 It is part of a large collection of isotopic 419 1451 21 evaluations, all created by running TALYS with either default or 419 1451 22 adjusted input parameters. This means that the data in this 419 1451 23 evaluation have been tested in detail for some isotopes against 419 1451 24 individual experimental data, while for other isotopes it is 419 1451 25 only as good as the global quality of TALYS at the present moment. 419 1451 26 The mutual quality of all individual evaluations is however 419 1451 27 consistent: The same set of nuclear models is used and, equally 419 1451 28 important, the same ENDF-6 formatting procedures for each isotope. 419 1451 29 The resulting data file provides a complete representation of 419 1451 30 nuclear data needed for transport, damage, heating, radioactivity, 419 1451 31 and shielding applications over the incident projectile energy 419 1451 32 range from 1.0E-11 to 200 MeV. 419 1451 33 419 1451 34 All transport data for neutrons, other particles, photons and 419 1451 35 residual nuclides are filed using a combination of MF1,3, 419 1451 36 and MF6. This includes cross sections, angular distributions, 419 1451 37 double-differential spectra, production cross sections, 419 1451 38 residual production (activation) cross sections and recoils. 419 1451 39 This evaluation can thus be used as both transport and activation 419 1451 40 library. The data file has been created automatically using the 419 1451 41 ENDF-6 format generator TEFAL. 419 1451 42 419 1451 43 ##### ORIGIN 419 1451 44 419 1451 45 All data < 200 MeV : Produced with TALYS code 419 1451 46 419 1451 47 *************************** T H E O R Y ************************** 419 1451 48 419 1451 49 TALYS is a computer code system for the prediction and analysis 419 1451 50 of nuclear reactions. TALYS simulates reactions that involve 419 1451 51 neutrons, gamma-rays, protons, deuterons, tritons, helions and 419 1451 52 alpha-particles, in the 1 keV - 200 MeV energy range and for 419 1451 53 target nuclides of mass 12 and heavier. This is achieved by 419 1451 54 implementing a suite of nuclear reaction models into a single 419 1451 55 code system. It enables to evaluate nuclear reactions from 419 1451 56 the unresolved resonance region up to intermediate energies. This 419 1451 57 evaluation is based on a theoretical analysis that utilizes the 419 1451 58 optical model, compound nucleus statistical theory, fission, 419 1451 59 direct reactions and pre-equilibrium processes, in combination 419 1451 60 with databases and models for nuclear structure. The following 419 1451 61 output of TALYS is stored in this data file: 419 1451 62 419 1451 63 - Elastic and non-elastic cross sections 419 1451 64 - Elastic scattering angular distributions 419 1451 65 - Residual production cross sections 419 1451 66 - Recoil data 419 1451 67 - Total particle cross sections, e.g. (p,xn), (p,xp),.. 419 1451 68 - Total particle energy spectra 419 1451 69 - Total particle double-differential spectra 419 1451 70 419 1451 71 Here follows a short description of the used nuclear models: 419 1451 72 419 1451 73 ##### OPTICAL MODEL 419 1451 74 419 1451 75 All optical model calculations are performed by ECIS-06 [ray94], 419 1451 76 in TALYS used as a subroutine. The default optical model 419 1451 77 potentials (OMP) used are the local and global parameterizations 419 1451 78 of Koning and Delaroche [kon03]. These are phenomenological OMPs 419 1451 79 for neutrons and protons which in principle are valid over the 419 1451 80 1 keV - 200 MeV energy range, though the low energy boundary of 419 1451 81 validity may differ from nucleus to nucleus. For neutrons and 419 1451 82 protons, the used parameterization is given in Eq. (7) of 419 1451 83 [kon03]. Revised versions of these potentials (unpublished) are 419 1451 84 used in the case of deformed nuclides. 