IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0
2.70590+ 4 5.84269+ 1 1 0 0 56199 1451 1
0.00000+ 0 0.00000+ 0 0 0 84 06199 1451 2
27-CO- 59 BNL ANL EVAL-JAN74 T.KRIEGER(BNL)A.SMITH,D.SMITH 6199 1451 3
DIST-1974 6199 1451 4
P.C.TO NORMALIZATION AND STANDARDS SUBCOMMITTEE OF CSEWG 10/73 6199 1451 5
THE PRESENT EVALUATION OF CO-59 (FOR ENDF/B IV) CONSISTS OF TWO6199 1451 6
PARTS, AN EVALUATION BELOW 100 KEV BY T.J. KRIEGER , BROOKHAVEN 6199 1451 7
NATIONAL LABORATORY, AND ONE ABOVE 100 KEV BY A.B. SMITH AND 6199 1451 8
D.L. SMITH, ARGONNE NATIONAL LABORATORY. 6199 1451 9
**** CO-59 EVALUATION BELOW 100 KEV, T.J. KRIEGER, BNL, 1/74. ****6199 1451 10
THE RESONANCE REGION HAS BEEN EXTENDED FROM 10**-5 EV - 36 KEV 6199 1451 11
IN ENDF/B III TO 10**-5 EV - 100 KEV FOR ENDF/B IV. HOWEVER, THE 6199 1451 12
LIST OF RESONANCES EXTENDS TO 119 KEV. THERE IS NO UNRESOLVED 6199 1451 13
REGION. CARE HAS BEEN TAKEN TO TIE IN SMOOTHLY WITH THE EVALUATION6199 1451 14
ABOVE 100 KEV. 6199 1451 15
THE RESONANCE PARAMETERS WERE TAKEN FROM THE RECENTLY PUBLISHED6199 1451 16
NEW EDITION OF THE BNL-325 COMPILATION (REF. 1) WITH THE FOLLOWING6199 1451 17
MODIFICATIONS, 6199 1451 18
(1) THE EFFECTIVE SCATTERING RADIUS R-PRIME WAS INCREASED FROM 6199 1451 19
5.3F (REF. 1) TO 6.8F IN ORDER TO IMPROVE THE FIT OF THE TOTAL 6199 1451 20
CROSS SECTION BETWEEN RESONANCES WITH THE DATA OF J. GARG ET AL. 6199 1451 21
(REF. 2), 6199 1451 22
(2) THE CHANGE IN R-PRIME MENTIONED ABOVE ENTAILED A CHANGE IN 6199 1451 23
THE BOUND STATE PARAMETERS. THESE ARE DETERMINED BY FITTING TO THE6199 1451 24
EXPERIMENTAL VALUES (REF. 1) OF THE THERMAL SCATTERING AND THERMAL6199 1451 25
CAPTURE CROSS SECTIONS AND OF THE COHERENT SCATTERING AMPLITUDE, 6199 1451 26
(3) UNKNOWN J-VALUES WERE ASSIGNED THE VALUES 3 OR 4 AT RANDOM, 6199 1451 27
AN ATTEMPT BEING MADE TO KEEP THE LEVEL DENSITY PROPORTIONAL TO 6199 1451 28
2J+1, 6199 1451 29
(4) TO IMPROVE THE FIT WITH THE DATA OF REF. 2, A FEW RESONANCES6199 1451 30
IN REF. 1 WERE ELIMINATED COMPLETELY AND SOME IN THE HIGH ENERGY 6199 1451 31
REGION WERE SHIFTED SLIGHTLY, 6199 1451 32
(5) UNKNOWN GAMMA WIDTHS (FOR RESONANCES ABOVE 18.92 KEV) WERE 6199 1451 33
ASSIGNED THE VALUE GAMMA-SUB-GAMMA = 0.48 EV, EXCEPT THAT ABOVE 6199 1451 34
90 KEV THE GAMMA WIDTH WAS INCREASED TO 1.5 EV IN ORDER TO IMPROVE6199 1451 35
THE FIT TO CAPTURE DATA AND TO SMOOTH THE TIE-IN WITH THE EVALUA- 6199 1451 36
TION ABOVE 100 KEV. 6199 1451 37
USING THE RESONANCE PARAMETERS OF REF. 1 WITH THE ABOVE MODI- 6199 1451 38
FICATIONS, BREIT-WIGNER MULTI-LEVEL CALCULATIONS WERE PERFORMED 6199 1451 39
AND COMPARED WITH THE DATA OF REF. 2. THE FIT WAS GENERALLY VERY 6199 1451 40
GOOD. HOWEVER, FOR FURTHER IMPROVEMENT, A SMALL BACKGROUND CONTR- 6199 1451 41
IBUTION (NO LARGER THAN +/- 1 B BELOW 95 KEV) TO THE ELASTIC SCAT-6199 1451 42
TERING CROSS SECTION WAS INTRODUCED IN FILE 3 IN SMALL, SELECTED 6199 1451 43
ENERGY REGIONS. THE CAPTURE CROSS SECTION WAS NOT ASSIGNED A FILE 6199 1451 44
3 BACKGROUND CONTRIBUTION. 6199 1451 45
THE THERMAL (0.0253 EV) CROSS SECTIONS CALCULATED FROM FILES 2 6199 1451 46
