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90-Th-230 NEA RCOM-JUN82 SCIENTIFIC CO-ORDINATION GROUP DIST-JAN09 20090105 ----JEFF-311 MATERIAL 9034 -----INCIDENT NEUTRON DATA ------ENDF-6 FORMAT *************************** JEFF-3.1.1 ************************* ** ** ** Original data taken from: JEFF-3.1 ** ** ** ****************************************************************** ***************************** JEFF-3.1 ************************* ** ** ** Original data taken from: JEFF-3.0 ** ** ** ****************************************************************** ***************************** JEFF-3.0 *********************** DATA TAKEN FROM :- JEF-2.2 (DIST-JAN92) Components of the energy released by fission (MT=458) updated by O. Serot et al. (JEF/DOC-887). Fission Q updated consistently. ****************************************************************** ****************************************************************** * JEF-2 * * DATA WERE TAKEN FROM ENDF/B-V(MAT=8030). * ****************************************************************** * 17-DEC-84: RADIOACTIVE DECAY DATA DELETED. * 26-DEC-84: Q-VALUE FOR MT=102 CORRECTED * 3-JAN-85: RESONANCE PARAM. CHANGED TO ORIGINAL SINGLE-LEVEL. * 31-MAR-88: CHANGE OF THE FLAG FROM SINGLE LEVEL TO MULTI LEVEL * BREIT-WIGNER RESONANCE PARAMETERS ****************************************************************** HEDL EVAL-NOV77 MANN DIST-DEC78 790307 MF=1 MT=452 NU. SYSTEMATICS. (REF. 5) MT=458 ENERGY OF FISSION. SYSTEMATICS OF SHER (REF. 6) MF=2 MT=151 RESONANCE PARAMETERS. RESOLVED PARAMETERS FROM BNL-325 (REF. 1), EXCEPT NEGATIVE ENERGY RESONANCE INCLUDED TO OBTAIN THERMAL CAPTURE CROSS SECTION (23.1 B VERUS 23.2 +-0.6 B IN BNL-325) AND THE NEUTRON WIDTH WAS REDUCED FOR THE FIRST RESONANCE TO OBTAIN BETTER AGREEMENT WITH CAPTURE RESONANCE INTEGRAL (1690 B VERUS 1010 B IN BNL-325). MF=3 MT=1 TOTAL. FROM OPTICAL MODEL MT=2 ELASTIC. DIFFERENCE OF TOTAL AND PARTIAL CROSS SECTIONS MT=4 INELASTIC. SUM OF 51,...,67,91. MT=16 (N,2N) MT=18 FISSION. BASED ON MUIR AND VESSER (REF. 2), LASL BOMB DATA. LOW ENERGY (.LT. 300 KEV) AND HIGH ENERGY (.GT. 3 MEV) FROM STATISTICAL MODEL CALCULATIONS (REF. 3). NOTE THAT DATA FROM LYNN ET AL (REF. 4) IS TWICE AS LARGE AS MUIR AND VESSER ABOVE 1.2 MEV ALTHOUGH ARE IN GOOD AGREEMENT BELOW. MT=51,...,67,91 INELASTIC. BASED ON STATISTICAL MODEL (REF. 3) MT=102 CAPTURE. BASED ON STATISTICAL MODEL (REF. 3) MT=251,252,253. DERIVED FROM MF=4,MT=1 MF=4 MT=2 ELASTIC BASED ON OPTICAL MODEL FOR POTENTIAL SCATTERING ONLY MT=16 (N,2N). ASSUMED ISOTROPIC MT=18 FISSION ASSUMED ISOTROPIC. MT=51,...,67,91 INELASTIC. ASSUMED ISOTROPIC MF=5 MT=16 (N,2N) SIMPLE EVAPORATION MODEL MT=18 FISSION. MAXWELLIAN WITH T=1.33 MEV MT=91 CONTINUUM INELASTIC SIMPLE EVAPORATION MODEL 90-TH-230 INEL EVAL-AUG78 REICH DATA ADDED TO THE FILE AT BNL BY R. KINSEY SEP78. REFERENCES 1. S.F. MUGHABGHAB AND D.I. GARBER, BNL-325,VOL. 1 (1973), BROOKHAVEN NATIONAL LABORATORY. 2. D.W. MUIR AND L.R. VESSER, LA-4648-MS (1971), LOS ALAMOS SCIENTIFIC LABORATORY. 3. F.M. MANN AND R.E. SCHENTER, HEDL-TME-MM-KJ (1977) HANFORD ENGINEERING DEVELOPMENT LABORATORY. 4. J.E. LYNN, G.D. JAMES, AND L.G. EARWARKER, NUCL. PHYS. A189 (1972) 225. 5. R.J. HOWERTON, NUCL. SCI. AND ENG. 62 (1977)438 6. R. SHER (PRIV. COMM., 1977)Back |