60-Nd-150
60-ND-150 JNDC EVAL-MAR90 JNDC FP NUCLEAR DATA W.G.
DIST-MAR02 REV3-FEB02 20020222
----JENDL-3.3 MATERIAL 6049
-----INCIDENT NEUTRON DATA
------ENDF-6 FORMAT
===========================================================
JENDL-3.2 data were automatically transformed to JENDL-3.3.
Interpolation of spectra: 22 (unit base interpolation)
(3,251) deleted, T-matrix of (4,2) deleted, and others.
===========================================================
HISTORY
84-10 EVALUATION FOR JENDL-2 WAS MADE BY JNDC FPND W.G./1/
90-03 MODIFICATION FOR JENDL-3 WAS MADE/2/.
93-10 MODIFICATION FOR JENDL-3.2 WAS MADE.
CONTRIBUTION OF THE DIRECT INELASTIC SCATTERING WAS
REPLACED BY A COUPLED-CHANNEL CALCULATION.
**** MODIFIED PARTS FOR JENDL-3.2 ********************************
(3,2),(3,4),(3,51),(3,52),(3,54),(3,56),(3,58)
(4,51),(4,52),(4,54),(4,56),(4,58)
******************************************************************
MF = 1 GENERAL INFORMATION
MT=451 COMMENTS AND DICTIONARY
MF = 2 RESONANCE PARAMETERS
MT=151 RESOLVED AND UNRESOLVED RESONANCE PARAMETERS
RESOLVED RESONANCE PARAMETERS FOR MLBW FORMULA (BELOW 13.69 KEV)
RESONANCE PARAMETERS WERE TAKEN FROM JENDL-2/3/.
NEUTRON WIDTHS WERE ADOPTED FROM TELLIER/4/. RADIATION
WIDTHS WERE TAKEN FROM THE RECOMMENDATION BY MAGHABGHAB AND
GARBER/5/. THE AVERAGE RADIATION WIDTH OF 0.070 EV WAS ASSUMED
FOR LEVELS WHICH HAD NO MEASURED RADIATION WIDTH. A NEGATIVE
RESONANCE WAS ADDED SO AS TO REPRODUCE THE CAPTURE CROSS
SECTION OF 1.2+-0.2 BARNS AT 0.0253 EV /6/.
UNRESOLVED RESONANCE REGION : 13.69 KEV - 100 KEV
UNRESOLVED RESONANCE PARAMETERS WERE ADOPTED FROM JENDL-2.
THE NEUTRON STRENGTH FUNCTIONS, S0, S1 AND S2 WERE CALCULATED
WITH OPTICAL MODEL CODE CASTHY/7/. THE OBSERVED LEVEL SPACING
WAS DETERMINED TO REPRODUCE THE CAPTURE CROSS SECTION
CALCULATED WITH CASTHY. THE EFFECTIVE SCATTERING RADIUS WAS
OBTAINED FROM FITTING TO THE CALCULATED TOTAL CROSS SECTION AT
100 KEV.
TYPICAL VALUES OF THE PARAMETERS AT 70 KEV:
S0 = 2.600E-4, S1 = 0.667E-4, S2 = 3.500E-4, SG = 3.39E-4,
GG = 0.037 EV, R = 7.993 FM.
CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS (BARNS)
2200 M/S RES. INTEG.
TOTAL 5.982 -
ELASTIC 4.780 -
CAPTURE 1.202 15.9
MF = 3 NEUTRON CROSS SECTIONS
BELOW 100 KEV, RESONANCE PARAMETERS WERE GIVEN.
ABOVE 100 KEV, THE SPHERICAL OPTICAL AND STATISTICAL MODEL
CALCULATION WAS PERFORMED WITH CASTHY, BY TAKING ACCOUNT OF
COMPETING REACTIONS, OF WHICH CROSS SECTIONS WERE CALCULATED
WITH PEGASUS/8/ STANDING ON A PREEQUILIBRIUM AND MULTI-STEP
EVAPORATION MODEL. THE OMP'S FOR NEUTRON GIVEN IN TABLE 1 WERE
DETERMINED BY IIJIMA AND KAWAI/9/ TO REPRODUCE A SYSTEMATIC
TREND OF THE TOTAL CROSS SECTION. THE OMP'S FOR CHARGED
PARTICLES ARE AS FOLLOWS:
PROTON = PEREY/10/
ALPHA = HUIZENGA AND IGO/11/
DEUTERON = LOHR AND HAEBERLI/12/
HELIUM-3 AND TRITON = BECCHETTI AND GREENLEES/13/
PARAMETERS FOR THE COMPOSITE LEVEL DENSITY FORMULA OF GILBERT
AND CAMERON/14/ WERE EVALUATED BY IIJIMA ET AL./15/ MORE
EXTENSIVE DETERMINATION AND MODIFICATION WERE MADE IN THE
PRESENT WORK. TABLE 2 SHOWS THE LEVEL DENSITY PARAMETERS USED
IN THE PRESENT CALCULATION. ENERGY DEPENDENCE OF SPIN CUT-OFF
PARAMETER IN THE ENERGY RANGE BELOW E-JOINT IS DUE TO GRUPPELAAR
/16/.
