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74-W -183 KHI,NEDAC EVAL-MAR87 T.WATANABE(KHI), T.ASAMI(NEDAC) DIST-JAN09 20090105 ----JEFF-311 MATERIAL 7434 -----INCIDENT NEUTRON DATA ------ENDF-6 FORMAT *************************** JEFF-3.1.1 ************************* ** ** ** Original data taken from: JEFF-3.1 ** ** ** ****************************************************************** ***************************** JEFF-3.1 ************************* ** ** ** Original data taken from: JENDL-3.3 ** ** ** ****************************************************************** HISTORY 87-03 New evaluation was made for JENDL-3. 94-01 JENDL-3.2. Compiled by T.Nakagawa (ndc/jaeri) 00-03 Reevaluation was made by T.Asami. 01-11 Compiled by K.Shibata (ndc/jaeri) ***** modified parts for JENDL-3.3 from JENDL-3.2 ****** (3,2) (3,16,28) revised (3,203,207) added (3,251) deleted (4,2) transformation matrix deleted (4,16,17,22,28,91) deleted (5,16,17,22,28,91) deleted (6,16,17,22,28,91) taken from JENDL fusion file (6,203,204,207) taken from JENDL fusion file (12,22-107) evaluated newly (13,3) evaluated newly (14,3-107) isotropic distributions (15,3-107) evaluated newly *********************************************************** The JENDL fusion file /1/ and the modification of JENDL-3.2 from JENDL-3.1 as follows: ------------------------------------------------------------- JENDL fusion file /1/ (as of Jan. 1994) Evaluated by K.Kosako (nedac) and S.Chiba (ndc/jaeri) Compiled by K.Kosako. Data were taken from JENDL-3.1 except for the following: - The inelastic scattering cross sections to cotinuum (mt=91) was calculated with casthy2y and dwucky in sincros-ii system/2/ including contributions from direct reactions. - The (n,2n), (n,3n), (n,na), (n,np), (n,p), (n,d) and (n,a) reaction cross sections (mt=16, 17, 22, 28, 103, 104, 107) were calculated by egnash2 in the sincros-ii. - Energy distributions of secondary neutrons were replaced by those calculated by egnash2. The ddx's of the continuum neutrons were calculated by Kumabe's systema- tics /3/ using f15tob /1/. The precompound/compound ratio was calculated by the sincros- ii code system. - Optical-model, level density and other parameters used in the sincros-ii calculation are described in ref./2/. Level schemes were determined on the basis of ENSDF/4/. ------------------------------------------------------------- mf=1 General information mt=451 Descriptive data and dictionary mf=2 Resonance parameters mt=151 Resolved resonance parameters Resolved parameters for MLBW formula were given in the energy region from 1.0e-5 eV to 2.2 keV. Parameters were evaluated by examining both the experimental data/5,6,7/ and the recommended data of BNL/8/. For unknown radiative width, an average value of 55 milli-ev was assumed. Parameters for a negative resonance were selected so that the 2200 m/s cross section for capture reproduced gave a recommended value of 10.2 barns/8/ and gave a good fit to the experimental data for total cross sections around thermal energies. The scattering radius was assumed to be 7.3 fm. Calculated 2200 m/sec cross sections and resonance integrals are as follows: 2200 m/s cross section(b) res. integral(b) elastic 2.38 capture 10.11 335. total 12.49 mf=3 Neutron cross sections Below 2.2 keV, zero background cross section was given and all the cross-section data are reproduced from the evaluated resonance parameters with MLBW formula. For JENDL-3.1, above 2.2 keV, the total and partial cross sections were given mainly based on the theoretical calcula- tions. the total, elastic and inelastic scattering, and capture cross sections were calculated with the coupled-channel model and the spherical optical-statistical model. The calculations were performed with a combined program of casthy/9/ and ecis /10/. the spherical optical potential parameters used are: V = 48.83 - 0.0809*En, Vso = 5.6 (MeV) Ws = 6.73 - 0.0536*En, Wv = 0 (MeV) r = 1.168, rs = 1.268, rso = 1.592 (fm) a = 0.617, aso = 0.664, b = 0.563 (fm) The deformed potential parameters were taken from the work of Delaroche/11/. mt=1 Total Calculated with the combined program of the ecis and casthy codes. Almost the