endf/b-iv tape 404 (rev. 3)                           1-sept-76   404-0 -0    0
 9.22340+ 4 2.32029+ 2          1          1          0         371043 1451    1
 0.00000+ 0 0.00000+ 0          1          0         40          01043 1451    2
 92-u -234 gga        eval-jan67 drake and nichols                1043 1451    3
 ga-8135 (set,1967)   dist-may74  rev-nov74                       1043 1451    4
 extended to 20 mev for endf/b version-iv   (apr74)               1043 1451    5
 added radioactive decay data (mf=1,mt=457) (apr74)               1043 1451    6
          *          *          *          *          *          *1043 1451    7
 uranium-234 neutron cross sections                               1043 1451    8
 data taken from report by drake and nichols  (ga-8135)           1043 1451    9
                                                                  1043 1451   10
 data modified for endf/b-ii formats (april, 1970)                1043 1451   11
 parameters for negative level changed (april, 1970)              1043 1451   12
          *          *          *          *          *          *1043 1451   13
 mf=1 mt=457 (rad. decay data) eval-feb74 by c.w.reich (anc)      1043 1451   14
 references  q(alpha)- 1973 revision of wapstra-gove mass table.  1043 1451   15
             half-life- n.e. holden, chart of the nuclides (1973) 1043 1451   16
                         and private communication (jan.,1974)    1043 1451   17
             other- y.a. ellis, nuclear data b4, no.6, 581(1970)  1043 1451   18
    note  )e-alpha  = 4840. kev.                                  1043 1451   19
            this value includes the kinetic energies of both the  1043 1451   20
            alpha particle and the recoiling daughter nucleus.    1043 1451   21
    note   the internal-conversion coefficients are theoretical   1043 1451   22
           values. the gamma-ray intensities are derived from     1043 1451   23
           these values, with the requirement that the total      1043 1451   24
           transition intensity agree with that given by the      1043 1451   25
           alpha-particle branching data.                         1043 1451   26
          *          *          *          *          *          *1043 1451   27
                                                                  1043 1451   28
 mf=3 mt=1  total       obtained by adding partial cross sections 1043 1451   29
 mf=3 mt=2  elastic     same as u-238 (ga-6087)                   1043 1451   30
 mf=3 mt=3  nonelastic  sum of (n-2n),(n-3n),(n-g),(n-f),(inel)   1043 1451   31
 mf=3 mt=4  inelastic   from parker (awre 0-37/64)                1043 1451   32
 mf=3 mt=16 (n-2n)      from parker (awre 0-37/64)                1043 1451   33
 mf=3 mt=17 (n-3n)      from parker (awre 0-37/64)                1043 1451   34
 mf=3 mt=18 fission     (ga-8135)                                 1043 1451   35
q-value ref.a.prince,private communication 16apr68                1043 1451   36
 mf=3 mt=102 (n-gamma)  (ga-8135)   also  mt=27 absorption        1043 1451   37
 mf=3 mt=251,252,253 calculated by chad                           1043 1451   38
 mf=4 mt=2  diff elastic(ga-8135)    same as thorium (ga-6404)    1043 1451   39
 mf=5 mt=16             (ga-8135)                                 1043 1451   40
 mf=5 mt=17             (ga-8135)                                 1043 1451   41
 mf=5 mt=18             (ga-8135)                                 1043 1451   42
                                1        451         79           1043 1451   43
                                1        452          3           1043 1451   44
                                1        453          7           1043 1451   45
                                1        457         20           1043 1451   46
                                2        151         33           1043 1451   47
                                3          1         41           1043 1451   48
                                3          2         29           1043 1451   49
                                3          4         22           1043 1451   50
                                3         16         10           1043 1451   51
                                3         17          6           1043 1451   52
                                3         18         29           1043 1451   53
                                3         51         13           1043 1451   54
                                3         52         11           1043 1451   55
                                3         53         10           1043 1451   56
                                3         54          8           1043 1451   57
                                3         55          7           1043 1451   58
                                3         56          6           1043 1451   59
                                3         91         17           1043 1451   60
                                3        102         29           1043 1451   61
                                3        251         31           1043 1451   62
                                3        252         31           1043 1451   63
                                3        253         31           1043 1451   64
                                4          2        279           1043 1451   65
                                4         16         10           1043 1451   66
                                4         17         10           1043 1451   67
                                4         18         10           1043 1451   68
                                4         51         10           1043 1451   69
                                4         52         10           1043 1451   70
                                4         53         10           1043 1451   71
                                4         54         10           1043 1451   72
                                4         55         10           1043 1451   73
                                4         56         10           1043 1451   74
                                4         91         10           1043 1451   75
                                5         16          7           1043 1451   76
                                5         17          7           1043 1451   77
                                5         18          7           1043 1451   78
                                5         91          7           1043 1451   79
                                                                  1043 1  0   80
 9.22340+ 4 2.32029+ 2          0          1          0          01043 1452   81
 0.00000+ 0 0.00000+ 0          0          0          2          01043 1452   82
 2.37000+ 0 1.25000- 7                                            1043 1452   83
                                                                  1043 1  0   84
 9.22340+ 4 2.32029+ 2          0          0          1          01043 1453   85
 9.22340+ 4 2.32029+ 2          0          0          2          21043 1453   86
 1.00000- 5 2.00000+ 7                                            1043 1453   87
 0.00000+ 0-6.77100+ 6          0          0          5          01043 1453   88
 1.60000+ 1 9.22330+ 4 1.35100-12 1.00000+ 0 1.00000+ 0           1043 1453   89
 0.00000+ 0 5.29700+ 6          0          0          5          01043 1453   90
 1.02000+ 2 9.22350+ 4 3.06800-16 1.00000+ 0 1.00000+ 0           1043 1453   91
                                                                  1043 1  0   92
 9.22340+ 4 2.32029+ 2          0          0          0          21043 1457   93
 7.69478+12 3.15360+10          0          0          6          31043 1457   94
 0.00000+ 0 0.00000+ 0 1.48000+ 4 0.00000+ 0 4.84000+ 6 0.00000+ 01043 1457   95
 9.22340+ 4 2.32029+ 2          0          0         12          21043 1457   96
 4.00000+ 0 0.00000+ 0 4.85640+ 6 1.90000+ 3 1.00000+ 0 0.00000+ 01043 1457   97
 6.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 1.00000-11 0.00000+ 01043 1457   98
 4.00000+ 0 0.00000+ 0          0          0         36          51043 1457   99
 1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01043 1457  100
 4.12000+ 6 0.00000+ 0 3.30000- 5 0.00000+ 0 0.00000+ 0 0.00000+ 01043 1457  101
 4.27400+ 6 0.00000+ 0 4.00000- 5 0.00000+ 0 0.00000+ 0 0.00000+ 01043 1457  102
 4.60300+ 6 8.00000+ 3 3.00000- 1 0.00000+ 0 0.00000+ 0 0.00000+ 01043 1457  103
 4.72280+ 6 1.00000+ 3 2.75000+ 1 1.50000+ 0 0.00000+ 0 0.00000+ 01043 1457  104
 4.77300+ 6 2.00000+ 3 7.25000+ 1 3.00000+ 0 0.00000+ 0 0.00000+ 01043 1457  105
 0.00000+ 0 0.00000+ 0          0          0         36          51043 1457  106
 1.17500- 3 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01043 1457  107
 5.31000+ 4 3.00000+ 2 1.00000+ 2 0.00000+ 0 2.32000+ 2 0.00000+ 01043 1457  108
 1.21000+ 5 1.00000+ 3 3.40000+ 1 4.40000+ 0 5.00000+ 0 0.00000+ 01043 1457  109
 4.56000+ 5 0.00000+ 0 1.90000- 2 4.00000- 3 1.50000- 2 0.00000+ 01043 1457  110
 5.08000+ 5 0.00000+ 0 1.50000- 2 4.00000- 3 1.20000- 2 0.00000+ 01043 1457  111
 5.85000+ 5 0.00000+ 0 1.00000- 2 4.00000- 3 2.90000- 2 0.00000+ 01043 1457  112
                                                                  1043 1  0  113
                                                                  1043 0  0  114
 9.22340+ 4 2.32029+ 2          0          0          1          01043 2151  115
 9.22340+ 4 1.00000+ 0          0          0          2          01043 2151  116
 1.00000- 5 3.78000+ 2          1          1          0          01043 2151  117
 0.00000+ 0 8.93000- 1          0          0          1          01043 2151  118
 2.32029+ 2 0.00000+ 0          0          0        126         211043 2151  119