AND 3 ARE AS FOLLOWS. 6199 1451 47
THERMAL TOTAL CROSS SECTION = 43.88 BARNS, 6199 1451 48
THERMAL ELASTIC SCATTERING CROSS SECTION = 6.66 BARNS, 6199 1451 49
THERMAL CAPTURE CROSS SECTION = 37.22 BARNS. 6199 1451 50
THESE VALUES ARE WITHIN THE LIMITS GIVEN IN REF. 1. 6199 1451 51
THE RESONANCE CAPTURE INTEGRAL (LOWER LIMIT =0.5 EV) CALCULATED6199 1451 52
FROM FILE 2 IS 76.7 BARNS WHICH IS WITHIN THE LIMITS GIVEN IN 6199 1451 53
REF. 1. 6199 1451 54
** EVALUATION 0.1-20.0 MEV,A.B. SMITH AND D.L. SMITH, ANL, 7/73***6199 1451 55
DETAILS GIVEN BY P.T. GUENTHER ET AL. (REF. 3). SUMMARY FOLLOWS. 6199 1451 56
*********** 6199 1451 57
MT-16, (N,2N) REACTION CROSS SECTION--- 6199 1451 58
CONSIDERABLE EXPERIMENTAL DATA ARE AVAILABLE FROM ACTIVATION 6199 1451 59
METHODS. A SMOOTH CURVE WAS CONSTRUCTED BASED ON DATA SETS JUD- 6199 1451 60
GED TO BE THE MOST RELIABLE. THE ENERGY SPECTRA OF EMITTED NEUT-6199 1451 61
RONS HAVE NOT BEEN MEASURED AND SO THEY WERE ASSUMED TO BE REP- 6199 1451 62
RESENTABLE BY AN EVAPORATION MODEL WITH A TEMPERATURE SOMEWHAT 6199 1451 63
SOFTER THAN FOR CONTINUUM ELASTIC SCATTERING. 6199 1451 64
MT-102, RADIATIVE CAPTURE CROSS SECTION--- 6199 1451 65
EXPERIMENTAL DATA ARE AVAILABLE FROM ACTIVATION AND PROMPT GAMMA6199 1451 66
RAY DETECTION MEASUREMENTS. ISOMER RATIO DATA ARE AVAILABLE TO 6199 1451 67
CORRECT ACTIVATION RESULTS. THE EXISTING DATA ARE SPARSE BUT 6199 1451 68
SUFFICIENT TO PROVIDE A GUIDE FOR AN EVALUATION. THERE SEEMS TO 6199 1451 69
BE NO EVIDENCE FOR GIANT RESONANCE BEHAVIOR IN THE ENERGY RANGE 6199 1451 70
2.0-14.0 MEV. 6199 1451 71
MT=107 EVALUATED APRIL 72 BY J.D.JENKINS 6199 1451 72
P.C.TO NORM.AND STAND.SUBCOM 8/72 6199 1451 73
EVALUATION PARALLELS THAT OF BRESESTI ET.AL 6199 1451 74
*** REFERENCES *** 6199 1451 75
1. S.F. MUGHABGHAB AND D.I. GARBER, NEUTRON CROSS SECTIONS, 6199 1451 76
VOLUME 1, RESONANCE PARAMETERS. BNL-325, THIRD EDITION, 6199 1451 77
VOLUME 1, JUNE, 1973. 6199 1451 78
2. J.B. GARG, J. RAINWATER, AND W.W. HAVENS, BAP,8,334 (1963) 6199 1451 79
AND COLUMBIA REPORT CR-1860 (1964). ALSO, PRIVATE COMMUNICA-6199 1451 80
TION, 1965. 6199 1451 81
3. P.T. GUENTHER, P.A. MOLDAUER, A.B. SMITH, D.L. SMITH, AND 6199 1451 82
J.F. WHALEN, COBALT FAST NEUTRON CROSS SECTIONS- MEASUREMENT6199 1451 83
AND EVALUATION, ANL REPORT ANL/NDM-1, JULY, 1973. 6199 1451 84
4. A. WAPSTRA AND N. GOVE, NUCLEAR DATA A9, 267 (1971). 6199 1451 85
5. BRESESTI ET.AL. NUC.SCI.AND ENG.40,331,1970 6199 1451 86
1 451 91 6199 1451 87
2 151 97 6199 1451 88
3 16 8 6199 1451 89
3 102 10 6199 1451 90
3 107 12 6199 1451 91
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3.50000+ 0 6.80000- 1 0 0 1 06199 2151 97
5.84269+ 1 0.00000+ 0 0 0 552 926199 2151 98
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1.32000+ 2 4.00000+ 0 5.60000+ 0 5.12000+ 0 4.80000- 1 0.00000+ 06199 2151 100
1.38000+ 3 3.00000+ 0 4.85600- 1 5.60000- 3 4.80000- 1 0.00000+ 06199 2151 101
2.85000+ 3 4.00000+ 0 5.85000- 1 1.05000- 1 4.80000- 1 0.00000+ 06199 2151 102
3.98000+ 3 3.00000+ 0 5.70000- 1 9.00000- 2 4.80000- 1 0.00000+ 06199 2151 103
