JENDL-3.3 Ac-226 0 0 0 0
8.922600+4 2.240840+2 0 0 0 28928 1451 1
0.000000+0 1.000000+0 0 0 0 68928 1451 2
1.000000+0 2.000000+7 3 0 10 38928 1451 3
0.000000+0 0.000000+0 0 0 83 198928 1451 4
89-AC-226 TIT EVAL-AUG88 N.TAKAGI 8928 1451 5
DIST-MAR02 REV2-FEB02 20020222 8928 1451 6
----JENDL-3.3 MATERIAL 8928 8928 1451 7
-----INCIDENT NEUTRON DATA 8928 1451 8
------ENDF-6 FORMAT 8928 1451 9
8928 1451 10
=========================================================== 8928 1451 11
JENDL-3.2 data were automatically transformed to JENDL-3.3. 8928 1451 12
Interpolation of spectra: 22 (unit base interpolation) 8928 1451 13
(3,251) deleted, T-matrix of (4,2) deleted, and others. 8928 1451 14
=========================================================== 8928 1451 15
8928 1451 16
HISTORY 8928 1451 17
88-08 NEW EVALUATION WAS MADE BY N. TAKAGI (TOKYO INSTITUTE OF 8928 1451 18
TECHNOLOGY, TIT) 8928 1451 19
8928 1451 20
MF=1 GENERAL INFORMATION 8928 1451 21
MT=451 COMMENT AND DICTIONARY 8928 1451 22
8928 1451 23
MF=2 RESONANCE PARAMETERS 8928 1451 24
MT=151 RESONANCE PARAMETERS 8928 1451 25
NO RESONANCE PARAMETERS WERE GIVEN. 8928 1451 26
8928 1451 27
2200-M/S CROSS SECTIONS AND RESONANCE INTEGRALS 8928 1451 28
2200 M/S VALUE RES. INT. 8928 1451 29
TOTAL 112.40 B - 8928 1451 30
ELASTIC 12.40 B - 8928 1451 31
CAPTURE 100.00 B 1680 B 8928 1451 32
8928 1451 33
MF=3 NEUTRON CROSS SECTIONS 8928 1451 34
MT=1 TOTAL CROSS SECTION 8928 1451 35
BELOW 0.4 EV, CALCULATED AS SUM OF MT'S = 2 AND 102. 8928 1451 36
ABOVE 0.4 EV, OPTICAL MODEL CALCULATION WAS MADE WITH 8928 1451 37
CASTHY/2/. THE POTENTIAL PARAMETERS/3/ USED ARE AS 8928 1451 38
FOLLOWS, 8928 1451 39
V = 41.0 - 0.05*EN (MEV) 8928 1451 40
WS= 6.4 - 0.15*SQRT(EN) (MEV) 8928 1451 41
WV= 0 , VSO = 7.0 (MEV) 8928 1451 42
R = RSO = 1.31 , RS = 1.38 (FM) 8928 1451 43
A = ASO = 0.47 , B = 0.47 (FM) 8928 1451 44
8928 1451 45
MT=2 ELASTIC SCATTERING CROSS SECTION 8928 1451 46
BELOW 0.4 EV, THE CONSTANT CROSS SECTION OF 12.4 BARNS WAS8928 1451 47
ASSUMED, WHICH WAS THE SHAPE ELASTIC SCATTERING CROSS 8928 1451 48
SECTION CALCULATED WITH OPTICAL MODEL. ABOVE THIS ENERGY,8928 1451 49
OPTICAL MODEL CALCULATION WAS ADOPTED. 8928 1451 50
8928 1451 51
MT=4,51-52,91 INELASTIC SCATTERING CROSS SECTIONS. 8928 1451 52
CALCULATED WITH OPTICAL AND STATISTICAL MODELS BY MEANS OF8928 1451 53
CASTHY/2/. NO EXCITED LEVELS WERE TAKEN INTO CALCULATION, 8928 1451 54
BECAUSE SPIN OF ALL LEVELS WERE UNKNOWN/4/. 8928 1451 55
NO ENERGY(KEV) SPIN-PARITY 8928 1451 56
G.S. 0.0 1 + 8928 1451 57
LEVELS ABOVE 290 KEV WERE ASSUMED TO BE OVERLAPPING. 8928 1451 58
THE LEVEL DENSITY PARAMETERS WERE TAKEN FROM REF. 5. 8928 1451 59
8928 1451 60
MT=16,17,37 (N,2N), (N,3N) AND (N,4N) REACTION CROSS SECTIONS 8928 1451 61
CALCULATED WITH EVAPORATION MODEL. 8928 1451 62
8928 1451 63
MT=102 CAPTURE CROSS SECTION 8928 1451 64
ASSUMED TO BE 100 BARNS AT 0.0253 EV, AND IN 1/V FORM 8928 1451 65
BELOW 0.4 EV. ABOVE 0.4 EV, CALCULATED WITH CASTHY. 8928 1451 66
THE GAMMA-RAY STRENGTH FUNCTION WAS ESTIMATED FROM 8928 1451 67
GAMMA-GAMMA = 0.040 EV AND LEVEL SPACING = 0.8 EV. 8928 1451 68
8928 1451 69
MT=251 MU-L 8928 1451 70
CALCULATED WITH CASTHY. 8928 1451 71
8928 1451 72
MF=4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 8928 1451 73
MT=2,91 CALCULATED WITH OPTICAL MODEL. 8928 1451 74
MT=16,17,37 ISOTROPIC IN THE LAB SYSTEM. 8928 1451 75
8928 1451 76
MF=5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS 8928 1451 77
MT=16,17,37,91 EVAPORATION SPECTRA 8928 1451 78
OBTAINED FROM LEVEL DENSITY PARAMETERS. 8928 1451 79
8928 1451 80
REFERENCES 8928 1451 81
1) HOWERTON R.J.: NUCL. SCI. ENG., 62, 438 (1977). 8928 1451 82
2) IGARASI S.: J.NUCL.SCI.TECHNOL.,12,67 (1975). 8928 1451 83
3) OHSAWA T., OHTA M.: J. NUCL. SCI. TECHNOL., 18, 408 (1981). 8928 1451 84
4) ELLIS-AKOVALI Y.A.: NUC;. DATA SHEETS, 50, 229 (1987). 8928 1451 85
5) GILBERT A., CAMERON A.G.W.: CAN. J. PHYS., 43, 1446 (1965). 8928 1451 86
8928 1451 87
1 451 106 18928 1451 88
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3 1 34 18928 1451 90
3 2 16 18928 1451 91
3 4 11 18928 1451 92
3 16 8 18928 1451 93
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3 37 4 18928 1451 95
3 91 11 18928 1451 96
3 102 16 18928 1451 97
4 2 129 28928 1451 98
4 16 10 18928 1451 99
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4 37 10 18928 1451 101
4 91 10 18928 1451 102
5 16 17 28928 1451 103
5 17 22 28928 1451 104
5 37 25 28928 1451 105
5 91 10 28928 1451 106
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