419 1451 85 To calculate the transmission coefficients and reaction 419 1451 86 cross sections for deuterons, tritons, helions and alpha 419 1451 87 particles, we use OMPs that are directly derived from our nucleon 419 1451 88 potentials using Watanabe's folding approach. 419 1451 89 419 1451 90 ##### DIRECT REACTIONS 419 1451 91 419 1451 92 The built-in ECIS-06 is used for DWBA or coupled-channels 419 1451 93 calculations for rotational or vibrational (or a combination of 419 1451 94 these) nuclides, depending on the information present in the 419 1451 95 nuclear structure database of TALYS. 419 1451 96 In addition, a macroscopic, phenomenological model to describe 419 1451 97 giant resonances in the inelastic channel is used. For each 419 1451 98 multipolarity an energy weighted sum rule applies and a DWBA 419 1451 99 calculation with ECIS-06 is performed for each giant resonance 419 1451 100 state. The cross section is then spread over the continuum with a 419 1451 101 Gaussian distribution. 419 1451 102 419 1451 103 ##### COMPOUND NUCLEUS 419 1451 104 419 1451 105 For compound nucleus reactions we use the the Hauser-Feshbach 419 1451 106 model. The transmission coefficients have been generated 419 1451 107 with the aforementioned OMPs and the full j,l-dependence of the 419 1451 108 transmission coefficients in the Hauser-Feshbach model is used. 419 1451 109 For each nucleus that can be reached through a binary reaction, 419 1451 110 several discrete levels and a continuum described by level 419 1451 111 densities are included simultaneously as competing channels. 419 1451 112 419 1451 113 For each residual nucleus several discrete states 419 1451 114 are included as well as a continuum described by level densities. 419 1451 115 Multiple compound emission is continued until all reaction 419 1451 116 channels are closed and the population distribution of all 419 1451 117 residual nuclides is depleted, through gamma decay, until they 419 1451 118 end up in the ground state or in an isomer. 419 1451 119 419 1451 120 For the level density, we take the Constant Temperature Model 419 1451 121 with level density parameters as given in [kon08]. This employs 419 1451 122 the temperature law at low energies and a Fermi gas expression at 419 1451 123 high energies, and takes into account the damping of shell 419 1451 124 effects at high excitation energy. We have obtained the level 419 1451 125 density parameters from a simultaneous fit to all experimental 419 1451 126 discrete levels and D0 values from the RIPL library [rip09]. 419 1451 127 419 1451 128 Gamma-ray transmission coefficients are generated with the 419 1451 129 Kopecky-Uhl generalized Lorentzian for strength functions, with 419 1451 130 giant dipole resonance parameters taken from the RIPL library 419 1451 131 [rip09], and normalized with experimental radiative widths. 419 1451 132 419 1451 133 ##### PRE-EQUILIBRIUM REACTIONS 419 1451 134 419 1451 135 For pre-equilibrium reactions, which become important for 419 1451 136 incident energies above about 10 MeV, we use the two-component 419 1451 137 exciton model [kon04], in which the neutron or proton types of 419 1451 138 particles and holes are followed throughout the reaction. For 419 1451 139 energies above 20 MeV, multiple pre-equilibrium emission up to 419 1451 140 any order of particle emission was included in the calculations. 