48-Cd-106
48-CD-106 JNDC EVAL-MAR90 JNDC FP NUCLEAR DATA W.G.
DIST-NOV90
----JENDL-3.2 MATERIAL 4825
-----INCIDENT NEUTRON DATA
------ENDF-6 FORMAT
HISTORY
90-03 NEW EVALUATION FOR JENDL-3 WAS COMPLETED BY JNDC FPND
W.G./1/
MF = 1 GENERAL INFORMATION
MT=451 COMMENTS AND DICTIONARY
MF = 2 RESONANCE PARAMETERS
MT=151 RESOLVED AND UNRESOLVED RESONANCE PARAMETERS
RESOLVED RESONANCE REGION (MLBW FORMULA) : BELOW 700 EV
RESONANCE PARAMETERS WERE BASED ON MUGHABGHAB ET AL./2/
NEUTRON ORBITAL ANGULAR MOMENTUM L OF SOME RESONANCES WAS
ESTIMATED WITH A METHOD OF BOLLINGER AND THOMAS/3/. AVERAGE
RADIATION WIDTH OF 0.153 EV WAS DETERMINED FROM THE EXPERIMEN-
TAL DATA OF MUSGROVE ET AL./4/ ABOVE 2.6 KEV. SCATTERING
RADIUS OF 6.5 FM WAS ADOPTED FROM THE SYSTEMATICS OF MEASURED
VALUES. A NEGATIVE RESONANCE WAS ADDED SO AS TO REPRODUCE THE
THERMAL CAPTURE CROSS SECTION GIVEN BY MUGHABGHAB ET AL.
UNRESOLVED RESONANCE REGION : 700 EV - 100 KEV
THE NEUTRON STRENGTH FUNCTIONS, S0 AND S1 WERE BASED ON THE
COMPILATION OF MUGHABGHAB ET AL., AND S2 WAS CALCULATED WITH
OPTICAL MODEL CODE CASTHY/5/. THE OBSERVED LEVEL SPACING WAS
ADJUSTED TO REPRODUCE THE CAPTURE CROSS SECTION MEASURED BY
MUSGROVE ET AL./6,7/ THE EFFECTIVE SCATTERING RADIUS WAS
OBTAINED FROM FITTING TO THE CALCULATED TOTAL CROSS SECTION AT
100 KEV. THE RADIATION WIDTHS, GG(S) AND GG(P), WERE BASED ON
THE COMPILATION OF MUGHABGHAB ET AL.
TYPICAL VALUES OF THE PARAMETERS AT 70 KEV:
S0 = 1.000E-4, S1 = 5.000E-4, S2 = 0.970E-4, SG(S)= 11.8E-4,
SG(P)= 13.3E-4, GG(S)= 0.155 EV, GG(P)= 0.175 EV, R= 4.699 FM.
CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS (BARNS)
2200 M/S RES. INTEG.
TOTAL 6.492 -
ELASTIC 5.522 -
CAPTURE 0.9695 10.7
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 TO REPRODUCE THE CD-NATURAL TOTAL CROSS SECTIONS
MEASURED BY FOSTER AND GLASGOW/9/, POENITZ AND WHALEN/10/ AND
SO ON. THE OMP'S FOR CHARGED PARTICLES ARE AS FOLLOWS:
PROTON = PEREY/11/
ALPHA = HUIZENGA AND IGO/12/
DEUTERON = LOHR AND HAEBERLI/13/
HELIUM-3 AND TRITON = BECCHETTI AND GREENLEES/14/
PARAMETERS FOR THE COMPOSITE LEVEL DENSITY FORMULA OF GILBERT
AND CAMERON/15/ WERE EVALUATED BY IIJIMA ET AL./16/ 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
/17/.
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 BASED ON EVALUATED NUCLEAR
STRUCTURE DATA FILE (1987 VERSION)/18/ AND NUCLEAR DATA
SHEETS/19/.
NO. ENERGY(MEV) SPIN-PARITY DWBA CAL.
GR. 0.0 0 +
1 0.6327 2 + *
2 1.4938 4 +
3 1.7166 2 +
4 2.1045 4 +
5 2.3050 4 +
6 2.3306 5 +
7 2.3386 4 +
8 2.3705 3 - *
9 2.4856 4 +
10 2.4917 6 +
11 2.5031 6 +
LEVELS ABOVE 2.522 MEV WERE ASSUMED TO BE OVERLAPPING.
FOR THE LEVELS WITH AN ASTERISK, THE CONTRIBUTION OF DIRECT
INELASTIC SCATTERING CROSS SECTIONS WAS CALCULATED BY THE
DWUCK-4 CODE/20/. DEFORMATION PARAMETERS (BETA2 = 0.1732 AND
BETA3 = 0.194) WERE BASED ON THE DATA COMPILED BY RAMAN ET
AL./21/ AND SPEAR/22/, RESPECTIVELY.
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/23/ AND NORMALIZED TO 1 MILLI-BARN AT 14 MEV.
THE GAMMA-RAY STRENGTH FUNCTION (1.42E-03) WAS ADJUSTED TO
REPRODUCE THE CAPTURE CROSS SECTION OF 340 MILLI-BARNS AT 70
KEV MEASURED BY MUSGROVE ET AL./6,7/
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 =103 (N,P) CROSS SECTION
MT =104 (N,D) CROSS SECTION
MT =105 (N,T) CROSS SECTION
MT =106 (N,HE3) CROSS SECTION
MT =107 (N,ALPHA) CROSS SECTION
MT =111 (N,2P) CROSS SECTION
THESE REACTION CROSS SECTIONS WERE CALCULATED WITH THE
PREEQUILIBRIUM AND MULTI-STEP EVAPORATION MODEL CODE PEGASUS.