same as JENDL-3.1. mt=2 Elastic scattering Obtained by subtracting the sum of the partial cross sections from the total cross section. mt=4, 51-60, 91 Inelastic scattering The data of mt=51 to 60 were calculated with the combined program of casthy /9/ and ecis/10/. These cross sections are the same as JENDL-3.1 except that new calculation was made at additional several energy points. The cross section of mt=91 was calculated with sincros-ii for JENDL fusion file. The level scheme was based on ref./4/ Contributions of the direct process were calculated for the levels marked with '*'. no. mt energy(MeV) spin-parity (direct process) g.s. 0.0 1/2 - 1 51 0.0465 3/2 - * 2 52 0.0991 5/2 - * 3 53 0.2070 7/2 - * 4 54 0.2088 3/2 - 5 55 0.2917 5/2 - 6 56 0.3089 9/2 - * 7 57 0.3095 11/2 + 8 58 0.4121 7/2 - 9 58 0.4530 7/2 - 10 59 0.4870 13/2 + 11 59 0.5330 1/2 + 12 60 0.5500 9/2 - 13 60 0.5953 9/2 - 14 60 0.6228 9/2 + Levels above 0.624 MeV were assumed to be overlapping. Data of levels 8-9, 10-11 and 12-14 were lumped as is indicated in the above table. The direct inelastic scattering cross section was calculated also for the levels at 0.904, 0.935, 1.025, 1.485, 1.866, 2.127, 2.505, 2.912, 3.404, 4.0, 4.5, 5.0 and 5.5 MeV, and added to mt=91. Finally, the data for mt=51,52,54,55,57,58 and 91 were adjusted to reproduce the benchmark integral data/16/. mt=16, 28 (n,2n), (n,np) calculated with the scincros-ii system/2/. mt=17, 22, 103, 104, 107 (n,3n), (n,na), (n,p), (n,d), (n,a) Theoretical calculation was made with sincros-ii. The results were normalized to (n,p) 0.0041 b at 14.7 MeV measured by Qaim/17/, (n,d)+(n,np) 0.0013 b at 14.7 MeV measured by Qaim/17/, (n,a) 0.0018 b at 14.7 MeV (systematics of Qaim/17/). mt=102 capture Calculated with the casthy code/9/ and normalized to 70+-9 mb at 500 kev/18/. Above 3 MeV, a straight line in log-log scale was adopted assuming 1.0 mb at 14 MeV for JENDL-3.2. mt=203 Total proton production Sum of mt=28 and 103. mt=204 Total deuteron production Equal to mt=104. mt=207 : total alpha production Sum of mt=22 and 107. mf=4 Angular distributions of secondary neutrons (mt=2, 51-60: the same as JENDL-3.1) mt=2 Calculated with the casthy code/9/. mt=51-60 Calculated with the combined program of casthy/9/ and ecis/10/ codes. mf=6 Energy-angle distributions of secondary particles mt=16, 17, 22, 28, 91 Based on Kumabe's systematics/1,3/. mt=203,204,207 Based on Kalbach's systematics/1,19/. mf=12 Photon production multiplicities and transition probability arrays mt=22, 51-60,102,103,107 Below 627.44 keV, given as multiplicities Calculated with the egnash code/2/ and processed by the gamfil2 code/20/. mt=102 was calculated with the casthy code/10/. mf=13 Photon production cross sections mt=3 Calculated with the egnash code/2/ and processed by the gamfil2 code/20/. mf=14 Photon angular distributions mt=3, 22, 51-60, 102, 103, 107 Assumed to be isotropic distributions mf=15 Continuous photon energy spectra mt=3, 22, 103, 107 Calculated with the egnash code/2/. mt=102 Calculated with the casthy code/10/. References 1) Chiba, S. et al.: JAERI-M 92-027, p.35 (1992). 2) Yamamuro, N.: JAERI-M 90-006 (1990). 3) Kumabe, I. et al.: Nucl. Sci. Eng., 104, 280 (1990). 4) ENSDF: Evaluated Nuclear Structure Data File, BNL/NNDC. 5) Camarda H.S. et al. : Phys. Rev. C8, 1813 (1973). 6) Ohkubo M. : JAERI-M 5624 (1974). 7) Macklin R.L. et al. : LA-9200-MS (1982). 8) Mughabghab S.f. :"Neutron Cross Sections", Vol. 1, part B (1984). 9) Igarasi S. and Fukahori T.: JAREI 1321 (1991). 10) Raynal J. : IAEA-SMR-9/8 p.281 (1972). 11) Delaroche J.F. et al. : 1979 Knoxville Conf. 336 (1979). 12) Perey F.G.: Phys. Rev., 131, 745 (1963). 13) Arthur, E.D. and Young, P.G.: LA-8626-MS (1980). 14) Lohr J.M. and Haeberli W.: Nucl. Phys., A232, 381 (1974). 15) Becchetti F.D. Jr. and Greenlees G.W.: "Polarization Phenomena in Nucl. Reactions," Univ. Wisconsin Press, p.682 (1971). 16) Oyama, Y. et al.: JAERI-CONF 96-005, 70(1996). 17) Qaim,S.M. and Graca, C.: Nucl. Phys., A242, 317 (1975). 18) Voignier J. et al.: Nucl. Sci. Eng., 93, 43 (1986). 19) Kalbach C. : Phys. Rev. C37, 2350(1988). 20) Hida K.: JAERI-M 86-150 (1986) (in Japanese).Back |