419 1451 141 A parameterization for the squared matrix element is used that is 419 1451 142 valid for the whole energy range of this evaluation. 419 1451 143 419 1451 144 For deuterons, tritons, helions and alpha-particles, an extra 419 1451 145 contribution was added from the pick/up and knock-out reaction 419 1451 146 model by Kalbach [kal05]. 419 1451 147 419 1451 148 For photons, the model of Akkermans and Gruppelaar [akk85] was 419 1451 149 applied, to simulate the direct and semi-direct capture 419 1451 150 processes. 419 1451 151 419 1451 152 The angular distribution systematics by Kalbach [kal88] were used 419 1451 153 to describe the angular distributions for all continuum 419 1451 154 particles. An isotopic distribution for photons was adopted. 419 1451 155 419 1451 156 ***************** F I L E I N F O R M A T I O N **************** 419 1451 157 419 1451 158 ##### MF1: GENERAL INFORMATION 419 1451 159 419 1451 160 - MT451 : Descriptive data and directory 419 1451 161 419 1451 162 This text and the full directory of used MF/MT sections. 419 1451 163 419 1451 164 ##### MF3: REACTION CROSS SECTIONS 419 1451 165 419 1451 166 All the data present in the following MT-sections have been 419 1451 167 calculated with TALYS. If the maximal cross section in an 419 1451 168 excitation function over the whole energy range does not exceed 419 1451 169 1.e-9 b, the MT-number is not included at all. Cross sections 419 1451 170 lower than 1.e-20 b are assumed to have no physical meaning and 419 1451 171 are set to zero. The minor reaction channels are also present 419 1451 172 but they are stored in MT5 and can be reproduced in combination 419 1451 173 with MF6. All MT numbers extend up to the highest incident energy. 419 1451 174 The following reaction channels/MT numbers are generally included: 419 1451 175 419 1451 176 - MT2 : Elastic scattering cross section: nuclear + 419 1451 177 interference terms 419 1451 178 419 1451 179 Obtained by integrating the "nuclear-plus-interference" angular 419 1451 180 distributions of MF=6. Note that because of the interference 419 1451 181 effect, the tabulations in both MF=6 and MF=3 can be negative at 419 1451 182 some energies and angles. 419 1451 183 419 1451 184 - MT5 : (p,anything) cross section 419 1451 185 419 1451 186 MT5 contains the reactions which can not be stored in any other 419 1451 187 MT-number. As the incident energy increases, the cross section 419 1451 188 of MT5 increases as more reaction channels are no longer stored 419 1451 189 under a specific MT number. The information of MF3/MT5 can be 419 1451 190 combined with MF6/MT5 to obtain residual production cross 419 1451 191 sections particle production cross sections and 419 1451 192 (double-)differential cross sections. 419 1451 193 419 1451 194 ##### MF6: PRODUCT ENERGY-ANGLE DISTRIBUTIONS 419 1451 195 419 1451 196 In MF6 we store all secondary energy, angle, and energy-angle 419 1451 197 distributions, as well as all residual and photon production 419 1451 198 cross sections. All data are generated with TALYS. 419 1451 199 419 1451 200 - MT2 : Elastic scattering angular distribution: nuclear + 419 1451 201 interference terms 419 1451 202 419 1451 203 Relative angular distributions are tabulated on an angular grid. 419 1451 204 They are obtained by using the "nuclear-plus-interference" option 419 1451 205 in MF=6, which corresponds to LAW=5, LTP=12, and the appropriate 419 1451 206 integrated cross section is stored in MF=3. Note that because 419 1451 207 of the interference effect, the tabulations in both MF=6 and 419 1451 208 MF=3 can be negative at some energies and angles. 