-1.67770+ 0 5.00000- 1 2.82200- 2 3.22000- 3 2.50000- 2 0.00000+ 01043 2151  120
 5.19000+ 0 5.00000- 1 2.91220- 2 4.10000- 3 2.50000- 2 0.00000+ 01043 2151  121
 3.14000+ 1 5.00000- 1 3.27000- 2 7.70000- 3 2.50000- 2 0.00000+ 01043 2151  122
 4.64000+ 1 5.00000- 1 2.50700- 2 7.00000- 5 2.50000- 2 0.00000+ 01043 2151  123
 4.94000+ 1 5.00000- 1 3.60000- 2 1.10000- 2 2.50000- 2 0.00000+ 01043 2151  124
 7.83000+ 1 5.00000- 1 3.14000- 2 6.40000- 3 2.50000- 2 0.00000+ 01043 2151  125
 8.87000+ 1 5.00000- 1 2.59000- 2 9.00000- 4 2.50000- 2 0.00000+ 01043 2151  126
 9.53000+ 1 5.00000- 1 5.30000- 2 2.80000- 2 2.50000- 2 0.00000+ 01043 2151  127
 1.06900+ 2 5.00000- 1 2.81000- 2 3.10000- 3 2.50000- 2 0.00000+ 01043 2151  128
 1.12100+ 2 5.00000- 1 3.80000- 2 1.30000- 2 2.50000- 2 0.00000+ 01043 2151  129
 1.32900+ 2 5.00000- 1 3.90000- 2 1.40000- 2 2.50000- 2 0.00000+ 01043 2151  130
 1.45900+ 2 5.00000- 1 4.20000- 2 1.70000- 2 2.50000- 2 0.00000+ 01043 2151  131
 1.54000+ 2 5.00000- 1 4.40000- 2 1.90000- 2 2.50000- 2 0.00000+ 01043 2151  132
 1.79000+ 2 5.00000- 1 9.50000- 2 7.00000- 2 2.50000- 2 0.00000+ 01043 2151  133
 1.84000+ 2 5.00000- 1 4.50000- 2 2.00000- 2 2.50000- 2 0.00000+ 01043 2151  134
 1.91000+ 2 5.00000- 1 1.35000- 1 1.10000- 1 2.50000- 2 0.00000+ 01043 2151  135
 2.74000+ 2 5.00000- 1 5.10000- 2 2.60000- 2 2.50000- 2 0.00000+ 01043 2151  136
 2.95000+ 2 5.00000- 1 1.05000- 1 8.00000- 2 2.50000- 2 0.00000+ 01043 2151  137
 3.19000+ 2 5.00000- 1 1.35000- 1 1.10000- 1 2.50000- 2 0.00000+ 01043 2151  138
 3.57000+ 2 5.00000- 1 5.50000- 2 3.00000- 2 2.50000- 2 0.00000+ 01043 2151  139
 3.69000+ 2 5.00000- 1 2.45000- 1 2.20000- 1 2.50000- 2 0.00000+ 01043 2151  140
 3.78000+ 2 1.00000+ 3          2          1          0          01043 2151  141
 0.00000+ 0 8.93000- 1          0          0          2          01043 2151  142
 2.32029+ 2 0.00000+ 0          0          0          6          11043 2151  143
 1.60000+ 1 5.00000- 1 1.00000+ 0 2.16000- 3 2.50000- 2 0.00000+ 01043 2151  144
 2.32029+ 2 0.00000+ 0          1          0         12          21043 2151  145
 1.60000+ 1 5.00000- 1 1.00000+ 0 1.60000- 3 2.50000- 2 0.00000+ 01043 2151  146
 8.00000+ 0 1.50000+ 0 1.00000+ 0 1.20000- 3 2.50000- 2 0.00000+ 01043 2151  147
                                                                  1043 2  0  148
                                                                  1043 0  0  149
 9.22340+ 4 2.32029+ 2          0         99          0          01043 3  1  150
 0.00000+ 0 0.00000+ 0          0          0          1        1131043 3  1  151
        113          2                                            1043 3  1  152
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 1.20000+ 3 1.99700+ 1 1.40000+ 3 1.92100+ 1 1.60000+ 3 1.83010+ 11043 3  1  154
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 4.50000+ 3 1.58380+ 1 5.00000+ 3 1.58090+ 1 6.00000+ 3 1.57500+ 11043 3  1  157
 7.00000+ 3 1.56000+ 1 8.00000+ 3 1.54700+ 1 9.00000+ 3 1.53500+ 11043 3  1  158
 1.00000+ 4 1.52400+ 1 1.20000+ 4 1.50850+ 1 1.40000+ 4 1.49300+ 11043 3  1  159
 1.50000+ 4 1.48520+ 1 1.60000+ 4 1.47840+ 1 1.80000+ 4 1.46470+ 11043 3  1  160
 2.00000+ 4 1.45110+ 1 2.20000+ 4 1.43150+ 1 2.40000+ 4 1.41180+ 11043 3  1  161
 2.50000+ 4 1.40200+ 1 2.60000+ 4 1.39680+ 1 2.80000+ 4 1.38630+ 11043 3  1  162
 3.00000+ 4 1.37580+ 1 3.50000+ 4 1.35670+ 1 4.00000+ 4 1.33760+ 11043 3  1  163
 4.43000+ 4 1.32000+ 1 4.50000+ 4 1.31780+ 1 5.00000+ 4 1.30180+ 11043 3  1  164
 5.50000+ 4 1.29190+ 1 6.00000+ 4 1.28190+ 1 6.50000+ 4 1.27260+ 11043 3  1  165
 7.00000+ 4 1.26330+ 1 7.50000+ 4 1.25810+ 1 8.00000+ 4 1.25300+ 11043 3  1  166
 8.50000+ 4 1.24520+ 1 9.00000+ 4 1.23750+ 1 9.50000+ 4 1.23740+ 11043 3  1  167
 1.00000+ 5 1.23740+ 1 1.20000+ 5 1.21191+ 1 1.40000+ 5 1.18642+ 11043 3  1  168
 1.45000+ 5 1.18005+ 1 1.50000+ 5 1.17490+ 1 1.60000+ 5 1.16660+ 11043 3  1  169
 1.80000+ 5 1.14990+ 1 2.00000+ 5 1.13330+ 1 2.20000+ 5 1.11610+ 11043 3  1  170
 2.40000+ 5 1.09900+ 1 2.50000+ 5 1.09040+ 1 2.60000+ 5 1.08320+ 11043 3  1  171
 2.80000+ 5 1.06880+ 1 3.00000+ 5 1.05440+ 1 3.50000+ 5 1.02380+ 11043 3  1  172
 4.00000+ 5 9.93300+ 0 4.50000+ 5 9.62100+ 0 5.00000+ 5 9.30900+ 01043 3  1  173
 5.50000+ 5 9.07550+ 0 6.00000+ 5 8.84200+ 0 6.50000+ 5 8.73450+ 01043 3  1  174
 7.00000+ 5 8.62700+ 0 7.50000+ 5 8.38550+ 0 8.00000+ 5 8.14400+ 01043 3  1  175
 8.05000+ 5 8.12570+ 0 8.50000+ 5 8.07790+ 0 9.00000+ 5 8.00900+ 01043 3  1  176
 9.50000+ 5 7.99500+ 0 1.00000+ 6 7.98500+ 0 1.04000+ 6 7.96500+ 01043 3  1  177
 1.20000+ 6 7.88000+ 0 1.40000+ 6 7.84000+ 0 1.60000+ 6 7.98300+ 01043 3  1  178
 1.80000+ 6 8.14100+ 0 2.00000+ 6 8.22900+ 0 2.20000+ 6 8.19800+ 01043 3  1  179
 2.40000+ 6 8.16100+ 0 2.60000+ 6 8.14200+ 0 2.80000+ 6 8.18900+ 01043 3  1  180
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 4.50000+ 6 8.10800+ 0 5.00000+ 6 8.06000+ 0 5.50000+ 6 7.90400+ 01043 3  1  182
 6.00000+ 6 7.60600+ 0 6.50000+ 6 7.29400+ 0 6.81800+ 6 7.05200+ 01043 3  1  183
 6.81840+ 6 7.05170+ 0 7.00000+ 6 6.92400+ 0 7.50000+ 6 6.50200+ 01043 3  1  184
 8.00000+ 6 6.12900+ 0 8.50000+ 6 5.99000+ 0 9.00000+ 6 5.89800+ 01043 3  1  185
 9.50000+ 6 5.78100+ 0 1.00000+ 7 5.64500+ 0 1.05000+ 7 5.52700+ 01043 3  1  186
 1.10000+ 7 5.43000+ 0 1.15000+ 7 5.40900+ 0 1.20000+ 7 5.39900+ 01043 3  1  187
 1.25000+ 7 5.36300+ 0 1.27300+ 7 5.34390+ 0 1.30000+ 7 5.34200+ 01043 3  1  188
 1.35000+ 7 5.36000+ 0 1.40000+ 7 5.38300+ 0 1.45000+ 7 5.51200+ 01043 3  1  189
 1.50000+ 7 5.42700+ 0 2.00000+ 7 5.68207+ 0                      1043 3  1  190
                                                                  1043 3  0  191
 9.22340+ 4 2.32029+ 2          0         99          0          01043 3  2  192
 0.00000+ 0 0.00000+ 0          0          0          1         761043 3  2  193
         76          2                                            1043 3  2  194
 1.00000- 5 0.00000+ 0 1.00000+ 3 0.00000+ 0 1.00000+ 3 1.73000+ 11043 3  2  195
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 1.80000+ 3 1.51000+ 1 2.00000+ 3 1.49000+ 1 2.50000+ 3 1.44000+ 11043 3  2  197
 3.00000+ 3 1.42000+ 1 3.50000+ 3 1.41500+ 1 4.00000+ 3 1.41500+ 11043 3  2  198
 4.50000+ 3 1.42000+ 1 5.00000+ 3 1.42500+ 1 6.00000+ 3 1.43000+ 11043 3  2  199
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 1.00000+ 4 1.41000+ 1 1.50000+ 4 1.39000+ 1 2.00000+ 4 1.37000+ 11043 3  2  201
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 8.00000+ 4 1.17530+ 1 9.00000+ 4 1.14870+ 1 1.00000+ 5 1.13290+ 11043 3  2  204
 1.50000+ 5 1.03500+ 1 2.00000+ 5 9.74700+ 0 2.50000+ 5 9.25400+ 01043 3  2  205
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 2.60000+ 6 4.45200+ 0 2.80000+ 6 4.52000+ 0 3.00000+ 6 4.57000+ 01043 3  2  211
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 1.25000+ 7 2.79000+ 0 1.30000+ 7 2.76000+ 0 1.35000+ 7 2.77000+ 01043 3  2  218
 1.40000+ 7 2.78000+ 0 1.45000+ 7 2.89000+ 0 1.50000+ 7 2.80000+ 01043 3  2  219
 2.00000+ 7 3.07687+ 0                                            1043 3  2  220
                                                                  1043 3  0  221
 9.22340+ 4 2.32029+ 2          0         99          0          01043 3  4  222
 0.00000+ 0-4.40000+ 4          0          0          1         561043 3  4  223
         56          2                                            1043 3  4  224
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 1.45000+ 5 1.00000+ 0 1.50000+ 5 1.05000+ 0 2.00000+ 5 1.25000+ 01043 3  4  227
 2.50000+ 5 1.31000+ 0 3.00000+ 5 1.40000+ 0 4.00000+ 5 1.44700+ 01043 3  4  228
 5.00000+ 5 1.35000+ 0 6.00000+ 5 1.27600+ 0 7.00000+ 5 1.19000+ 01043 3  4  229
 8.00000+ 5 1.05000+ 0 8.05000+ 5 1.05100+ 0 9.00000+ 5 1.30000+ 01043 3  4  230
 9.50000+ 5 1.42000+ 0 1.00000+ 6 1.55000+ 0 1.04000+ 6 1.60000+ 01043 3  4  231
 1.20000+ 6 1.81000+ 0 1.40000+ 6 1.97000+ 0 1.60000+ 6 2.06000+ 01043 3  4  232
 1.80000+ 6 2.13000+ 0 2.00000+ 6 2.18000+ 0 2.20000+ 6 2.19000+ 01043 3  4  233
 2.40000+ 6 2.20000+ 0 2.60000+ 6 2.21000+ 0 2.80000+ 6 2.21000+ 01043 3  4  234
 3.00000+ 6 2.19000+ 0 3.50000+ 6 2.18000+ 0 4.00000+ 6 2.14000+ 01043 3  4  235
 4.50000+ 6 2.21000+ 0 5.00000+ 6 2.27000+ 0 5.50000+ 6 2.26000+ 01043 3  4  236
 6.00000+ 6 2.15000+ 0 6.50000+ 6 1.85000+ 0 7.00000+ 6 1.45000+ 01043 3  4  237
 7.50000+ 6 1.08000+ 0 8.00000+ 6 8.00000- 1 8.50000+ 6 6.65000- 11043 3  4  238
 9.00000+ 6 5.90000- 1 9.50000+ 6 5.50000- 1 1.00000+ 7 5.10000- 11043 3  4  239
 1.05000+ 7 4.75000- 1 1.10000+ 7 4.55000- 1 1.15000+ 7 4.35000- 11043 3  4  240
 1.20000+ 7 3.95000- 1 1.25000+ 7 2.65000- 1 1.30000+ 7 2.10000- 11043 3  4  241
 1.35000+ 7 1.74000- 1 1.40000+ 7 1.50000- 1 1.45000+ 7 1.49000- 11043 3  4  242
 1.50000+ 7 1.49000- 1 2.00000+ 7 1.49000- 1                      1043 3  4  243
                                                                  1043 3  0  244
 9.22340+ 4 2.32029+ 2          0         99          0          01043 3 16  245
 0.00000+ 0-6.77100+ 6          0          0          1         191043 3 16  246
         19          2                                            1043 3 16  247
 6.81840+ 6 0.00000+ 0 7.00000+ 6 1.00000- 2 7.50000+ 6 4.00000- 21043 3 16  248
 8.00000+ 6 8.00000- 2 8.50000+ 6 1.40000- 1 9.00000+ 6 2.20000- 11043 3 16  249
 9.50000+ 6 2.60000- 1 1.00000+ 7 3.06000- 1 1.05000+ 7 3.10000- 11043 3 16  250
 1.10000+ 7 3.13000- 1 1.15000+ 7 3.24000- 1 1.20000+ 7 3.84000- 11043 3 16  251
 1.25000+ 7 4.83000- 1 1.30000+ 7 5.03000- 1 1.35000+ 7 4.72000- 11043 3 16  252
 1.40000+ 7 3.82000- 1 1.45000+ 7 2.82000- 1 1.50000+ 7 2.02000- 11043 3 16  253
 2.00000+ 7 2.02000- 1                                            1043 3 16  254
