TENDL-2011 gen. purp. file: deuteron + 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 1.99626000 200000000. 1 0 10020 0 528 1451 3 0.0 0.0 1 0 271 6 528 1451 4 5-B - 11 NRG EVAL-NOV11 A.J. Koning 528 1451 5 TENDL-2011 DIST- REV1- 528 1451 6 ----TENDL-2011 Material 528 REVISION 1 528 1451 7 -----Incident deuteron 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 14060 1 528 1451 280 8 5 27 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 49 528 3 2 285 49 1 528 3 2 286 13000000.0-.001082940 14000000.0 .007830312 15000000.0 .015163036 528 3 2 287 16000000.0 .021196961 17000000.0 .026178877 18000000.0 .030321851 528 3 2 288 19000000.0 .033800222 20000000.0 .037876776 22000000.0 .042249920 528 3 2 289 24000000.0 .045486843 26000000.0 .047945169 28000000.0 .049901578 528 3 2 290 30000000.0 .052588212 35000000.0 .056038905 40000000.0 .059152683 528 3 2 291 45000000.0 .062120334 50000000.0 .064669344 54000000.0 .066040124 528 3 2 292 55000000.0 .067513046 60000000.0 .070676040 70000000.0 .073562565 528 3 2 293 80000000.0 .074487530 90000000.0 .073737618 100000000. .069551601 528 3 2 294 120000000. .060253303 140000000. .048993951 160000000. .038278297 528 3 2 295 180000000. .029553644 200000000. .025799780 240000000. .025799780 528 3 2 296 280000000. .025799780 320000000. .025799780 360000000. .025799780 528 3 2 297 400000000. .025799780 440000000. .025799780 480000000. .025799780 528 3 2 298 520000000. .025799780 560000000. .025799780 600000000. .025799780 528 3 2 299 640000000. .025799780 680000000. .025799780 720000000. .025799780 528 3 2 300 760000000. .025799780 800000000. .025799780 840000000. .025799780 528 3 2 301 880000000. .025799780 920000000. .025799780 960000000. .025799780 528 3 2 302 1.00000E+9 0.0 528 3 2 303 528 3 0 304 5011.00000 10.9147300 0 0 0 0 528 3 5 305 0.0 0.0 0 0 1 106 528 3 5 306 106 1 528 3 5 307 1000000.00 .441063275 1125000.00 .496963560 1250000.00 .552852818 528 3 5 308 1375000.00 .608733934 1500000.00 .664608864 1625000.00 .720478986 528 3 5 309 1750000.00 .776345295 1875000.00 .832208532 2000000.00 .869281625 528 3 5 310 2125000.00 .887170527 2250000.00 .905058871 2375000.00 .922946742 528 3 5 311 2500000.00 .940834209 2625000.00 .958721329 2750000.00 .976608149 528 3 5 312 2875000.00 .994494706 3000000.00 1.00602024 3125000.00 1.01109591 528 3 5 313 3250000.00 1.01617154 3375000.00 1.02124712 3500000.00 1.02632266 528 3 5 314 3625000.00 1.03139816 3750000.00 1.03647363 3875000.00 1.04154907 528 3 5 315 4000000.00 1.04583577 4200000.00 1.04933643 4400000.00 1.05283704 528 3 5 316 4600000.00 1.05633759 4800000.00 1.05983809 5000000.00 1.06193778 528 3 5 317 5200000.00 1.06261786 5400000.00 1.06329794 5600000.00 1.06397801 528 3 5 318 5800000.00 1.06465808 6000000.00 1.06441322 6200000.00 1.06323312 528 3 5 319 6400000.00 1.06205303 6600000.00 1.06087294 6800000.00 1.05969285 528 3 5 320 7000000.00 1.05815446 7200000.00 1.05625434 7400000.00 1.05435422 528 3 5 321 7600000.00 1.05245411 7800000.00 1.05055401 8000000.00 1.04848461 528 3 5 322 8200000.00 1.04624450 8400000.00 1.04400439 8600000.00 1.04176429 528 3 5 323 8800000.00 1.03952419 9000000.00 1.03721436 9200000.00 1.03483427 528 3 5 324 9400000.00 1.03245418 9600000.00 1.03007409 9800000.00 1.02769401 528 3 5 325 10000000.0 1.02074291 11000000.0 1.01204060 12000000.0 1.00392635 528 3 5 326 13000000.0 .993161927 14000000.0 .982292713 15000000.0 .971408454 528 3 5 327 16000000.0 .960633953 17000000.0 .950183679 18000000.0 .940233663 528 3 5 328 19000000.0 .930779458 20000000.0 .918060288 22000000.0 .901136441 528 3 5 329 24000000.0 .884085914 26000000.0 .867729172 28000000.0 .852092327 528 3 5 330 30000000.0 .829936549 35000000.0 .802165327 40000000.0 .777937757 528 3 5 331 45000000.0 .756398253 50000000.0 .738812294 54000000.0 .729533621 528 3 5 332 55000000.0 .719411850 60000000.0 .696059055 70000000.0 .668026183 528 3 5 333 80000000.0 .643345311 90000000.0 .620799087 100000000. .592282857 528 3 5 334 120000000. .559640602 140000000. 