MT = 1 TOTAL
SPHERICAL OPTICAL MODEL CALCULATION WAS ADOPTED.
MT = 2 ELASTIC SCATTERING
CALCULATED AS (TOTAL - SUM OF PARTIAL CROSS SECTIONS).
MT = 4, 51 - 91 INELASTIC SCATTERING
SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WAS
ADOPTED. THE LEVEL SCHEME WAS TAKEN FROM REF./17/.
NO. ENERGY(MEV) SPIN-PARITY CC CAL.
GR. 0.0 0 +
1 0.1301 2 + *
2 0.3815 4 + *
3 0.6767 0 +
4 0.7212 6 + *
5 0.8514 2 +
6 0.9300 3 - *
7 1.0624 2 +
8 1.1307 8 + *
9 1.1386 4 +
10 1.3535 4 +
LEVELS ABOVE 1.45 MEV WERE ASSUMED TO BE OVERLAPPING.
FOR THE LEVELS WITH AN ASTERISK, THE CONTRIBUTION OF DIRECT
INELASTIC SCATTERING CROSS SECTIONS WAS CALCULATED BY THE
ECIS-88 CODE/18/. DEFORMATION PARAMETERS (BETA2 = 0.2848 AND
BETA3 = 0.070) WERE BASED ON THE DATA COMPILED BY RAMAN ET
AL./19/ AND SPEAR/20/, RESPECTIVELY. THE COUPLING OF G.S.
ROTATIONAL BAND (0+,2+,4+,6+,8+,10+) AND OCTUPOLE VIBRATIONAL
BAND (1-,3-,5-) WAS CONSIDERED. IN THE CC CALCULATION, THE
IMAGINARY SURFACE STRENGTH WAS REDUVED TO 7.35 MEV.
MT = 102 CAPTURE
SPHERICAL OPTICAL AND STATISTICAL MODEL CALCULATION WITH
CASTHY WAS ADOPTED. DIRECT AND SEMI-DIRECT CAPTURE CROSS
SECTIONS WERE ESTIMATED ACCORDING TO THE PROCEDURE OF BENZI
AND REFFO/21/ AND NORMALIZED TO 1 MILLI-BARN AT 14 MEV.
THE GAMMA-RAY STRENGTH FUNCTION (3.01E-04) WAS ADJUSTED TO
REPRODUCE THE CAPTURE CROSS SECTION OF 153 MILLI-BARNS AT 30
KEV MEASURED BY KONONOV ET AL./22/
MT = 16 (N,2N) CROSS SECTION
MT = 17 (N,3N) CROSS SECTION
MT = 22 (N,N'A) CROSS SECTION
MT = 28 (N,N'P) CROSS SECTION
MT = 32 (N,N'D) CROSS SECTION
MT = 33 (N,N'T) CROSS SECTION
MT =103 (N,P) CROSS SECTION
MT =104 (N,D) CROSS SECTION
MT =105 (N,T) CROSS SECTION
MT =107 (N,ALPHA) CROSS SECTION
THESE REACTION CROSS SECTIONS WERE CALCULATED WITH THE
PREEQUILIBRIUM AND MULTI-STEP EVAPORATION MODEL CODE PEGASUS.
THE KALBACH'S CONSTANT K (= 10.0) WAS DETERMINED TO REPRODUCE
ENERGY DEPENDENCE OF THE (N,2N) CROSS SECTION MEASURED BY
FREHAUT ET AL./23/
FINALLY, THE (N,P) CROSS SECTION WAS NORMALIZED TO THE
FOLLOWING VALUE AT 14.5 MEV:
(N,P) 1.61 MB (SYSTEMATICS OF FORREST/24/)
THE (N,2N) CROSS SECTION WAS DETERMINED BY EYE-GUIDING OF
THE DATA MEASURED BY FREHAUT ET AL./23/
MT = 251 MU-BAR
CALCULATED WITH CASTHY.
MF = 4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS
LEGENDRE POLYNOMIAL COEFFICIENTS FOR ANGULAR DISTRIBUTIONS ARE
GIVEN IN THE CENTER-OF-MASS SYSTEM FOR MT=2 AND DISCRETE INELAS-
TIC LEVELS, AND IN THE LABORATORY SYSTEM FOR MT=91. THEY WERE
CALCULATED WITH CASTHY. CONTRIBUTION OF DIRECT INELASTIC
SCATTERING WAS CALCULATED WITH ECIS-88. FOR OTHER REACTIONS,
ISOTROPIC DISTRIBUTIONS IN THE LABORATORY SYSTEM WERE ASSUMED.
MF = 5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS
ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS WERE CALCULATED WITH
PEGASUS FOR INELASTIC SCATTERING TO OVERLAPPING LEVELS AND FOR
OTHER NEUTRON EMITTING REACTIONS.