                                                                  1043 3  0  255
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 1.22600- 1 6.86000- 2 2.17000- 2 1.06000- 2 3.00000- 4           1043 4  2  723
 0.00000+ 0 5.50000+ 6          0          0         12          01043 4  2  724
 7.38400- 1 6.18500- 1 5.21500- 1 4.38100- 1 3.31600- 1 2.15600- 11043 4  2  725
 1.38800- 1 8.29000- 2 2.98000- 2 1.52000- 2 2.10000- 3 1.00000- 31043 4  2  726
 0.00000+ 0 6.00000+ 6          0          0         12          01043 4  2  727
 7.34600- 1 6.18000- 1 5.28000- 1 4.46400- 1 3.45400- 1 2.33100- 11043 4  2  728
 1.55300- 1 9.73000- 2 3.78000- 2 1.98000- 2 4.20000- 3 2.10000- 31043 4  2  729
 0.00000+ 0 6.50000+ 6          0          0         13          01043 4  2  730
 7.30800- 1 6.17500- 1 5.34500- 1 4.54800- 1 3.59200- 1 2.50600- 11043 4  2  731
 1.71600- 1 1.11500- 1 4.58000- 2 2.44000- 2 6.30000- 3 3.10000- 31043 4  2  732
 1.00000- 4                                                       1043 4  2  733
 0.00000+ 0 7.00000+ 6          0          0         13          01043 4  2  734
 7.27000- 1 6.17000- 1 5.41000- 1 4.63000- 1 3.73000- 1 2.68000- 11043 4  2  735
 1.88000- 1 1.26000- 1 5.39000- 2 2.89000- 2 8.50000- 3 4.20000- 31043 4  2  736
 2.00000- 4                                                       1043 4  2  737
 0.00000+ 0 7.50000+ 6          0          0         14          01043 4  2  738
 7.15000- 1 6.02000- 1 5.34000- 1 4.58000- 1 3.67000- 1 2.68000- 11043 4  2  739
 1.86000- 1 1.28000- 1 6.38000- 2 3.82000- 2 1.29000- 2 6.00000- 31043 4  2  740
 5.00000- 4 0.00000+ 0                                            1043 4  2  741
 0.00000+ 0 8.00000+ 6          0          0         14          01043 4  2  742
 7.00000- 1 5.89000- 1 5.22000- 1 4.48000- 1 3.57000- 1 2.65000- 11043 4  2  743
 1.81000- 1 1.28000- 1 7.30000- 2 4.80000- 2 1.88000- 2 7.80000- 31043 4  2  744
 1.40000- 3 2.00000- 4                                            1043 4  2  745
 0.00000+ 0 9.00000+ 6          0          0         14          01043 4  2  746
 6.71000- 1 5.56000- 1 4.84000- 1 4.19000- 1 3.36000- 1 2.54000- 11043 4  2  747
 1.73000- 1 1.27000- 1 9.30000- 2 7.00000- 2 3.40000- 2 1.33000- 21043 4  2  748
 3.30000- 3 1.40000- 3                                            1043 4  2  749
 0.00000+ 0 1.00000+ 7          0          0         14          01043 4  2  750
 6.43000- 1 5.16000- 1 4.34000- 1 3.87000- 1 3.15000- 1 2.46000- 11043 4  2  751
 1.75000- 1 1.30000- 1 1.13500- 1 9.52000- 2 5.44000- 2 2.25000- 21043 4  2  752
 6.80000- 3 3.20000- 3                                            1043 4  2  753
 0.00000+ 0 1.10000+ 7          0          0         15          01043 4  2  754
 6.20000- 1 4.75000- 1 3.90000- 1 3.54000- 1 2.92000- 1 2.42000- 11043 4  2  755
 1.87000- 1 1.45000- 1 1.34800- 1 1.22400- 1 7.93000- 2 3.55000- 21043 4  2  756
 1.32000- 2 5.40000- 3 0.00000+ 0                                 1043 4  2  757
 0.00000+ 0 1.20000+ 7          0          0         15          01043 4  2  758
 6.05000- 1 4.40000- 1 3.56000- 1 3.18000- 1 2.75000- 1 2.37000- 11043 4  2  759
 1.97000- 1 1.64000- 1 1.54800- 1 1.45300- 1 1.05100- 1 5.18000- 21043 4  2  760
 2.17000- 2 7.70000- 3 1.10000- 3                                 1043 4  2  761
 0.00000+ 0 1.30000+ 7          0          0         15          01043 4  2  762
 6.06000- 1 4.37000- 1 3.36000- 1 3.00000- 1 2.61000- 1 2.32000- 11043 4  2  763
 2.04000- 1 1.82000- 1 1.72000- 1 1.61700- 1 1.26700- 1 7.04000- 21043 4  2  764
 3.28000- 2 1.10000- 2 3.00000- 3                                 1043 4  2  765
 0.00000+ 0 1.40000+ 7          0          0         15          01043 4  2  766
 6.23000- 1 4.53000- 1 3.43000- 1 3.02000- 1 2.65000- 1 2.35000- 11043 4  2  767
 2.16000- 1 1.96000- 1 1.85000- 1 1.74900- 1 1.45000- 1 8.81000- 21043 4  2  768
 4.50000- 2 1.60000- 2 4.80000- 3                                 1043 4  2  769
 0.00000+ 0 1.50000+ 7          0          0         15          01043 4  2  770
 6.42000- 1 4.81000- 1 3.62000- 1 3.20000- 1 2.88000- 1 2.54000- 11043 4  2  771
 2.29000- 1 2.11000- 1 1.96000- 1 1.84000- 1 1.57000- 1 1.04000- 11043 4  2  772
 5.60000- 2 2.20000- 2 7.00000- 3                                 1043 4  2  773
 0.00000+ 0 2.00000+ 7          0          0         15          01043 4  2  774
 6.42000- 1 4.81000- 1 3.62000- 1 3.20000- 1 2.88000- 1 2.54000- 11043 4  2  775
 2.29000- 1 2.11000- 1 1.96000- 1 1.84000- 1 1.57000- 1 1.04000- 11043 4  2  776
 5.60000- 2 2.20000- 2 7.00000- 3                                 1043 4  2  777
                                                                  1043 4  0  778
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 16  779
 0.00000+ 0 2.32029+ 2          0          1          0          01043 4 16  780
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 16  781
          2          2                                            1043 4 16  782
 0.00000+ 0 6.81840+ 6          0          0          1          21043 4 16  783
          2          2                                            1043 4 16  784
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 16  785
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 16  786
          2          2                                            1043 4 16  787
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 16  788
                                                                  1043 4  0  789
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 17  790
 0.00000+ 0 2.32029+ 2          0          1          0          01043 4 17  791
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 17  792
          2          2                                            1043 4 17  793
 0.00000+ 0 1.27300+ 7          0          0          1          21043 4 17  794
          2          2                                            1043 4 17  795
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 17  796
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 17  797
          2          2                                            1043 4 17  798
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 17  799
                                                                  1043 4  0  800
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 18  801
 0.00000+ 0 2.32029+ 2          0          1          0          01043 4 18  802
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 18  803
          2          2                                            1043 4 18  804
 0.00000+ 0 1.00000- 5          0          0          1          21043 4 18  805
          2          2                                            1043 4 18  806
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 18  807
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 18  808
          2          2                                            1043 4 18  809
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 18  810
                                                                  1043 4  0  811
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 51  812
 0.00000+ 0 2.32029+ 2          0          2          0          01043 4 51  813
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 51  814
          2          2                                            1043 4 51  815
 0.00000+ 0 4.43000+ 4          0          0          1          21043 4 51  816
          2          2                                            1043 4 51  817
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 51  818
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 51  819
          2          2                                            1043 4 51  820
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 51  821
                                                                  1043 4  0  822
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 52  823
 0.00000+ 0 2.32029+ 2          0          2          0          01043 4 52  824
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 52  825
          2          2                                            1043 4 52  826
 0.00000+ 0 1.45000+ 5          0          0          1          21043 4 52  827
          2          2                                            1043 4 52  828
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 52  829
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 52  830
          2          2                                            1043 4 52  831
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 52  832
                                                                  1043 4  0  833
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 53  834
 0.00000+ 0 2.32029+ 2          0          2          0          01043 4 53  835
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 53  836
          2          2                                            1043 4 53  837
 0.00000+ 0 3.00000+ 5          0          0          1          21043 4 53  838
          2          2                                            1043 4 53  839
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 53  840
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 53  841
          2          2                                            1043 4 53  842
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 53  843
                                                                  1043 4  0  844
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 54  845
 0.00000+ 0 2.32029+ 2          0          2          0          01043 4 54  846
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 54  847
          2          2                                            1043 4 54  848
