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94-Pu-238 MAPI,JAERI EVAL-MAR89 T.KAWAKITA, T.NAKAGAWA DIST-JAN09 20090105 ----JEFF-311 MATERIAL 9434 -----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 ** ** ** ****************************************************************** 05-01 NEA/OECD (Rugama) 8 delayed neutron groups Jefdoc-976 (Wilson and England, Prog Nucl Eng 41,71(2002) ***************************** JEFF-3.0 *********************** DATA TAKEN FROM :- JENDL-3.2 (DIST-SEP89 REV2-JUN94) Unresolved resonance parameters from BROND-2.2 ENDF/B-VI for MT=458 (fission energy) Fission Q value modified accordignly ****************************************************************** HISTORY 79-03 NEW EVALUATION WAS MADE BY T.KAWAKITA (PNC). 89-03 RE-EVALUATION WAS MADE BY T.KAWAKITA (MAPI) AND T.NAKAGAWA(JAERI). 94-06 JENDL-3.2. NU-P, NU-D AND NU-TOTAL WERE MODIFIED. COMPILED BY T.NAKAGAWA (NDC/JAERI) ***** MODIFIED PARTS FOR JENDL-3.2 ******************** (1,452), (1,455), (1,456) *********************************************************** ***** MODIFIED PARTS FOR JEFF-3.0 ******************** A. Nouri (Data Bank) June 1999 MF=1 MT=456 Number of propmt neutrons emitted by fission use the same representation as for MT=452 (ENDF-6 recommendation): convert LNU=1 (polynomial (linear) representation) used in JENDL-32 to tabular representation (LNU=2). MF=2 MT=151 Add unresolved resonance parameters from BROND-2.2 *********************************************************** MF=1 GENERAL INFORMATION MT=451 COMMENT AND DICTIONARY MT=452 NUMBER OF NEUTRONS PER FISSION SUM OF NU-P NAD NU-D. MT=455 DELAYED NEUTRONS PER FISSION AVERAGE VALUES OF SYSTEMATICS BY TUTTLE/1/, BENEDETTI ET AL./2/ AND WALDO ET AL./3/ DECAY CONSTANTS WERE EVALUATED BY BRADY AND ENGLAND/4/. MT=456 PROMPT NEUTRONS PER FISSION THE THERMAL VALUE OF PROMPT NEUTRONS WAS BASED ON EXPERI- MENTAL DATA OF JAFFEY AND LERNER /5/, KROSHKIN ET AL./6/ AND HADDAD AND ASGHER/7/. THE ENERGY DEPENDENT TERM WAS ESTIMATED FROM HOWRTON'S FORMULA /8/. MF=2 RESONANCE PARAMETERS MT=151 RESOLVED RESONANCE PARAMETERS FOR MLBW FORMULA. ENERGY RANGE IS FROM 1.0E-5 EV TO 500 EV. PARAMETERS WERE TAKEN FROM THE FOLLOWING EXPERIMENTAL DATA. 49 RESONANCES ABOVE 10 EV : SILBERT /9/ 4 RESONANCES BELOW 10 EV : YOUNG /10/ THE PARAMETERS OF TWO NEGATIVE AND 2.9-EV RESONANCES WERE ADJUSTED TO THE THERMAL CROSS SECTIONS/11/. CALCULATED 2200-M/S CROSS SECTIONS AND RESONANCE INTEGRALS 2200-M/S RES. INTEG. TOTAL 586.7 B - ELASTIC 28.53 B - FISSION 17.89 B 32.7 B CAPTURE 540.3 B 154 B MF=3 NEUTRON CROSS SECTIONS THE ENERGY REGION BELOW 500 EV IS THE RESONANCE REGION. ABOVE 500 EV, THE CROSS SECTIONS WERE EVALUATED AS FOLLOWS. MT=1,2,4,51-78,91,102 TOTAL, ELASTIC AND INELASTIC SCATTERING, AND CAPTURE CROSS SECTIONS CALCULATED WITH OPTICAL AND STATISTICAL MODELS. CASTHY/12/ WAS USED FOR THE CALCULATION. OPTICAL POTENTIAL PARAMETERS: THE REAL POTENTIAL WAS ADJUSTED SO AS TO OBTAINED THE REASONABLE COMPOUND NUCLEUS FORMATION CROSS SECTION. THE OTHER PARAMETERS WERE TAKEN FROM MURATA'S EVALUATION /13/. V = 38.8 - 0.05*EN (MEV) WS = 6.5 + 