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.626824012 2375000.00 .646987292 52810 5 352 2500000.00 .667150117 2625000.00 .687312551 2750000.00 .707474646 52810 5 353 2875000.00 .727636445 3000000.00 .742390536 3125000.00 .751661412 52810 5 354 3250000.00 .760932195 3375000.00 .770202895 3500000.00 .779473520 52810 5 355 3625000.00 .788744079 3750000.00 .798014577 3875000.00 .807285021 52810 5 356 4000000.00 .816181529 4200000.00 .824726947 4400000.00 .833272222 52810 5 357 4600000.00 .841817370 4800000.00 .850362409 5000000.00 .856869932 52810 5 358 5200000.00 .861312633 5400000.00 .865755295 5600000.00 .870197920 52810 5 359 5800000.00 .874640514 6000000.00 .877397665 6200000.00 .878450560 52810 5 360 6400000.00 .879503449 6600000.00 .880556334 6800000.00 .881609213 52810 5 361 7000000.00 .882037687 7200000.00 .881835783 7400000.00 .881633880 52810 5 362 7600000.00 .881431977 7800000.00 .881230075 8000000.00 .880965458 52810 5 363 8200000.00 .880637599 8400000.00 .880309742 8600000.00 .879981885 52810 5 364 8800000.00 .879654029 9000000.00 .878958314 9200000.00 .877892005 52810 5 365 9400000.00 .876825699 9600000.00 .875759394 9800000.00 .874693090 52810 5 366 10000000.0 .871642329 11000000.0 .867353553 12000000.0 .857915409 52810 5 367 13000000.0 .850617216 14000000.0 .848788130 15000000.0 .840859528 52810 5 368 16000000.0 .829350519 17000000.0 .817110448 18000000.0 .805047045 52810 5 369 19000000.0 .793865707 20000000.0 .786046858 22000000.0 .785365858 52810 5 370 24000000.0 .795765957 26000000.0 .801099272 28000000.0 .795844485 52810 5 371 30000000.0 .799132478 35000000.0 .827475473 40000000.0 .842061495 52810 5 372 45000000.0 .852089668 50000000.0 .878046055 54000000.0 .884966016 52810 5 373 55000000.0 .880121732 60000000.0 .891119441 70000000.0 .935476191 52810 5 374 80000000.0 .989041387 90000000.0 1.01315264 100000000. 1.02570596 52810 5 375 120000000. 1.05212007 140000000. 1.05578596 160000000. 1.04908690 52810 5 376 180000000. 1.04819061 200000000. 1.04767601 240000000. 1.04767601 52810 5 377 280000000. 1.04767601 320000000. 1.04767601 360000000. 1.04767601 52810 5 378 400000000. 1.04767601 440000000. 1.04767601 480000000. 1.04767601 52810 5 379 520000000. 1.04767601 560000000. 1.04767601 600000000. 1.04767601 52810 5 380 640000000. 1.04767601 680000000. 1.04767601 720000000. 1.04767601 52810 5 381 760000000. 1.04767601 800000000. 1.04767601 840000000. 1.04767601 52810 5 382 880000000. 1.04767601 920000000. 1.04767601 960000000. 1.04767601 52810 5 383 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 .001436786 1125000.00 .004370917 1250000.00 .007304469 52810 5 387 1375000.00 .010237593 1500000.00 .013170393 1625000.00 .016102940 52810 5 388 1750000.00 .019035287 1875000.00 .021967473 2000000.00 .023651803 52810 5 389 2125000.00 .024062102 2250000.00 .024472389 2375000.00 .024882664 52810 5 390 2500000.00 .025292930 2625000.00 .025703188 2750000.00 .026113440 52810 5 391 2875000.00 .026523685 3000000.00 .027577351 3125000.00 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