 0.00000+ 0 8.05000+ 5          0          0          1          21043 4 54  849
          2          2                                            1043 4 54  850
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 54  851
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 54  852
          2          2                                            1043 4 54  853
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 54  854
                                                                  1043 4  0  855
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 55  856
 0.00000+ 0 2.32029+ 2          0          2          0          01043 4 55  857
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 55  858
          2          2                                            1043 4 55  859
 0.00000+ 0 9.50000+ 5          0          0          1          21043 4 55  860
          2          2                                            1043 4 55  861
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 55  862
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 55  863
          2          2                                            1043 4 55  864
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 55  865
                                                                  1043 4  0  866
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 56  867
 0.00000+ 0 2.32029+ 2          0          2          0          01043 4 56  868
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 56  869
          2          2                                            1043 4 56  870
 0.00000+ 0 1.04000+ 6          0          0          1          21043 4 56  871
          2          2                                            1043 4 56  872
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 56  873
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 56  874
          2          2                                            1043 4 56  875
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 56  876
                                                                  1043 4  0  877
 9.22340+ 4 2.32029+ 2          0          2          0          01043 4 91  878
 0.00000+ 0 2.32029+ 2          0          2          0          01043 4 91  879
 0.00000+ 0 0.00000+ 0          0          0          1          21043 4 91  880
          2          2                                            1043 4 91  881
 0.00000+ 0 9.00000+ 5          0          0          1          21043 4 91  882
          2          2                                            1043 4 91  883
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 91  884
 0.00000+ 0 2.00000+ 7          0          0          1          21043 4 91  885
          2          2                                            1043 4 91  886
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1043 4 91  887
                                                                  1043 4  0  888
                                                                  1043 0  0  889
 9.22340+ 4 2.32029+ 2          0          0          1          01043 5 16  890
 6.81840+ 6 0.00000+ 0          0          9          1          21043 5 16  891
          2          2                                            1043 5 16  892
 6.81840+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1043 5 16  893
 0.00000+ 0 0.00000+ 0          0          0          1          31043 5 16  894
          3          5                                            1043 5 16  895
 6.81840+ 6 1.43900+ 5 1.50000+ 7 7.90600+ 5 2.00000+ 7 1.47208+ 61043 5 16  896
                                                                  1043 5  0  897
 9.22340+ 4 2.32029+ 2          0          0          1          01043 5 17  898
 1.27300+ 7 0.00000+ 0          0          9          1          21043 5 17  899
          2          2                                            1043 5 17  900
 1.27300+ 7 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1043 5 17  901
 0.00000+ 0 0.00000+ 0          0          0          1          31043 5 17  902
          3          5                                            1043 5 17  903
 5.00000+ 5 1.38600+ 5 1.50000+ 7 7.59000+ 5 2.00000+ 7 8.76404+ 51043 5 17  904
                                                                  1043 5  0  905
 9.22340+ 4 2.32029+ 2          0          0          1          01043 5 18  906
-3.00000+ 7 0.00000+ 0          0          7          1          21043 5 18  907
          2          2                                            1043 5 18  908
 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1043 5 18  909
 0.00000+ 0 0.00000+ 0          0          0          1          31043 5 18  910
          3          5                                            1043 5 18  911
 1.00000- 5 1.29550+ 6 1.50000+ 7 1.49230+ 6 2.00000+ 7 1.49447+ 61043 5 18  912
                                                                  1043 5  0  913
 9.22340+ 4 2.32029+ 2          0          0          1          01043 5 91  914
 4.43000+ 4 0.00000+ 0          0          9          1          21043 5 91  915
          2          2                                            1043 5 91  916
 9.00000+ 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1043 5 91  917
 0.00000+ 0 0.00000+ 0          0          0          1          31043 5 91  918
          3          5                                            1043 5 91  919
 9.00000+ 5 1.50700+ 5 1.50000+ 7 8.25700+ 5 2.00000+ 7 9.82558+ 51043 5 91  920
                                                                  1043 5  0  921
                                                                  1043 0  0  922
                                                                     0 0  0  923
 9.42380+ 4 2.36167+ 2          1          1          0         431050 1451    1
 0.00000+ 0 0.00000+ 0          1          0        101          01050 1451    2
 94-pu-238 ai         eval-may67 alter and dunford                1050 1451    3
 naa-sr-12271(may,67) dist-may74  rev-nov74                       1050 1451    4
 extended to 20 mev for endf/b version-iv   (apr74)               1050 1451    5
 added radioactive decay data (mf=1,mt=457) (apr74)               1050 1451    6
 *         *          *          *         *          *           1050 1451    7
  data modified for endf/b-ii formats (april 1970)                1050 1451    8
 *         *          *          *         *          *           1050 1451    9
      plutonium-238   revised july 14,1967                        1050 1451   10
                                                                  1050 1451   11
  evaluated by atomics international                              1050 1451   12
  documentation - naa-sr-12271  may 1,1967 + supp. 1, july 14,19671050 1451   13
                                                                  1050 1451   14
  mf=1                general information                         1050 1451   15
    mt=452 nubar   no experimental data available. correlation of 1050 1451   16
       reference 1 is used.                                       1050 1451   17
    mt=453 branching ratio data     all masses and decay constants1050 1451   18
       from ref. 2.                                               1050 1451   19
          *          *          *          *          *          *1050 1451   20
   mt=457 (rad. decay data) eval-feb74 by c.w.reich (anc)         1050 1451   21
             q(alpha)- 1973 revision of wapstra-gove mass table   1050 1451   22
             half-life- n.e. holden, chart of the nuclides (1973) 1050 1451   23
                         and private communication (jan., 1974).  1050 1451   24
             other- y.a. ellis, nuclear data b 4, no.6, 635(1970).1050 1451   25
    note  )e-alpha  = 5576. kev.                                  1050 1451   26
            this value includes the kinetic energy of the alpha   1050 1451   27
            particle and the recoil energy of the daughter nucleus1050 1451   28
          *          *          *          *          *          *1050 1451   29
                                                                  1050 1451   30
  mf=2                resonance parameters                        1050 1451   31
    mt=151 resolved resonances   parameters for 14 single-level   1050 1451   32
       resonances are given (ref. 3). fission widths deduced from 1050 1451   33
       data of ref. 4. potential scattering of 10.89 barns based  1050 1451   34
       on deformed optical model.                                 1050 1451   35
           unresolved resonances   average resonance parameters   1050 1451   36
       obtained from resolved resonances and deformed optical     1050 1451   37
       model.                                                     1050 1451   38
           this data gives a resonance integral of 169.1 barns in 1050 1451   39
       good agreement with 160 barns measured (ref. 5).           1050 1451   40
                                                                  1050 1451   41
  mf=3                smooth cross sections                       1050 1451   42
    mt=1   total cross section   thermal region obtained from     1050 1451   43
       resonance parameters. 2200m/s value 583.47b compared to    1050 1451   44
       590 reported in ref. 6. fast region from deformed optical  1050 1451   45
       model(dom).                                                1050 1451   46
    mt=2   elastic scattering   data obtained in procedure        1050 1451   47
       idenical to mt=1.                                          1050 1451   48
