IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0
3.00600+ 3 5.96340+ 0 0 0 0 241271 1451 1
0.00000+ 0 0.00000+ 0 0 0 196 01271 1451 2
3-LI- 6 LASL EVAL-APR74 G.M.HALE, D.DODDER, P.YOUNG + 1271 1451 3
DIST-MAY74 1271 1451 4
*****************************************************************1271 1451 5
* *1271 1451 6
* TOTAL, ELASTIC, AND (N,ALPHA) CROSS SECTIONS AND ELASTIC *1271 1451 7
* ANGULAR DISTRIBUTIONS REPLACED FOR NEUTRON ENERGIES BELOW *1271 1451 8
2.0 MEV BY G.M.HALE, D.DODDER, P.YOUNG, AND L.STEWART AT LASL,*1271 1451 9
APR.,1974. THE NEW DATA RESULT FROM A COUPLED-CHANNEL *1271 1451 10
* R-MATRIX ANALYSIS THAT IS BRIEFLY DESCRIBED BELOW. *1271 1451 11
* THE (N,GAMMA) CROSS SECTION FOR THERMAL NEUTRONS WAS ALSO *1271 1451 12
* REPLACED, AS DESCRIBED BELOW. *1271 1451 13
* *1271 1451 14
* THE THERMAL CROSS SECTIONS ARE AS FOLLOWS, *1271 1451 15
* TOTAL MT=1 SIGMA = 940.76 BARNS *1271 1451 16
* ELASTIC MT=2 SIGMA = 0.72124 BARNS *1271 1451 17
* (N,GAMMA) MT=102 SIGMA = 0.03850 BARNS *1271 1451 18
* (N,ALPHA) MT=107 SIGMA = 940.00 BARNS *1271 1451 19
* *1271 1451 20
*****************************************************************1271 1451 21
* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 1271 1451 22
* * 1271 1451 23
* PHOTON PRODUCTION ADDED BY LABAUVE AND STEWART AT *1271 1451 24
* LASL. OCT. 1972. *1271 1451 25
* * 1271 1451 26
* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 1271 1451 27
LI-6 LASL EVAL-AUG71 M.E.BATTAT AND R.J.LABAUVE 1271 1451 28
DIST-JAN72 1271 1451 29
* * * * * * *1271 1451 30
1271 1451 31
* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *1271 1451 32
* *1271 1451 33
* CROSS SECTION STANDARD -- LI-6 (N,ALPHA) *1271 1451 34
* *1271 1451 35
* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *1271 1451 36
1271 1451 37
1271 1451 38
MF = 2 RESONANCE PARAMETERS 1271 1451 39
1271 1451 40
MT = 151. SCATTERING RADIUS ONLY. 1271 1451 41
1271 1451 42
1271 1451 43
MF = 3 SMOOTH CROSS SECTIONS 1271 1451 44
1271 1451 45
MT=1, TOTAL. BELOW 1.5 MEV, THE DATA ARE BASED ON A COUPLED- 1271 1451 46
CHANNEL R-MATRIX ANALYSIS OF THE TOTAL CROSS SECTION MEASURE- 1271 1451 47
MENTS OF REF. 2, THE (N,ALPHA) MEASUREMENTS OF REF.14 BELOW 1271 1451 48
400 KEV AND REF.15 AT HIGHER ENERGIES, AND VARIOUS MEASURE- 1271 1451 49
MENTS OF N-6LI AND ALPHA-T ELASTIC SCATTERING. THE TOTAL 1271 1451 50
WAS MATCHED BETWEEN 1.5 AND 2.0 MEV TO A CURVE BASED PRI- 1271 1451 51
MARILY ON THE DATA OF FOSTER AND GLASGOW (REF.4) WHICH EXTEND 1271 1451 52
TO 15 MEV. EXTRAPOLATION TO 20 MEV IS BASED ON THE DATA OF 1271 1451 53
PETERSON (REF.5). 1271 1451 54
1271 1451 55
MT=2,ELASTIC. BELOW 1.5 MEV, PREDICTIONS OF THE R-MATRIX 1271 1451 56