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8.05000+ 3 3.00000+ 0 3.73000+ 1 3.70000+ 1 3.00000- 1 0.00000+ 06199 2151 107
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9.69000+ 3 3.00000+ 0 3.26000+ 0 2.70000+ 0 5.60000- 1 0.00000+ 06199 2151 109
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2.19400+ 4 3.00000+ 0 7.45430+ 2 7.45000+ 2 4.80000- 1 0.00000+ 06199 2151 116
2.25100+ 4 4.00000+ 0 2.53480+ 2 2.53000+ 2 4.80000- 1 0.00000+ 06199 2151 117
2.44600+ 4 3.00000+ 0 3.60480+ 2 3.60000+ 2 4.80000- 1 0.00000+ 06199 2151 118
2.51500+ 4 4.00000+ 0 1.84480+ 2 1.84000+ 2 4.80000- 1 0.00000+ 06199 2151 119
2.59200+ 4 4.00000+ 0 2.54800+ 1 2.50000+ 1 4.80000- 1 0.00000+ 06199 2151 120
2.73500+ 4 4.00000+ 0 1.70480+ 2 1.70000+ 2 4.80000- 1 0.00000+ 06199 2151 121
2.94000+ 4 3.00000+ 0 1.64800+ 1 1.60000+ 1 4.80000- 1 0.00000+ 06199 2151 122
3.01100+ 4 4.00000+ 0 3.27480+ 2 3.27000+ 2 4.80000- 1 0.00000+ 06199 2151 123
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5.97600+ 4 4.00000+ 0 1.00080+ 2 9.96000+ 1 4.80000- 1 0.00000+ 06199 2151 145
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1.10950+ 5 3.00000+ 0 9.25000+ 1 9.10000+ 1 1.50000+ 0 0.00000+ 06199 2151 181
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1.13210+ 5 4.00000+ 0 1.34500+ 2 1.33000+ 2 1.50000+ 0 0.00000+ 06199 2151 184
1.14110+ 5 3.00000+ 0 1.95000+ 1 1.80000+ 1 1.50000+ 0 0.00000+ 06199 2151 185
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1.16440+ 5 4.00000+ 0 9.05000+ 1 8.90000+ 1 1.50000+ 0 0.00000+ 06199 2151 187
1.17260+ 5 4.00000+ 0 6.05500+ 2 6.04000+ 2 1.50000+ 0 0.00000+ 06199 2151 188
1.18630+ 5 3.00000+ 0 1.39550+ 3 1.39400+ 3 1.50000+ 0 0.00000+ 06199 2151 189
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0.00000+ 0-1.04610+ 7 0 0 1 146199 3 16 194
14 2 6199 3 16 195
1.06400+ 7 0.00000+ 0 1.10000+ 7 2.00000- 2 1.15000+ 7 1.50000- 16199 3 16 196
1.20000+ 7 2.80000- 1 1.25000+ 7 4.00000- 1 1.30000+ 7 5.00000- 16199 3 16 197
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21 2 6199 3102 204
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5.00000+ 5 9.00000- 3 6.00000+ 5 8.00000- 3 7.00000+ 5 8.00000- 36199 3102 207
8.00000+ 5 8.50000- 3 9.00000+ 5 8.40000- 3 1.25000+ 6 7.60000- 36199 3102 208
1.50000+ 6 6.20000- 3 1.75000+ 6 4.80000- 3 2.00000+ 6 4.00000- 36199 3102 209
2.50000+ 6 3.30000- 3 4.00000+ 6 2.50000- 3 6.00000+ 6 2.00000- 36199 3102 210
1.00000+ 7 1.70000- 3 1.40000+ 7 1.50000- 3 2.00000+ 7 1.50000- 36199 3102 211
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0.00000+ 0 3.17800+ 5 0 0 1 266199 3107 214
26 2 6199 3107 215
5.00000+ 6 0.00000+ 0 5.50000+ 6 4.00000- 4 6.00000+ 6 1.00000- 36199 3107 216
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1.31000+ 7 2.79000- 2 1.35000+ 7 2.89000- 2 1.38500+ 7 2.91000- 26199 3107 220
1.42500+ 7 2.91000- 2 1.45000+ 7 2.89000- 2 1.50000+ 7 2.80000- 26199 3107 221
1.60000+ 7 2.48000- 2 1.70000+ 7 2.12000- 2 1.75000+ 7 1.88000- 26199 3107 222
1.77500+ 7 1.77000- 2 1.85000+ 7 1.52000- 2 1.87500+ 7 1.37000- 26199 3107 223
1.90000+ 7 1.27000- 2 2.00000+ 7 1.14000- 2 6199 3107 224
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