    mt=4   inelastic scattering   data results from the scattering1050 1451   49
       to  9 levels plus continuum. again a dom is used with a    1050 1451   50
       statistical compound nucleus model.                        1050 1451   51
    mt=16  n,2n   calculation based on evaporation model (ref. 7).1050 1451   52
    mt=17  n,3n   same as mt=16                                   1050 1451   53
    mt=18  fission   thermal region data calculated from resonance1050 1451   54
       parameters. 2200m/s value is 16.29b compared to the        1050 1451   55
       measured value of 16.6b (ref. 8). fast region data         1050 1451   56
       calculated from compound nucleus theory using the hill-    1050 1451   57
       wheeler model(ref. 9). data agrees with recent measurements1050 1451   58
       from lasl(ref. 10), but are 20 percent lower than earlier  1050 1451   59
       measurements at 1.0 mev(ref. 11).                          1050 1451   60
    mt=102 capture   thermal data calculated from resonance       1050 1451   61
       parameters. 2200m/s value is 546.5b. fast region data from 1050 1451   62
       a statistical model assuming dipole radiation.             1050 1451   63
    mt=251 mubar   calculated from dom angular distributions      1050 1451   64
    mt=252 xibar   calculated from dom angular distributions      1050 1451   65
    mt=253 gamma   calculated from dom angular distributions      1050 1451   66
                                                                  1050 1451   67
  mf=4                legendre polynomials                        1050 1451   68
    mt=2   elastic scattering   legendre coefficints for 15th     1050 1451   69
       order fit to calculated angular distributions (dom) are    1050 1451   70
       provided between 10 kev and 11 mev and 19th order between  1050 1451   71
       12 and 15 mev.                                             1050 1451   72
                                                                  1050 1451   73
  mf=5                secondary energy distributions              1050 1451   74
    mt=2   inelastic scattering   calculated data for 9 levels    1050 1451   75
       plus continuum. direct scattering for the first excited    1050 1451   76
       level from threshold to 15mev plus compound nucleus        1050 1451   77
       scattering to 3 mev for all levels is included. continuum  1050 1451   78
       inelastic scattering is given by a maxwellian with an      1050 1451   79
       energy dependent temperature calculated from ref. 7.       1050 1451   80
    mt=16  n,2n   nuclear temperature with energy dependence as in1050 1451   81
       reference 12.                                              1050 1451   82
    mt=17  n,3n   nuclear temperature with energy dependence as in1050 1451   83
       reference 12.                                              1050 1451   84
    mt=18  fission   maxwellian with constant temperature from    1050 1451   85
       correlation of ref. 13.                                    1050 1451   86
                                                                  1050 1451   87
                                                                  1050 1451   88
                      references                                  1050 1451   89
    1.  shuster, s., howerton, r., ucrl 7389(1963)                1050 1451   90
    2.  goldman, d., roesser, j.,  chart of the nuclides (1966)   1050 1451   91
    3.  young, t., in-10266 (to be published)                     1050 1451   92
    4.  stubbins, w., et.al., ucrl-70033(1966)                    1050 1451   93
    5.  hellstrand, e., private communication (1966)              1050 1451   94
    6.  young, t., wash 1068(1966)                                1050 1451   95
    7.  pearlstein, s., bnl 897(1964)                             1050 1451   96
    8.  hulet, e., et.al., phys.rev. 107,1294(1957)               1050 1451   97
    9.  hill, d., wheeler, j., phys.rev. 89,1102(1953)            1050 1451   98
   10.  barton, d., private communication (1966)                  1050 1451   99
   11.  butler, d., sjoblom, r., bull.am.phys.soc. 8,359(1963)    1050 1451  100
   12.  parker, k., awre0-79/63(1964)                             1050 1451  101
   13.  barnard, e., et.al., nucl.phys. 71,228(1965)              1050 1451  102
                                                                  1050 1451  103
                                1        451        146           1050 1451  104
                                1        452          3           1050 1451  105
                                1        453          7           1050 1451  106
                                1        457         49           1050 1451  107
                                2        151         33           1050 1451  108
                                3          1         35           1050 1451  109
                                3          2         28           1050 1451  110
                                3          4         23           1050 1451  111
                                3         16          7           1050 1451  112
                                3         17          5           1050 1451  113
                                3         18         28           1050 1451  114
                                3         51         23           1050 1451  115
                                3         52         17           1050 1451  116
                                3         53         13           1050 1451  117
                                3         54         12           1050 1451  118
                                3         55         11           1050 1451  119
                                3         56         10           1050 1451  120
                                3         57          9           1050 1451  121
                                3         58          9           1050 1451  122
                                3         59          8           1050 1451  123
                                3         91         11           1050 1451  124
                                3        102         28           1050 1451  125
                                3        251         16           1050 1451  126
                                3        252         16           1050 1451  127
                                3        253         16           1050 1451  128
                                4          2        235           1050 1451  129
                                4         16         10           1050 1451  130
                                4         17         10           1050 1451  131
                                4         18         10           1050 1451  132
                                4         51         10           1050 1451  133
                                4         52         10           1050 1451  134
                                4         53         10           1050 1451  135
                                4         54         10           1050 1451  136
                                4         55         10           1050 1451  137
                                4         56         10           1050 1451  138
                                4         57         10           1050 1451  139
                                4         58         10           1050 1451  140
                                4         59         10           1050 1451  141
                                4         91         10           1050 1451  142
                                5         16         10           1050 1451  143
                                5         17          8           1050 1451  144
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 3.71045- 5                                                       1050 4  2  806
 0.00000+ 0 1.30000+ 7          0          0         19          01050 4  2  807
 8.81994- 1 7.67000- 1 6.61424- 1 5.79914- 1 5.08502- 1 4.50386- 11050 4  2  808
 3.91815- 1 3.41733- 1 2.89033- 1 2.41959- 1 1.83680- 1 1.18056- 11050 4  2  809
 6.12191- 2 2.74426- 2 1.04826- 2 3.34360- 3 1.03710- 3 2.34373- 41050 4  2  810
 7.89974- 5                                                       1050 4  2  811
 0.00000+ 0 1.40000+ 7          0          0         19          01050 4  2  812
 8.93028- 1 7.85960- 1 6.79907- 1 5.96216- 1 5.22482- 1 4.63968- 11050 4  2  813
 4.05898- 1 3.57014- 1 3.04404- 1 2.56160- 1 1.99546- 1 1.35544- 11050 4  2  814
 7.64085- 2 3.79461- 2 1.63050- 2 5.96524- 3 2.01317- 3 5.12093- 41050 4  2  815
 1.72784- 4                                                       1050 4  2  816
 0.00000+ 0 1.50000+ 7          0          0         19          01050 4  2  817
 9.04608- 1 8.07801- 1 7.04135- 1 6.19719- 1 5.42609- 1 4.81675- 11050 4  2  818
 4.22251- 1 3.72276- 1 3.19048- 1 2.69160- 1 2.13370- 1 1.51736- 11050 4  2  819
 9.20153- 2 5.02540- 2 2.40844- 2 9.94113- 3 3.63661- 3 1.05740- 31050 4  2  820
 3.66789- 4                                                       1050 4  2  821
 0.00000+ 0 2.00000+ 7          0          0         19          01050 4  2  822
 9.04608- 1 8.07801- 1 7.04135- 1 6.19719- 1 5.42609- 1 4.81675- 11050 4  2  823
 4.22251- 1 3.72276- 1 3.19048- 1 2.69160- 1 2.13370- 1 1.51736- 11050 4  2  824
 9.20153- 2 5.02540- 2 2.40844- 2 9.94113- 3 3.63661- 3 1.05740- 31050 4  2  825
 3.66789- 4                                                       1050 4  2  826
                                                                  1050 4  0  827
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 16  828
 0.00000+ 0 2.36167+ 2          0          1          0          01050 4 16  829