ANALYSIS DESCRIBED UNDER MT=1 WERE USED. THESE PREDICTIONS 1271 1451 57
ARE CONSISTENT WITH THE DATA OF REF.16 (BUT SUBSTANTIALLY 1271 1451 58
HIGHER THAN THOSE OF REF.9) BELOW 200 KEV. ABOVE 200 KEV, 1271 1451 59
THEY AGREE WITH THE DATA OF REF.9 AND REF.3. MATCHED BETWEEN 1271 1451 60
1.5 AND 2 MEV TO A CURVE BASED PRIMARILY ON THE HOPKINS 1271 1451 61
EVALUATION (REF.6) BETWEEN 4 AND 10 MEV. AT 14 MEV, A VALUE 1271 1451 62
OF .880 BARNS INSTEAD OF .865 BARNS (REF.1) WAS USED. 1271 1451 63
1271 1451 64
MT = 4, TOTAL INELASTIC. SUM OF MT = 52 AND MT = 91. 1271 1451 65
1271 1451 66
MT =24, (N,2N)ALPHA-P. EVALUATION OF REF. 1 TO 15 MEV. E.TRAP-1271 1451 67
OLATED TO 20 MEV. 1271 1451 68
1271 1451 69
MT =52, (N,N PRIME)GAMMA. DATA OF PRESSER (REF. 7) TO 7 MEV. 1271 1451 70
CONSTANT CROSS SECTION OF 5 MILLIBARN ASSUMED ABOVE 7 MEV. 1271 1451 71
1271 1451 72
MT = 91, (N,N PRIME)ALPHA-D. REF. 1 UP TO ABOUT 3 MEV. HOP- 1271 1451 73
KINS EVALUATION (REF. 6) CONSIDERED BETWEEN 4 AND 10 MEV. A 1271 1451 74
SOMEWHAT HIGHER VALUE - 433 VERSUS 403 MILLIBARN - THAN IN 1271 1451 75
REF. 1 WAS USED AT 14 MEV. EXTRAPOLATION TO 20 MEV USING 1271 1451 76
DIFFERENCE BETWEEN TOTAL AND OTHER PARTIAL CROSS SECTIONS. 1271 1451 77
THIS CROSS SECTION IS HIGHER THAN THE ROSEN AND STEWART 1271 1451 78
DATA AT ALL ENERGIES WITH THE 14 MEV. POINT 433 MB INSTEAD OF 1271 1451 79
THE MEASURED VALUE OF 315 MB. 1271 1451 80
1271 1451 81
MT=102, (N,GAMMA). BELOW 15 KEV, BASED ON A NEW THERMAL MEA- 1271 1451 82
SUREMENT BY JURNEY (REF.19) OF 38.5 +/- 3 MB. AT HIGHER ENER- 1271 1451 83
GIES, BASED ON THE EVALUATION OF REF. 1. 1271 1451 84
1271 1451 85
MT = 103, (N,P). DATA OF PRESSER (REF. 7) TO 7 MEV. REF. 1 1271 1451 86
FROM 7 TO 15 MEV. E.TRAPOLATED TO 20 MEV. 1271 1451 87
1271 1451 88
MT=107, (N,ALPHA). BELOW 1.5 MEV, BASED ON THE R-MATRIX ANALY-1271 1451 89
SIS DESCRIBED UNDER MT=1. THE EVALUATION AGREES BELOW 50 KEV 1271 1451 90
WITH THE DATA OF REF.14, AND WITH THE RATIO MEASUREMENT OF 1271 1451 91
REF.18, CONVERTED WITH THE VERSION 4 10B(N,ALPHA) CROSS 1271 1451 92
SECTION. BETWEEN 50 AND 300 KEV, THE EVALUATED CROSS SECTION 1271 1451 93
IS SUBSTANTIALLY HIGHER THAN THE DATA OF REF.14 (BUT NOT AS 1271 1451 94
HIGH AS THOSE OF REF.12). THE HIGHER (N,ALPHA) CROSS SECTION 1271 1451 95
SEEMS TO BE REQUIRED TO FIT THE TOTAL CROSS SECTION DATA OF 1271 1451 96
REF.2, AND THE ALPHA-T ELASTIC SCATTERING DATA OF REF.17. 1271 1451 97
ABOVE 400 KEV, THE EVALUATION AGREES REASONABLY WELL 1271 1451 98
WITH THE DATA OF REF.13 AND REF.15. MATCHED BETWEEN 1.5 AND 1271 1451 99
2 MEV TO THE (N,ALPHA) CROSS SECTION EVALUATION BETWEEN 2 AND 1271 1451 100
