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68-Er-170 TIT EVAL-SEP00 A.K.M. HARUN-AR-RASHID+ DIST-JAN09 20090105 ----JEFF-311 MATERIAL 6849 -----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 2000-09 Evaluation was performed by A.K.M.Harun-ar-Rashid (tit), M.Igashira (tit), T.Ohsaki (tit), and K.Shibata (jaeri). 2001-02 Compiled by K.Shibata (jaeri). mf=1 General information mt=451 Descriptive data and dictionary mf=2 Resonance parameters mt=151 Resolved resonances Resonance range (1.0e-05 to 3.00e+03 eV). Resolved resonance parameters from Ref.1 (Ehi=3000.0 eV). The bound level at -336.0 eV has Gamma-n = 13.0645 eV and Gamma-gamma = 0.082 eV. This choice gives the desired value for the thermal capture cross section, 5.8+-0.3 b. Values of gamma-gamma not given in Ref.1 are set to 0.092 eV. 21 resonances [L=1] did not have values given for "J", 10 are assigned to J= 0.5 and the remaining 11 to J= 1.5 by random method. The value for the scattering radius is 8.0 fm, taken from Ref.2 with small change with in the given error, so as to produce the close value of the thermal neutron scattering cross section recommended by Mughabghab [2]. Highest energy resonance included is 2977.8 eV. No background cross sections are given. Calculated 2200-m/s cross sections and res. integrals 2200-m/s res. integ. elastic 11.967 b - capture 5.776 b 45.211 b total 17.743 b - mf=3 Neutron cross sections mt= 1 Total cross section Spherical optical model calculation was made by using casthy code [3]. Parameters are as follows, V = 48.2-0.25*E-16.0*(N-Z)/A , r0=1.18, a0=0.63 Ws = 7.84-0.51*E , rs=1.29, as=0.63 Vso= 6.0 , rso=1.26, aso=0.63 (energies in MeV, lengths in fm). mt= 2 Elastic scattering cross section The cross sections were obtained by subtracting a sum of reaction cross sections from the total cross sections. mt= 4,51,52,.,64,91 Inelastic scattering cross sections Calculated by using egnash code [4,5]. The direct-process component was considered for mt=51 from dwba calculation by dwucky code. [4,6] The level scheme is given as follows: no energy(MeV) spin parity g.s 0.00000 0.0 + 1 0.07870 2.0 + 2 0.26020 4.0 + 3 0.54080 6.0 + 4 0.89100 0.0 + 5 0.91230 8.0 + 6 0.93400 2.0 + 7 0.95990 2.0 + 8 1.01040 3.0 + 9 1.10330 4.0 + 10 1.12720 4.0 + 11 1.21740 3.0 + 12 1.23620 5.0 + 13 1.26640 1.0 - 14 1.26860 4.0 - Levels above 1.300 MeV are assumed to be overlapping mt= 16,17,22,28,32,103,104,105,107 (n,2n), (n,3n), (n,n'a), (n,n'p), (n,n'd) (n,p), (n,d), (n,t), (n,a) Calculated using egnash [4,5]. mt=102 Capture cross secton The capture cross section is based on the statistical model calculations. The measured data of Refs. 7 and 8 were taken into account. The direct and semidirect capture cross sections were added above 2 MeV by using the quick gnash code [5,9]. mf=4 Angular distributions of secondary neutrons mt=2 Calculated with the casthy code. mt=16,17,22,28,32, Assumed to be isotropic in the laboratory system. mt=51,---,64,91 Calculated with the casthy code. For mt=51, the dwba component was taken into account. mf=5 Energy distributions of secondary neutrons mt=16,17,22,28,32,91 Calculated with the egnash code. mf=12 Photon production multiplicities mt=16,17,22,28,51-64,91,102,103,104,107 Calculated with the egnash code. mf=14 Photon angular distributions mt=16,17,22,28,51-64,91,102,103,104,107 Assumed to be isotropic. mf=15 Photon energy distributions mt=16,17,22,28,91,102,103,104,107 Calculated with the egnash code. References 1. Landolt-Boernstein New Series I/16B (Aug 1998). 2. S. F. Mughabghab: "Neutron Cross Sections: Vol. 1, Neutron Resonance Parameters and Thermal Cross Sections, Part B: Z=61-100," Academic press (1984). 3. S. Igarasi, T. Fukahori: JAERI 1321 (1991). 4. N. Yamamuro: JAERI-M 90-006 (1990). 5. P.G. Young et al.: LA-12343-MS, UC-413 (1992). 6. P.D. Kunz: Program DWUCK4, Computational Nuclear Physics 2: Nuclear Reaction; edited by K. Langanke et al., published by Springer-Verlag (1992). 7. D.C. Stupegia et al.: JNE, 22, 267 (1968) . 8. M. Igashira et al.: Private communication (2002).Back |