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 16  830
          2          2                                            1050 4 16  831
 0.00000+ 0 6.97000+ 6          0          0          1          21050 4 16  832
          2          2                                            1050 4 16  833
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 16  834
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 16  835
          2          2                                            1050 4 16  836
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 16  837
                                                                  1050 4  0  838
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 17  839
 0.00000+ 0 2.36167+ 2          0          1          0          01050 4 17  840
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 17  841
          2          2                                            1050 4 17  842
 0.00000+ 0 1.29700+ 7          0          0          1          21050 4 17  843
          2          2                                            1050 4 17  844
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 17  845
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 17  846
          2          2                                            1050 4 17  847
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 17  848
                                                                  1050 4  0  849
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 18  850
 0.00000+ 0 2.36167+ 2          0          1          0          01050 4 18  851
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 18  852
          2          2                                            1050 4 18  853
 0.00000+ 0 1.00000- 5          0          0          1          21050 4 18  854
          2          2                                            1050 4 18  855
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 18  856
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 18  857
          2          2                                            1050 4 18  858
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 18  859
                                                                  1050 4  0  860
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 51  861
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 51  862
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 51  863
          2          2                                            1050 4 51  864
 0.00000+ 0 4.43000+ 4          0          0          1          21050 4 51  865
          2          2                                            1050 4 51  866
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 51  867
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 51  868
          2          2                                            1050 4 51  869
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 51  870
                                                                  1050 4  0  871
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 52  872
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 52  873
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 52  874
          2          2                                            1050 4 52  875
 0.00000+ 0 1.49200+ 5          0          0          1          21050 4 52  876
          2          2                                            1050 4 52  877
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 52  878
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 52  879
          2          2                                            1050 4 52  880
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 52  881
                                                                  1050 4  0  882
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 53  883
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 53  884
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 53  885
          2          2                                            1050 4 53  886
 0.00000+ 0 6.08000+ 5          0          0          1          21050 4 53  887
          2          2                                            1050 4 53  888
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 53  889
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 53  890
          2          2                                            1050 4 53  891
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 53  892
                                                                  1050 4  0  893
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 54  894
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 54  895
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 54  896
          2          2                                            1050 4 54  897
 0.00000+ 0 6.75000+ 5          0          0          1          21050 4 54  898
          2          2                                            1050 4 54  899
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 54  900
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 54  901
          2          2                                            1050 4 54  902
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 54  903
                                                                  1050 4  0  904
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 55  905
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 55  906
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 55  907
          2          2                                            1050 4 55  908
 0.00000+ 0 7.58000+ 5          0          0          1          21050 4 55  909
          2          2                                            1050 4 55  910
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 55  911
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 55  912
          2          2                                            1050 4 55  913
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 55  914
                                                                  1050 4  0  915
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 56  916
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 56  917
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 56  918
          2          2                                            1050 4 56  919
 0.00000+ 0 9.41000+ 5          0          0          1          21050 4 56  920
          2          2                                            1050 4 56  921
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 56  922
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 56  923
          2          2                                            1050 4 56  924
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 56  925
                                                                  1050 4  0  926
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 57  927
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 57  928
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 57  929
          2          2                                            1050 4 57  930
 0.00000+ 0 9.89000+ 5          0          0          1          21050 4 57  931
          2          2                                            1050 4 57  932
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 57  933
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 57  934
          2          2                                            1050 4 57  935
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 57  936
                                                                  1050 4  0  937
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 58  938
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 58  939
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 58  940
          2          2                                            1050 4 58  941
 0.00000+ 0 1.03500+ 6          0          0          1          21050 4 58  942
          2          2                                            1050 4 58  943
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 58  944
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 58  945
          2          2                                            1050 4 58  946
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 58  947
                                                                  1050 4  0  948
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 59  949
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 59  950
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 59  951
          2          2                                            1050 4 59  952
 0.00000+ 0 1.07500+ 6          0          0          1          21050 4 59  953
          2          2                                            1050 4 59  954
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 59  955
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 59  956
          2          2                                            1050 4 59  957
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 59  958
                                                                  1050 4  0  959
 9.42380+ 4 2.36167+ 2          0          2          0          01050 4 91  960
 0.00000+ 0 2.36167+ 2          0          2          0          01050 4 91  961
 0.00000+ 0 0.00000+ 0          0          0          1          21050 4 91  962
          2          2                                            1050 4 91  963
 0.00000+ 0 1.20000+ 6          0          0          1          21050 4 91  964
          2          2                                            1050 4 91  965