15 MEV OF REF.1. EXTRAPOLATION TO 20 MEV IS BASED ON THE 1271 1451 101
KERN AND KREGER DATA (REF.8) BETWEEN 15 AND 18 MEV. 1271 1451 102
1271 1451 103
MT = 251, 252, 253 (MUBAR, .I, GAMMA). CALCULATED USING 1271 1451 104
ELASTIC ANGULAR DISTRIBUTIONS GIVEN IN FILE 4. 1271 1451 105
1271 1451 106
1271 1451 107
MF = 4 SECONDARY ANGULAR DISTRIBUTIONS 1271 1451 108
1271 1451 109
MT=2, ELASTIC. LEGENDRE COEFFICIENTS DETERMINED AS FOLLOWS. 1271 1451 110
BELOW 1.5 MEV, BASED ON THE R-MATRIX ANALYSIS DESCRIBED UNDER 1271 1451 111
MT=1. THESE COEFFICIENTS ARE CONSISTENT WTIH ANGULAR DISTRI- 1271 1451 112
BUTIONS OF LANE (REF.9) AND KNITTER (REF.3). MATCHED BETWEEN 1271 1451 113
1.5 AND 2.5 MEV TO FITS OF THE LANE DATA (REF.9). BETWEEN 1271 1451 114
4.83 AND 7.5 MEV, FIT OF HOPKINS DATA (REF. 7) WAS USED. BASED 1271 1451 115
ON 14-MEV ELASTIC SCATTERING DATA GIVEN IN BNL-400, OPTICAL 1271 1451 116
MODEL CALCULATIONS (ABACUS CODE) WERE USED TO INFER LEGENDRE 1271 1451 117
COEFFICIENTS BETWEEN 10 AND 20 MEV. 1271 1451 118
1271 1451 119
MT = 24, (N,2N)ALPHA-P. EVALUATION OF REF. 1. ISOTROPIC IN 1271 1451 120
LAB SYSTEM. 1271 1451 121
1271 1451 122
MT = 52, (N,N PRIME)GAMMA. TABULATED DISTRIBUTION. ISOTROPIC 1271 1451 123
IN CM SYSTEM. 1271 1451 124
1271 1451 125
MT = 91. (N,N PRIME)ALPHA D. TABULATED DISTRIBUTION (L SYSTEM)1271 1451 126
OF REF. 1. CONTAINS NEUTRONS FROM FIRST LEVEL (DISCRETE) IN 1271 1451 127
LI-6. EXTRAPOLATED TO 20 MEV. 1271 1451 128
1271 1451 129
1271 1451 130
MF = 5 SECONDARY ENERGY DISTRIBUTIONS 1271 1451 131
1271 1451 132
MT = 24, (N,2N)ALPHA D. DISTRIBUTIONS GIVEN IN REF. 1 APPROX- 1271 1451 133
IMATED BY ENDF/B LAW 9 WITH THETA EQUAL 0.21 * SQRT(E). 1271 1451 134
1271 1451 135
MT = 91, (N,N PRIME)ALPHA-D. DISTRIBUTIONS GIVEN IN REF. 1 1271 1451 136
APPROXIMATED BY ENDF/B LAW 9. THETA VALUES OBTAINED BY 1271 1451 137
LINEAR INTERPOLATION BETWEEN FOLLOWING POINTS - - - 1271 1451 138
E = 1.718 MEV, THETA = 0.05 MEV 1271 1451 139
E = 4.1 MEV, THETA = 0.75 MEV 1271 1451 140
E =20.0 MEV, THETA = 8.40 MEV 1271 1451 141
THESE DISTRIBUTIONS CONTAIN ONE DISCRETE LEVEL AND DO NOT 1271 1451 142
ALWAYS CONSERVE ENERGY. 1271 1451 143
1271 1451 144
MF=12 1271 1451 145
1271 1451 146
MT=52. THE FIRST LEVEL IN LI-6 DECAYS BY PARTICLE EMISSION 1271 1451 147
AND IS THEREFORE INCLUDED IN MT=91. THE SECOND LEVEL IS A 1271 1451 148
GAMMA EMITTER THEREFORE THE ENERGY AND MULTIPLICITY WERE TAKEN 1271 1451 149
FROM REFERENCE 1. 1271 1451 150
1271 1451 151
1271 1451 152
MT=102 THE ENERGIES AND TRANSITION ARRAYS FOR RADIATIVE 1271 1451 153
CAPTURE WERE TAKEN FROM REFERENCE 11. NOTE THAT THESE 1271 1451 154
ARE DIFFERENT FROM THOSE ATTACHED TO VERSION III AND 1271 1451 155