419 1451 209 419 1451 210 - MT5 : (p,anything) yields and energy-angle distributions 419 1451 211 419 1451 212 MT5 contains the production yields of particles and residual 419 1451 213 products. It also contains the secondary energy-angle 419 1451 214 distributions for all particles and photons. First, the yields 419 1451 215 for neutrons are given for the whole energy range. Next, on a 419 1451 216 secondary energy grid the relative emission spectra are given 419 1451 217 together with the parameters for the Kalbach systematics for 419 1451 218 angular distributions. Inelastic scattering cross sections for 419 1451 219 discrete states have been broadened and added to the continuum 419 1451 220 spectra. This procedure is repeated for protons, deuterons, 419 1451 221 tritons, Helium-3, alpha particles and photons. Finally, the 419 1451 222 residual production yields are given per final product. All these 419 1451 223 yields and relative distributions can be multiplied with the 419 1451 224 cross sections given in MF3/MT5 to get the production cross 419 1451 225 sections and (double-)differential cross sections. 419 1451 226 419 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 **** 419 1451 228 419 1451 229 This file has been checked successfully by the BNL checking 419 1451 230 codes CHECKR-8.0, FIZCON-8.0 and PSYCHE-8.0 [her08] and has 419 1451 231 been processed successfully into an MCNP library by the 419 1451 232 processing code NJOY99.90 [mac00]. 419 1451 233 419 1451 234 *********************** R E F E R E N C E S ********************** 419 1451 235 419 1451 236 [akk85] J.M. Akkermans and H. Gruppelaar, Phys. Lett. 157B, 95 419 1451 237 (1985). 419 1451 238 [her08] M. Herman, ENDF Utility Codes Release 8.0, (2008). 419 1451 239 [kal88] C. Kalbach, Phys. Rev. C37, 2350 (1988). 419 1451 240 [kal05] C. Kalbach, Phys. Rev. C71, 034606 (2005). 419 1451 241 [kon03] A.J. Koning and J.P. Delaroche, Nucl. Phys. A713, 231 419 1451 242 (2003). 419 1451 243 [kon04] A.J. Koning and M.C. Duijvestijn, Nucl. Phys. A744, 15 419 1451 244 (2004). 419 1451 245 [kon07] A.J. Koning, S. Hilaire and M.C. Duijvestijn, TALYS-1.0, 419 1451 246 Proceedings of the International Conference on Nuclear 419 1451 247 Data for Science and Technology - ND-2007, 419 1451 248 April 22-27, 2007, Nice, France 419 1451 249 [kon08] A.J. Koning, S. Hilaire and S. Goriely, ``Global and 419 1451 250 local level density models'', Nucl Phys. A810, 419 1451 251 13-76 (2008). 419 1451 252 [mac00] R.E. Macfarlane, NJOY99 - Code system for producing 419 1451 253 pointwise and multigroup neutron and photon cross 419 1451 254 sections from ENDF/B Data, RSIC PSR-480 (2000). 419 1451 255 [ray94] J. Raynal, Notes on ECIS94, CEA Saclay Report 419 1451 256 No. CEA-N-2772, 1994. 419 1451 257 [rip09] R. Capote, M. Herman, P. Oblozinsky, P.G. Young, 419 1451 258 S. Goriely, T. Belgya, A.V. Ignatyuk, A.J. Koning, 419 1451 259 S. Hilaire, V. Plujko, M. Avrigeanu, O. Bersillon, 419 1451 260 M.B. Chadwick, T. Fukahori, S. Kailas, J. Kopecky, 419 1451 261 V.M. Maslov, G. Reffo, M. Sin, E. Soukhovitskii, 419 1451 262 P. Talou, H. Yinlu, and G. Zhigang, 419 1451 263 RIPL - Reference Input Parameter Library for calculation 419 1451 264 of nuclear reactions and nuclear data evaluation, 419 1451 265 Nucl. Data Sheets 110, 3107 (2009). 