0.15*EN (MEV) VSO= 7.0 (MEV) A = B = ASO= 0.47 (FM) R = RSO= 1.32 (FM) RS = 1.52 (FM) THE LEVEL SCHEME: TAKEN FROM REF. /14/. NO. ENERGY(KEV) SPIN-PARITY G.S. 0.0 0 + 1 44.08 2 + 2 145.98 4 + 3 303.4 6 + 4 514.0 8 + 5 605.1 1 - 6 661.4 3 - 7 763.2 5 - 8 941.5 0 + 9 962.77 1 - 10 968.2 2 - 11 983.0 2 + 12 985.5 2 - 13 1028.55 2 + 14 1069.95 3 + 15 1082.57 4 - 16 1125.8 4 + 17 1174.5 2 + 18 1202.7 3 - 19 1228.6 0 + 20 1264.2 2 + 21 1310.3 2 + 22 1426.6 0 + 23 1447.3 1 - 24 1458.5 2 + 25 1560.0 1 - 26 1596.5 2 + 27 1621.4 1 - 28 1636.6 1 - CONTINUUM LEVELS ASSUMED ABOVE 1.65 MEV. THE LEVEL DENSITY PARAMETERS OF GILBERT AND CAMERON /15/. THE FISSION, (N,2N) AND (N,3N) CROSS SECTIONS WERE TAKEN INTO ACCOUNT AS THE COMPETING PROCESSES. FOR THE CAPTURE CROSS SECTION, THE GAMMA-RAY STRENGTH FUNCTION WAS ESTIMATED FROM D-OBS = 9.5EV AND AVERAGE RADIATIVE WIDTH = 0.04 EV. MT=16,17 (N,2N) AND (N,3N) REACTION CROSS SECTIONS CALCULATION BASED ON THE PEARLSTEIN'S METHOD /16/. MT=18 FISSION CROSS SECTION EVALUATED MAINLY ON THE BASIS OF DATA MEASURED BY BUDTZ-JORGENSEN/17/. OTHER EXPERIMENTS /9, 18, 19, 20, 21, 22, 23, 24, 25/ WERE ALSO TAKEN INTO CONSIDERATION. MT=251 MU-BAR CALCULATED WITH OPTICAL MODEL. MF=4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS MT=2,51-78,91 CALCULATED WITH OPTICAL MODEL. MT=16,17,18 ISOTROPIC IN THE LABORATORY SYSTEM. MF=5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS MT=16,17,91 EVAPORATION SPECTRUM WAS ASSUMED. MT=18 MAXWELLIAN TYPE FISSION SPECTRUM. TEMPERATURE WAS ESTIMATED FROM Z**2/A SYSTEMATICS BY SMITH ET AL. /26/. REFERENCES 1) R.J. TUTTLE: INDC(NDS)-107/G+SPECIAL, P.29 (1979), 2) G. BENEDETTI ET AL.: NUCL. SCI. ENG., 80, 379 (1982). 3) R. WALDO ET AL.: PHYS. REV., C23, 1113 (1981). 4) M.C. BRADY AND T.R. ENGLAND: NUCL. SCI. ENG., 103, 129 (1989). 5) A.H. JAFFEY AND J.L. LERNER: NUCL. PHYS., A145, 1 (1970). 6) N.I. KROSHKIN ET AL.: ATOMNAJA ENERGIJA, 29, 95 (1970). = EXFOR40064007. 7) M. HADDAD AND M. ASGHAR: 1988 MITO, P.979 (1988). 8) R.J. HOWERTON: NUCL. SCI. ENG., 62, 438 (1977). 9) M.G. SILBERT ET AL.: NUCL. SCI. ENG., 52, 176 (1973). 10) T.E. YOUNG ET AL.: NUCL. SCI. ENG., 30, 355 (1967). 11) MUGHABGHAB S.F.: "NEUTRON CROSS SECTIONS, VOL. 1, PART B", ACADEMIC PRESS (1984). 12) S. IGARASI AND T. FUKAHORI: JAERI 1321 (1991). 13) T. MURATA: PRIVATE COMMUNICATION. 14) C.M. LEDERER ET AL.: TABLE OF ISOTOPES, 7TH ED. (1978). 15) A. GILBERT AND A.G.W. CAMERON: CAN. J. PHYS., 43, 1446 (1965). 16) S. PEARLSTEIN: NUCL. SCI. ENG., 23, 238 (1965). 17) C. BUDTZ-JORGENSEN ET AL.: 1982 ANTWERP, 206 (1983). 18) D.M. BARTON AND P.G. KOONTY: PHYS. REV., 162, 1070 (1967). 19) E.F. FOMUSHKIN ET AL.: SOV. J. NUCL. PHYS., 5, 689 (1967). 20) S.B. ERMAGAMBETOV AND G.N. SHIRENKIN: SOV. J. NUCL. PHYS., 25, 1364 (1968). 21) D.M. DRAKE ET AL.: LA-4420, P.101 (1970). 22) S.B. ERMAGAMBETOV ET AL.: SOV. J. NUCL. ENERGY,29, 1190(1970). 23) E.F. FOMUSHKIN ET AL.: SOV. J. NUCL. PHYS., 10, 529 (1970). 24) D.L. SHPAK ET AL.: JETP LETTERS, 15, 228 (1972). 25) B. ALAM ET AL.: NUCL. SCI. ENG., 99, 267 (1988). 26) A.B. SMITH ET AL.: ANL/NDM-50 (1979).Back |