PREVIOUSLY CIRCULATED. 1271 1451 156
1271 1451 157
THE LP FLAG WAS USED TO DESCRIBE THE MT=102 PHOTONS 1271 1451 158
1271 1451 159
MF=14 1271 1451 160
1271 1451 161
MT=52 THE GAMMA IS ASSUMED ISOTROPIC. 1271 1451 162
1271 1451 163
MT=102 THE TWO HIGH-ENERGY GAMMAS ARE ASSUMED ISOTROPIC, 1271 1451 164
DATA ON THE 477 KEV GAMMA INDICATE ISOTROPY. 1271 1451 165
1271 1451 166
1271 1451 167
1271 1451 168
REFERENCES 1271 1451 169
1271 1451 170
1. PENDLEBURY, E.D., REPORT AWRE O-60/64. 1271 1451 171
2. DIMENT, K.M., AND UTTLEY, C.A., NUCLEAR PHYSICS DIVISION 1271 1451 172
PROGRESS REPORTS AERE-PR/NP 15 AND AERE-PR/NP 16 (1969). 1271 1451 173
ALSO PRIVATE COMMUNICATION FROM C. A. UTTLEY TO LEONA 1271 1451 174
STEWART. 1271 1451 175
3. H.H. KNITTER AND M. COPPOLA, EUR-3454 (1967). 1271 1451 176
4. FOSTER, D.G.,JR., AND GLASGOW, D.W., HW-73116 AND HW-77311.1271 1451 177
5. PETERSON, J.M., ET AL, PHYS REV 120, 521 (1960). 1271 1451 178
6. HOPKINS, J.C., ET AL, LOS ALAMOS SCI LAB REPORT LA-3765 1271 1451 179
(1967). 1271 1451 180
7. PRESSER, G., ET AL, NUCL PHYS A131, 679 (1969). 1271 1451 181
8. KERN, B.D., AND KREGER, W.E., PHYS REV 112, 926 (1958). 1271 1451 182
9. LANE, R.O., ET AL, ANN PHYS 12, 135 (1961). 1271 1451 183
10. L. ROSEN AND L. STEWART, LA-2643. 1271 1451 184
11. F. AJZENBERG-SELOVE AND T.LAURITZEN, ENERGY LEVELS OF 1271 1451 185
LIGHT NUCLEI, TO BE PUBLISHED. 1271 1451 186
12. S.J. FRIESENHAHN, PRIVATE COMMUNICATION TO P. YOUNG (1974).1271 1451 187
13. E.FORT AND J.P.MARQUETTE, PRIVATE COMMUNICATION TO 1271 1451 188
L.STEWART, (1973). 1271 1451 189
14. M.S.COATES, G.J.HUNT, AND C.A.UTTLEY, PRIVATE COMMUNICA- 1271 1451 190
TION TO L.STEWART, (1973). 1271 1451 191
15. W.P.POENITZ, PRIVATE COMMUNICATION TO L.STEWART, (1973). 1271 1451 192
16. A.ASAMI AND M.C.MOXON, NUCL.DATA FOR REACTORS, HELSINKI, 1271 1451 193
1970, P153. 1271 1451 194
17. R.J.SPIGER AND T.A.TOMBRELLO, PHYS.REV. 163, 964 (1970). 1271 1451 195
18. M.G.SOWERBY ET AL., J.NUCL.ENERGY 24, 323 (1970). 1271 1451 196
19. E.T.JURNEY, LASL, PRIVATE COMMUNICATION, (1973). 1271 1451 197
1271 1451 198
1 451 222 1271 1451 199
2 151 4 1271 1451 200
3 1 62 1271 1451 201
3 2 62 1271 1451 202
3 4 21 1271 1451 203
3 24 11 1271 1451 204
3 52 14 1271 1451 205
3 91 21 1271 1451 206
3 102 5 1271 1451 207
3 103 16 1271 1451 208
3 107 62 1271 1451 209
3 251 26 1271 1451 210
3 252 26 1271 1451 211
3 253 26 1271 1451 212
4 2 179 1271 1451 213
4 24 10 1271 1451 214
4 52 10 1271 1451 215
4 91 100 1271 1451 216
5 24 7 1271 1451 217
5 91 7 1271 1451 218
12 52 4 1271 1451 219
12 102 13 1271 1451 220
14 52 1 1271 1451 221
14 102 1 1271 1451 222
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