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 91  966
 0.00000+ 0 2.00000+ 7          0          0          1          21050 4 91  967
          2          2                                            1050 4 91  968
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1050 4 91  969
                                                                  1050 4  0  970
                                                                  1050 0  0  971
 9.42380+ 4 2.36167+ 2          0          0          1          01050 5 16  972
 6.97000+ 6 0.00000+ 0          0          9          1          21050 5 16  973
          2          2                                            1050 5 16  974
 6.97000+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1050 5 16  975
 0.00000+ 0 0.00000+ 0          0          0          1         121050 5 16  976
         12          2                                            1050 5 16  977
 6.97000+ 6 1.00000+ 4 7.00000+ 6 1.40000+ 4 7.50000+ 6 1.14000+ 51050 5 16  978
 8.00000+ 6 2.14000+ 5 9.00000+ 6 2.63000+ 5 1.00000+ 7 3.12000+ 51050 5 16  979
 1.10000+ 7 3.61000+ 5 1.20000+ 7 4.10000+ 5 1.30000+ 7 4.59000+ 51050 5 16  980
 1.40000+ 7 5.08000+ 5 1.50000+ 7 5.57000+ 5 2.00000+ 7 8.02000+ 51050 5 16  981
                                                                  1050 5  0  982
 9.42380+ 4 2.36167+ 2          0          0          1          01050 5 17  983
 1.29700+ 7 0.00000+ 0          0          9          1          21050 5 17  984
          2          2                                            1050 5 17  985
 1.29700+ 7 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1050 5 17  986
 0.00000+ 0 0.00000+ 0          0          0          1          51050 5 17  987
          5          2                                            1050 5 17  988
 1.29700+ 7 1.00000+ 4 1.30000+ 7 6.00000+ 4 1.40000+ 7 2.06000+ 51050 5 17  989
 1.50000+ 7 2.55000+ 5 2.00000+ 7 5.00000+ 5                      1050 5 17  990
                                                                  1050 5  0  991
 9.42380+ 4 2.36167+ 2          0          0          1          01050 5 18  992
-3.00000+ 7 0.00000+ 0          0          7          1          21050 5 18  993
          2          2                                            1050 5 18  994
 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1050 5 18  995
 0.00000+ 0 0.00000+ 0          0          0          1          31050 5 18  996
          3          5                                            1050 5 18  997
 1.00000- 5 1.33330+ 6 1.50000+ 7 1.33330+ 6 2.00000+ 7 1.33330+ 61050 5 18  998
                                                                  1050 5  0  999
 9.42380+ 4 2.36167+ 2          0          0          1          01050 5 91 1000
 1.49000+ 5 0.00000+ 0          0          9          1          21050 5 91 1001
          2          2                                            1050 5 91 1002
 1.20000+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1050 5 91 1003
 0.00000+ 0 0.00000+ 0          0          0          1          41050 5 91 1004
          4          2                                            1050 5 91 1005
 1.20000+ 6 2.25289+ 5 2.00000+ 6 2.79436+ 5 1.50000+ 7 7.65267+ 51050 5 91 1006
 2.00000+ 7 9.52125+ 5                                            1050 5 91 1007
                                                                  1050 5  0 1008
                                                                  1050 0  0 1009
                                                                     0 0  0 1010
 9.52410+ 4 2.38950+ 2          1          1          0         201056 1451    1
 0.00000+ 0 0.00000+ 0          1          1        110          01056 1451    2
 95-am-241 anc        eval-nov66 j.r.smith and r.a.grimesey       1056 1451    3
 pri.comm.(nov.1966)  dist-may74  rev-nov74                       1056 1451    4
 extended to 20 mev for endf/b version-iv   (apr74)               1056 1451    5
 added radioactive decay data (mf=1,mt=457) (apr74)               1056 1451    6
          *          *          *          *          *          *1056 1451    7
   mt=457 (rad. decay data) eval-feb74 by c.w.reich (anc)         1056 1451    8
             q(alpha)- 1973 revision of wapstra-gove mass table.  1056 1451    9
             half-life- n.e. holden, chart of the nuclides (1973) 1056 1451   10
                         and private communication (jan., 1974).  1056 1451   11
             gamma-ray energies and intensities,where reported,are1056 1451   12
              from j.e. cline, usaec report in-1448 (1971).       1056 1451   13
             the internal-conversion coefficients of the stronger 1056 1451   14
             gamma-ray transitions below 100kev are taken from    1056 1451   15
             m.j. martin and p.h. blichert-toft, nuclear data     1056 1451   16
             tables a, nos.1-2, 144(1970).                        1056 1451   17
             other- y.a. ellis, nucl. data b 6, no.6, 621(1971).  1056 1451   18
  note  )e-alpha  =  5572. kev.                                   1056 1451   19
         this value includes the kinetic energy of both the       1056 1451   20
         alpha particle and the recoil nucleus.                   1056 1451   21
          *          *          *          *          *          *1056 1451   22
 *         *          *          *         *          *         * 1056 1451   23
 data modified june,1970 to conform to endf/b-ii formats          1056 1451   24
 *         *          *          *         *          *         * 1056 1451   25
americium 241 evaluated by idaho nuclear corp nrts                1056 1451   26
mf=1 mt=452 a weighted average of the individual determinations   1056 1451   27
            of nu assigns most all weight to the v.i.lebedev et.al1056 1451   28
            atomnaya energiya, 5 2 176 1958,value. using the      1056 1451   29
            currently favored value of nu for 235 of 2.43, we     1056 1451   30
            obtain nu=3.09 for the constant term. the slope is    1056 1451   31
            that of the universal curve of j.c.hopkins and b.c.   1056 1451   32
            diven,nuc.phys. 48 433 1963.                          1056 1451   33
     mt=453 decay data from d.t.goldman and j.r.stehn, chart of   1056 1451   34
            the nuclides, 1965.  when branching occurs,           1056 1451   35
            only the major branch is followed.                    1056 1451   36
     mt=454 the data of j.g.cuninghame,j.inorg.nucl.chem. 4 7 19571056 1451   37
            and r.r.richard et.al. trans.am.nuc.soc. 6 2 1963,    1056 1451   38
            were plotted and a smooth curve drawn through the pts.1056 1451   39
            the data were taken from the smooth curve and the     1056 1451   40
            authors normalization was accepted.                   1056 1451   41
mf=2 mt=151 below 16 ev the data appeared to be adequately        1056 1451   42
            represented by a fit by s.pearlstein,cross sections   1056 1451   43
            for trans-uranium element production,bnl 982.1966,    1056 1451   44
            using the recommended parameters from bnl 325 supp2.  1056 1451   45
            g=.5 potential scattering= 10 barns. smooth capture   1056 1451   46
            cs in resolved and unresolved range is 1/v and is     1056 1451   47
            417 barns at .0253 ev. smooth fission cs in resolved  1056 1451   48
            range only is 1/v and is 2.05 barns at .0253 ev.      1056 1451   49
            pointwise bomb shot fission data used throughout      1056 1451   50
            unresolved range to .1mev and consequently no fission 1056 1451   51
            widths specified in unresolved range. unresolved      1056 1451   52
            calculation is for capture only. average neutron width1056 1451   53
            calculated for one degree of freedom in porter thomas 1056 1451   54
            distribution.                                         1056 1451   55
mf=3 mt=  1 no total cs measurements available above 16 ev. the   1056 1451   56
            total cs was not added due to complications with bomb 1056 1451   57
            shot fission data. total cs is sum of reaction cs.    1056 1451   58
     mt=  2 below .1mev elastic cs is 10 barns. above .1mev       1056 1451   59
            elastic cs  is that for pu 239,j.j.schmidt evaluation 1056 1451   60
            kfk 120 karlsruhe,extrapolated to 15 mev.             1056 1451   61
     mt=  4 no data available. since level structure of am241 is  1056 1451   62
            somewhat similar to u238,we used u238 total inelastic 1056 1451   63
            cs taken from j.j.schmidt evaluation,kfk 120 karlsruhe1056 1451   64
     mt= 18 in the thermal range to .2ev a smooth curve was       1056 1451   65
            drawn through the experimental points in bnl 325 supp21056 1451   66
            from 16 to 20 ev data was taken from g.d.bowman       1056 1451   67
            (lrl,pvt.com.). from 20 ev to 0.4 mev petrel nuclear  1056 1451   68
            explosion data are used (p-3 and w-8 staff, lasl 3586)1056 1451   69
            from 20 ev to 40 ev petrel pointwise data are used.   1056 1451   70
            from 40 ev to 0.4 mev 10 percent average data (p.a.   1056 1451   71
            seeger,pvt.com.) are used. above 0.4 mev data are from1056 1451   72
            smooth curve drawn through petrel data (to 2 mev) and 1056 1451   73
            data of nobles et al (phys.rev.99,616a (1955)), norm. 1056 1451   74
            at plateau (2-4 mev) to 1.75b, which is wtd. ave. of  1056 1451   75
            values from seeger (petrel), nobles, bowman (iaea conf1056 1451   76