TABLE 1 NEUTRON OPTICAL POTENTIAL PARAMETERS
DEPTH (MEV) RADIUS(FM) DIFFUSENESS(FM)
---------------------- ------------ ---------------
V = 47.94 R0 = 6.748 A0 = 0.6
WS = 9.13 RS = 7.598 AS = 0.45
VSO= 7.0 RSO= 6.801 ASO= 0.6
THE FORM OF SURFACE ABSORPTION PART IS DER. WOODS-SAXON TYPE.
TABLE 2 LEVEL DENSITY PARAMETERS
NUCLIDE SYST A(1/MEV) T(MEV) C(1/MEV) EX(MEV) PAIRING
---------------------------------------------------------------
58-CE-146 1.918E+01 6.037E-01 1.355E+00 7.176E+00 2.160E+00
58-CE-147 * 2.514E+01 5.363E-01 2.925E+01 6.672E+00 1.170E+00
58-CE-148 * 2.454E+01 5.338E-01 2.640E+00 7.549E+00 2.280E+00
58-CE-149 * 2.392E+01 5.314E-01 1.525E+01 6.206E+00 1.170E+00
59-PR-147 2.440E+01 4.420E-01 3.742E+00 4.298E+00 9.900E-01
59-PR-148 1.996E+01 4.690E-01 1.108E+01 2.807E+00 0.0
59-PR-149 * 2.470E+01 5.314E-01 2.403E+01 6.371E+00 1.110E+00
59-PR-150 * 2.408E+01 5.290E-01 1.412E+02 5.027E+00 0.0
60-ND-148 2.359E+01 5.150E-01 1.328E+00 6.751E+00 2.170E+00
60-ND-149 2.657E+01 4.750E-01 1.192E+01 5.636E+00 1.180E+00
60-ND-150 2.415E+01 5.280E-01 1.867E+00 7.314E+00 2.290E+00
60-ND-151 2.618E+01 4.800E-01 1.152E+01 5.656E+00 1.180E+00
---------------------------------------------------------------
SYST: * = LDP'S WERE DETERMINED FROM SYSTEMATICS.
SPIN CUTOFF PARAMETERS WERE CALCULATED AS 0.146*SQRT(A)*A**(2/3).
IN THE CASTHY CALCULATION, SPIN CUTOFF FACTORS AT 0 MEV WERE
ASSUMED TO BE 10.32 FOR ND-150 AND 5.0 FOR ND-151.
REFERENCES
1) AOKI, T. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR BASIC
AND APPLIED SCIENCE, SANTA FE., VOL. 2, P.1627 (1985).
2) KAWAI, M. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR SCIENCE
AND TECHNOLOGY, MITO, P. 569 (1988).
3) KIKUCHI, Y. ET AL.: JAERI-M 86-030 (1986).
4) TELLIER, H.: CEA-N-1459 (1971).
5) MUGHABGHAB, S.F. AND GARBER, D.I.: "NEUTRON CROSS SECTIONS,
VOL.1, RESONANCE PARAMETERS", BNL 325, 3RD ED., VOL. 1,
(1973).
6) FEDOROVA, A.F., ET AL.: "PROC. 3RD ALL-UNION CONF. ON NEUTRON
PHYSICS, KIEV 1975", VOL. 1, 169.
7) IGARASI, S.: J. NUCL. SCI. TECHNOL., 12, 67 (1975).
8) IIJIMA, S. ET AL.: JAERI-M 87-025, P. 337 (1987).
9) IIJIMA, S. AND KAWAI, M.: J. NUCL. SCI. TECHNOL., 20, 77
(1983).
10) PEREY, F.G: PHYS. REV. 131, 745 (1963).
11) HUIZENGA, J.R. AND IGO, G.: NUCL. PHYS. 29, 462 (1962).
12) LOHR, J.M. AND HAEBERLI, W.: NUCL. PHYS. A232, 381 (1974).
13) BECCHETTI, F.D., JR. AND GREENLEES, G.W.: POLARIZATION
PHENOMENA IN NUCLEAR REACTIONS ((EDS) H.H. BARSHALL AND
W. HAEBERLI), P. 682, THE UNIVERSITY OF WISCONSIN PRESS.
(1971).
14) GILBERT, A. AND CAMERON, A.G.W.: CAN. J. PHYS., 43, 1446
(1965).
15) IIJIMA, S., ET AL.: J. NUCL. SCI. TECHNOL. 21, 10 (1984).
16) GRUPPELAAR, H.: ECN-13 (1977).
17) MATSUMOTO, J.: PRIVATE COMMUNICATION (1981).
18) RAYNAL, J.: PRIVATE COMMUNICATION.
19) RAMAN, S., ET AL.: ATOM. DATA AND NUCL. DATA TABLES 36, 1
(1987)
20) SPEAR, R.H.: ATOM. DATA AND NUCL. DATA TABLE, 42, 55 (1989).
21) BENZI, V. AND REFFO, G.: CCDN-NW/10 (1969).
22) KONONOV, V.N., ET AL.: SOV. J. NUCL. PHYS., 27, 5 (1978).
23) FREHAUT, J., ET AL.: SYMP. ON NEUTRON CROSS SECTIONS FROM
10-50MEV, BNL, P.399 (1980).
24) FORREST, R.A.: AERE-R 12419 (1986).