419 1451 266 419 1451 267 ************************* C O N T E N T S ************************ 419 1451 268 419 1451 269 *************** PROGRAM ACTIVATE (VERSION 2010-1) *************** 419 1451 270 MF=10 Activation Cross Sections Defined by Combining MF=3 419 1451 271 Cross Sections and MF=9 Multipliers. MF=9 Deleted. 419 1451 272 1 451 275 1 419 1451 273 3 2 18 1 419 1451 274 3 5 18 1 419 1451 275 6 2 1401 1 419 1451 276 6 5 11466 1 419 1451 277 8 5 13 1 419 1451 278 419 1 0 279 419 0 0 280 4007.00000 6.95665100 0 0 0 0 419 3 2 281 0.000000+0 0.000000+0 0 0 1 45 419 3 2 282 45 2 419 3 2 283 1.000000+6-1.098334-1 2.000000+6-3.108258-1 3.000000+6-2.753844-1 419 3 2 284 4.000000+6-2.082957-1 5.000000+6-1.518511-1 6.000000+6-1.092995-1 419 3 2 285 7.000000+6-7.710885-2 8.000000+6-5.248550-2 9.000000+6-3.348646-2 419 3 2 286 1.000000+7-1.860396-2 1.100000+7-6.726824-3 1.200000+7 2.888962-3 419 3 2 287 1.300000+7 1.073450-2 1.400000+7 1.716438-2 1.500000+7 2.246415-2 419 3 2 288 1.600000+7 2.686588-2 1.700000+7 3.056099-2 1.800000+7 3.369462-2 419 3 2 289 1.900000+7 3.637440-2 2.000000+7 3.867889-2 2.200000+7 4.239025-2 419 3 2 290 2.400000+7 4.519276-2 2.600000+7 4.735509-2 2.800000+7 4.907543-2 419 3 2 291 3.000000+7 5.048279-2 3.500000+7 5.313625-2 4.000000+7 5.507913-2 419 3 2 292 4.500000+7 5.666695-2 5.000000+7 5.804618-2 5.500000+7 5.926323-2 419 3 2 293 6.000000+7 6.032794-2 6.500000+7 6.123222-2 7.000000+7 6.196111-2 419 3 2 294 7.500000+7 6.250037-2 8.000000+7 6.283726-2 9.000000+7 6.287129-2 419 3 2 295 1.000000+8 6.203671-2 1.100000+8 6.035814-2 1.200000+8 5.789899-2 419 3 2 296 1.300000+8 5.476133-2 1.400000+8 5.101519-2 1.500000+8 4.689775-2 419 3 2 297 1.600000+8 4.239491-2 1.800000+8 3.285896-2 2.000000+8 2.508831-2 419 3 2 298 419 3 0 299 4.007000+3 6.956651+0 0 0 0 0 419 3 5 300 0.000000+0 0.000000+0 0 0 1 45 419 3 5 301 45 2 419 3 5 302 1.000000+6 5.198700-1 2.000000+6 7.961800-1 3.000000+6 8.722900-1 419 3 5 303 4.000000+6 8.911501-1 5.000000+6 9.145800-1 6.000000+6 9.355600-1 419 3 5 304 7.000000+6 9.433700-1 8.000000+6 9.424200-1 9.000000+6 9.373701-1 419 3 5 305 1.000000+7 9.309200-1 1.100000+7 9.236200-1 1.200000+7 9.154400-1 419 3 5 306 1.300000+7 9.066501-1 1.400000+7 8.975801-1 1.500000+7 8.885301-1 419 3 5 307 1.600000+7 8.797200-1 1.700000+7 8.831700-1 1.800000+7 8.741201-1 419 3 5 308 1.900000+7 8.654001-1 2.000000+7 8.570901-1 2.200000+7 8.412200-1 419 3 5 309 2.400000+7 8.282701-1 2.600000+7 8.159900-1 2.800000+7 8.031300-1 419 3 5 310 3.000000+7 7.911100-1 3.500000+7 7.637600-1 4.000000+7 7.394300-1 419 3 5 311 4.500000+7 7.176901-1 5.000000+7 6.979700-1 5.500000+7 6.798401-1 419 3 5 312 6.000000+7 6.630000-1 6.500000+7 6.472400-1 7.000000+7 6.323500-1 419 3 5 313 7.500000+7 6.181901-1 8.000000+7 6.046501-1 9.000000+7 5.790400-1 419 3 5 314 1.000000+8 5.549200-1 1.100000+8 5.318700-1 1.200000+8 5.095800-1 419 3 5 315 1.300000+8 4.878100-1 1.400000+8 4.667400-1 1.500000+8 4.456300-1 419 3 5 316 1.600000+8 4.265000-1 1.800000+8 4.089200-1 2.000000+8 3.931400-1 419 3 5 317 419 3 0 318 419 0 0 319 4007.00000 6.95665100 0 0 13 0 41910 5 320 0.0 0.0 1 0 1 45 41910 5 321 45 2 41910 5 322 1.000000+6 0.0 2.000000+6 0.0 3.000000+6 .014203673 41910 5 323 4.000000+6 .026322881 5.000000+6 .065824975 6.000000+6 .128173591 41910 5 324 7.000000+6 .170566956 8.000000+6 .196957298 9.000000+6 .211137928 41910 5 325 1.000000+7 .215516358 1.100000+7 .215798271 1.200000+7 .214741169 41910 5 326 1.300000+7 .211927648 1.400000+7 .207791588 1.500000+7 .202919839 41910 5 327 1.600000+7 .197361663 1.700000+7 .146146972 1.800000+7 .154143213 41910 5 328 1.900000+7 .160892590 2.000000+7 .167783101 2.200000+7 .182591848 41910 5 329 2.400000+7 .174183545 2.600000+7 .172780171 