THE KALBACH'S CONSTANT K (= 122.0) WAS ESTIMATED BY THE
FORMULA DERIVED FROM KIKUCHI-KAWAI'S FORMALISM/24/ AND LEVEL
DENSITY PARAMETERS.
FINALLY, THE (N,2N) AND (N,ALPHA) CROSS SECTIONS WERE
NORMALIZED TO THE FOLLOWING VALUES AT 14.5 MEV:
(N,2N) 900.00 MB (RECOMMENDED BY BYCHKOV+/25/)
(N,ALPHA) 100.00 MB (RECOMMENDED BY FORREST/26/)
THE (N,P) CROSS SECTION WAS DETERMINED BY EYE-GUIDING OF THE
DATA MEASURED BY BORMANN ET AL./27/
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 DWUCK-4. 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 FROM OVERLAPPING LEVELS AND FOR
OTHER NEUTRON EMITTING REACTIONS.
TABLE 1 NEUTRON OPTICAL POTENTIAL PARAMETERS
DEPTH (MEV) RADIUS(FM) DIFFUSENESS(FM)
---------------------- ------------ ---------------
V = 50.01-0.5528E R0 = 5.972 A0 = 0.56
WS = 8.165 RS = 6.594 AS = 0.44
VSO= 5.261 RSO= 5.97 ASO= 0.267
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
---------------------------------------------------------------
46-PD-102 1.831E+01 6.210E-01 6.406E-01 7.665E+00 2.640E+00
46-PD-103 1.733E+01 6.550E-01 5.327E+00 6.637E+00 1.350E+00
46-PD-104 1.630E+01 6.650E-01 8.743E-01 7.305E+00 2.290E+00
46-PD-105 1.791E+01 6.700E-01 9.137E+00 7.207E+00 1.350E+00
47-AG-103 * 1.627E+01 6.427E-01 2.835E+00 5.882E+00 1.290E+00
47-AG-104 * 1.737E+01 6.403E-01 3.551E+01 5.016E+00 0.0
47-AG-105 * 1.848E+01 6.379E-01 1.390E+01 6.378E+00 9.400E-01
47-AG-106 1.839E+01 5.480E-01 1.824E+01 3.696E+00 0.0
48-CD-104 * 1.643E+01 6.403E-01 3.532E-01 7.266E+00 2.650E+00
48-CD-105 1.600E+01 6.850E-01 4.000E+00 6.612E+00 1.360E+00
48-CD-106 1.468E+01 6.950E-01 5.785E-01 7.078E+00 2.300E+00
48-CD-107 1.647E+01 6.740E-01 4.374E+00 6.626E+00 1.360E+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 1.094 FOR CD-106 AND 5.0 FOR CD-107.
REFERENCES
1) KAWAI, M. ET AL.: PROC. INT. CONF. ON NUCLEAR DATA FOR SCIENCE
AND TECHNOLOGY, MITO, P. 569 (1988).
2) MUGHABGHAB, S.F. ET AL.: "NEUTRON CROSS SECTIONS, VOL. I,
PART A", ACADEMIC PRESS (1981).
3) BOLLINGER, L.M. AND THOMAS, G.E.: PHYS. REV., 171,1293(1968).
4) MUSGROVE, A.R. DE L., ET AL.: J. PHSICS PT G, 4, 771 (1978).
5) IGARASI, S.: J. NUCL. SCI. TECHNOL., 12, 67 (1975).
6) MUSGROVE, A.R. DE L., ET AL.: PROC. OF INT. CONF. ON NEUTRON
PHYSICS AND NUCL. DATA FOR REACTORS, HARWELL 1978, P.449
7) ALLEN, B.J., ET AL.: NUCL. SCI. ENG., 82, 230 (1982).
8) IIJIMA, S. ET AL.: JAERI-M 87-025, P. 337 (1987).
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(1971).
10) POENITZ, W.P. AND WHALEN, J.F.: ANL-NDM-80 (1983).
11) PEREY, F.G: PHYS. REV. 131, 745 (1963).
12) HUIZENGA, J.R. AND IGO, G.: NUCL. PHYS. 29, 462 (1962).
13) LOHR, J.M. AND HAEBERLI, W.: NUCL. PHYS. A232, 381 (1974).
14) 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).
15) GILBERT, A. AND CAMERON, A.G.W.: CAN. J. PHYS., 43, 1446
(1965).
16) IIJIMA, S., ET AL.: J. NUCL. SCI. TECHNOL. 21, 10 (1984).
17) GRUPPELAAR, H.: ECN-13 (1977).
18) ENSDF: EVALUATED NUCLEAR STRUCTURE DATA FILE (JUNE 1987).
19) NUCLEAR DATA SHEETS, 30, 305 (1980).
20) KUNZ, P.D.: PRIVATE COMMUNICATION.
21) RAMAN, S., ET AL.: ATOM. DATA AND NUCL. DATA TABLES 36, 1
(1987)
22) SPEAR, R.H.: ATOM. DATA AND NUCL. DATA TABLE, 42, 55 (1989).
23) BENZI, V. AND REFFO, G.: CCDN-NW/10 (1969).
24) KIKUCHI, K. AND KAWAI, M.: "NUCLEAR MATTER AND NUCLEAR
REACTIONS", NORTH HOLLAND (1968).
25) BYCHKOV, V.M. ET AL.: INDC(CCP)-146/LJ (1980).
26) FORREST, R.A.: AERE-R 12419 (1986).
27) BORMANN, M., ET AL.: NUCL. PHYS., A115, 309 (1968).