2.800000+7 .181324266 41910 5 330 3.000000+7 .190307839 3.500000+7 .213068418 4.000000+7 .241810617 41910 5 331 4.500000+7 .251893436 5.000000+7 .249820912 5.500000+7 .256123639 41910 5 332 6.000000+7 .269553258 6.500000+7 .291423046 7.000000+7 .293417356 41910 5 333 7.500000+7 .297262273 8.000000+7 .315362515 9.000000+7 .329476655 41910 5 334 1.000000+8 .359087067 1.100000+8 .373135526 1.200000+8 .381634144 41910 5 335 1.300000+8 .385303558 1.400000+8 .377019970 1.500000+8 .371525296 41910 5 336 1.600000+8 .371090400 1.800000+8 .368521975 2.000000+8 .377985239 41910 5 337 0.0 0.0 1001 0 1 45 41910 5 338 45 2 41910 5 339 1.000000+6 0.0 2.000000+6 .340612970 3.000000+6 .354648690 41910 5 340 4.000000+6 .362608085 5.000000+6 .511413930 6.000000+6 .693193826 41910 5 341 7.000000+6 .796431632 8.000000+6 .852837324 9.000000+6 .884872688 41910 5 342 1.000000+7 .899559167 1.100000+7 .906008414 1.200000+7 .910738300 41910 5 343 1.300000+7 .910947621 1.400000+7 .906376385 1.500000+7 .899423479 41910 5 344 1.600000+7 .890795675 1.700000+7 .679504816 1.800000+7 .677868774 41910 5 345 1.900000+7 .671268357 2.000000+7 .670777568 2.200000+7 .661592611 41910 5 346 2.400000+7 .539014161 2.600000+7 .513614298 2.800000+7 .495262965 41910 5 347 3.000000+7 .480441894 3.500000+7 .458185734 4.000000+7 .465119956 41910 5 348 4.500000+7 .458644165 5.000000+7 .438636455 5.500000+7 .435889678 41910 5 349 6.000000+7 .436168473 6.500000+7 .446690097 7.000000+7 .432679164 41910 5 350 7.500000+7 .424051826 8.000000+7 .429919523 9.000000+7 .422938344 41910 5 351 1.000000+8 .436856886 1.100000+8 .439118786 1.200000+8 .438838576 41910 5 352 1.300000+8 .435754331 1.400000+8 .422029108 1.500000+8 .417194350 41910 5 353 1.600000+8 .421758600 1.800000+8 .420443366 2.000000+8 .433672734 41910 5 354 0.0 0.0 1002 0 1 45 41910 5 355 45 2 41910 5 356 1.000000+6 0.0 2.000000+6 .030861370 3.000000+6 .048465654 41910 5 357 4.000000+6 .055768530 5.000000+6 .047075079 6.000000+6 .034543401 41910 5 358 7.000000+6 .040101998 8.000000+6 .049198848 9.000000+6 .053427284 41910 5 359 1.000000+7 .062130346 1.100000+7 .073181738 1.200000+7 .081770763 41910 5 360 1.300000+7 .091014977 1.400000+7 .101453479 1.500000+7 .111452773 41910 5 361 1.600000+7 .121023960 1.700000+7 .072765524 1.800000+7 .081870351 41910 5 362 1.900000+7 .090250846 2.000000+7 .098543934 2.200000+7 .111254710 41910 5 363 2.400000+7 .112831094 2.600000+7 .139823966 2.800000+7 .167798754 41910 5 364 3.000000+7 .191606051 3.500000+7 .242197461 4.000000+7 .260903439 41910 5 365 4.500000+7 .265483616 5.000000+7 .267723145 5.500000+7 .259727471 41910 5 366 6.000000+7 .250618641 6.500000+7 .241440584 7.000000+7 .238054481 41910 5 367 7.500000+7 .228489243 8.000000+7 .225059837 9.000000+7 .206843511 41910 5 368 1.000000+8 .192416290 1.100000+8 .177450979 1.200000+8 .163042159 41910 5 369 1.300000+8 .148847417 1.400000+8 .136125188 1.500000+8 .125302243 41910 5 370 1.600000+8 .115838253 1.800000+8 .108696252 2.000000+8 .099817067 41910 5 371 0.0 0.0 1003 0 1 45 41910 5 372 45 2 41910 5 373 1.000000+6 0.0 2.000000+6 0.0 3.000000+6 0.0 41910 5 374 4.000000+6 0.0 5.000000+6 0.0 6.000000+6 1.06558E-5 41910 5 375 7.000000+6 8.61464E-4 8.000000+6 .001938614 9.000000+6 .007758041 41910 5 376 1.000000+7 .016372369 1.100000+7 .024161714 1.200000+7 .030505299 41910 5 377 1.300000+7 .035615120 1.400000+7 .039811806 1.500000+7 .043440947 41910 5 378 1.600000+7 .046727383 1.700000+7 .076558828 1.800000+7 .078026495 41910 5 379 1.900000+7 .075191932 2.000000+7 .075333934 2.200000+7 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