            paris cn-23/18 1966), kazarinova (at.energ.ussr 8 139 1056 1451   77
            1960) 15 mev value is ave. between kazarinova and     1056 1451   78
            protopopov (at.energ.ussr 6 67 1959).                 1056 1451   79
q-value ref.a.prince,private communication 23apr68                1056 1451   80
     mt=102 points from 0.001ev to 0.2 ev are from smooth curve   1056 1451   81
            drawn through data of adamchuk et al (proc.int conf on1056 1451   82
            puae /p/645 1955), with 10 b. pot. scat. subtracted to1056 1451   83
            obtain abs. cs. the fission cs was then subtracted too1056 1451   84
            obtain capture cs. between .2 and .3 ev the smooth    1056 1451   85
            capture file represents the difference between the    1056 1451   86
            pearlstein fit (nbl 982) and a smooth curve through   1056 1451   87
            the experimental points of slaughter (ornl 3085) and  1056 1451   88
            adumchuk.                                             1056 1451   89
            .3ev to.1mev the smooth capture cs is 1/u with a value1056 1451   90
            of 417 barns at.0253ev. an unresolved calc. using the 1056 1451   91
            parameters in file 2 yielded a value of .43 barns at  1056 1451   92
            .1mev. this added to the residual 1/v smooth capture  1056 1451   93
            cs gave a value of .64 barns capture at .1mev. a      1056 1451   94
            straight line was drawn from .64 barns at .1mev to    1056 1451   95
            the optical model value of d.t.goldman,trans.am.nucl. 1056 1451   96
            soc. 7 84 1964, at .6 mev for np237. the capture cs   1056 1451   97
            value used from here to 10 mev is based on an         1056 1451   98
            extrapolation of the goldman curve for np237.         1056 1451   99
    mt=251,252,253 mu-bar(l-system),xi,gamma calculated by chad   1056 1451  100
mf=4 mt=  2 angular distributions supplied by h.alter of ai, comp-1056 1451  101
            osed of a mixture of measured data for u235,u238,and  1056 1451  102
            pu239. values of gamma slowing down parameter above   1056 1451  103
            10 kev are suspect and are not to be used without     1056 1451  104
            futher study.                                         1056 1451  105
mf=5 mt=  4 evaporation model specified for inelastic cs, temp    1056 1451  106
            calculated from 3230 squarr rt(e/a). no level data    1056 1451  107
            available.                                            1056 1451  108
      mt=18  fission spectrum has maxwellian density with the temp1056 1451  109
             based on  terrells prescription (terrell,j.,physics  1056 1451  110
             and chemistry of fission,vol 2.,iaea,1965).the therm 1056 1451  111
             value of nu was used to determin the temperature.    1056 1451  112
                                1        451        132           1056 1451  113
                                1        452          3           1056 1451  114
                                1        453          9           1056 1451  115
                                1        454         33           1056 1451  116
                                1        457         97           1056 1451  117
                                2        151         31           1056 1451  118
                                3          1        198           1056 1451  119
                                3          2         13           1056 1451  120
                                3          4         16           1056 1451  121
                                3         18        189           1056 1451  122
                                3         91         16           1056 1451  123
                                3        102         12           1056 1451  124
                                3        251         16           1056 1451  125
                                3        252         16           1056 1451  126
                                3        253         16           1056 1451  127
                                4          2        199           1056 1451  128
                                4         18         10           1056 1451  129
                                4         91         10           1056 1451  130
                                5         18          7           1056 1451  131
                                5         91         11           1056 1451  132
                                                                  1056 1  0  133
 9.52410+ 4 2.38950+ 2          0          1          0          01056 1452  134
 0.00000+ 0 0.00000+ 0          0          0          2          01056 1452  135
 3.09000+ 0 1.60000- 7                                            1056 1452  136
                                                                  1056 1  0  137
 9.52410+ 4 2.38950+ 2          0          0          1          01056 1453  138
 9.52410+ 4 2.38950+ 2          0          0          2          31056 1453  139
 1.00000- 5 2.00000+ 7                                            1056 1453  140
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 0.00000+ 0 8.50000+ 5          0          0          9          01056 4  2  949
 3.94518- 1 2.04052- 1 1.09070- 1 4.92385- 2 1.34170- 2 2.10312- 31056 4  2  950
-1.20776- 3 6.18284- 5 8.31156- 4                                 1056 4  2  951
 0.00000+ 0 9.00000+ 5          0          0          9          01056 4  2  952
 4.32578- 1 2.37751- 1 1.34152- 1 5.15560- 2 8.03460- 3 2.08049- 31056 4  2  953
-8.29790- 4-2.27734- 4 1.10874- 3                                 1056 4  2  954
 0.00000+ 0 9.50000+ 5          0          0          9          01056 4  2  955
 4.46607- 1 2.64977- 1 1.22226- 1 3.31196- 2 2.53548- 3 8.12435- 41056 4  2  956
-3.20350- 4-9.59325- 6 6.32208- 4                                 1056 4  2  957
 0.00000+ 0 1.00000+ 6          0          0          9          01056 4  2  958
 4.44036- 1 2.34427- 1 1.60385- 1 5.60398- 2-1.66255- 3-1.19733- 21056 4  2  959
-5.47596- 3-6.54808- 4-1.81102- 4                                 1056 4  2  960
 0.00000+ 0 1.05000+ 6          0          0          9          01056 4  2  961
 4.41276- 1 2.95561- 1 1.91881- 1 9.82002- 2 3.02872- 2 2.45372- 31056 4  2  962
-2.20543- 3 5.81421- 4 9.84641- 4                                 1056 4  2  963
 0.00000+ 0 1.10000+ 6          0          0          9          01056 4  2  964
 4.35165- 1 2.65842- 1 1.81954- 1 8.31117- 2 1.67715- 2 2.72754- 31056 4  2  965
-1.38186- 3-1.74019- 4 1.45669- 3                                 1056 4  2  966
 0.00000+ 0 1.15000+ 6          0          0          9          01056 4  2  967
 4.16839- 1 2.45080- 1 1.67122- 1 7.48796- 2 9.71660- 3-2.07436- 41056 4  2  968
-6.75760- 5-1.71672- 4 9.60077- 4                                 1056 4  2  969
 0.00000+ 0 1.20000+ 6          0          0          9          01056 4  2  970
 4.30179- 1 2.73304- 1 1.83373- 1 8.56124- 2 2.14650- 2 3.72234- 31056 4  2  971
-2.01216- 3-6.12140- 6 1.49193- 3                                 1056 4  2  972
 0.00000+ 0 1.25000+ 6          0          0          9          01056 4  2  973
 4.20688- 1 2.59980- 1 1.97871- 1 9.35682- 2 1.51488- 2 1.63747- 31056 4  2  974
-8.29056- 4-3.19795- 4 1.50728- 3                                 1056 4  2  975
 0.00000+ 0 1.29500+ 6          0          0          9          01056 4  2  976
 4.30705- 1 2.73546- 1 2.03596- 1 1.09004- 1 3.02946- 2 3.54913- 31056 4  2  977
-2.35442- 3 1.82121- 4 1.52007- 3                                 1056 4  2  978
 0.00000+ 0 1.35000+ 6          0          0          9          01056 4  2  979
 3.98358- 1 2.39171- 1 1.85083- 1 9.64841- 2 2.01074- 2 1.26862- 31056 4  2  980
-1.02350- 3-6.37440- 5 1.25881- 3                                 1056 4  2  981
 0.00000+ 0 1.40000+ 6          0          0          9          01056 4  2  982
 4.30662- 1 2.59630- 1 1.96530- 1 1.04192- 1 2.08869- 2-6.75852- 41056 4  2  983
-4.56102- 4 1.44862- 4 9.11551- 4                                 1056 4  2  984
 0.00000+ 0 1.45000+ 6          0          0          9          01056 4  2  985
 4.26523- 1 2.70130- 1 2.08551- 1 1.16101- 1 3.10470- 2 2.08351- 31056 4  2  986
-1.90302- 3 2.87671- 4 1.29242- 3                                 1056 4  2  987
 0.00000+ 0 1.49500+ 6          0          0          9          01056 4  2  988
 4.48826- 1 3.06650- 1 2.38702- 1 1.53640- 1 6.37323- 2 9.13384- 31056 4  2  989
-6.01040- 3 9.57001- 4 2.09428- 3                                 1056 4  2  990
 0.00000+ 0 2.00000+ 6          0          0          9          01056 4  2  991
 5.51404- 1 3.72565- 1 3.00695- 1 1.98353- 1 7.42062- 2 1.59169- 21056 4  2  992
-2.43779- 3-6.30132- 3-6.63877- 3                                 1056 4  2  993
 0.00000+ 0 2.50000+ 6          0          0          9          01056 4  2  994
 6.55613- 1 4.93352- 1 3.51640- 1 2.63128- 1 1.38256- 1 4.50684- 21056 4  2  995
 3.95270- 3-5.35058- 3-3.64636- 3                                 1056 4  2  996
 0.00000+ 0 4.10000+ 6          0          0          9          01056 4  2  997
 7.63418- 1 6.20854- 1 4.92776- 1 3.95979- 1 2.67223- 1 1.54076- 11056 4  2  998
 8.43991- 2 4.30327- 2 1.65042- 2                                 1056 4  2  999
 0.00000+ 0 7.00000+ 6          0          0         20          01056 4  2 1000
 7.85369- 1 6.48133- 1 5.49672- 1 4.48463- 1 3.39480- 1 2.31379- 11056 4  2 1001
 1.48663- 1 9.49746- 2 5.69390- 2 2.71378- 2 6.95825- 3-2.41052- 31056 4  2 1002
-5.28045- 3-6.68533- 3-7.40794- 3-6.81612- 3-5.51271- 3-4.32058- 31056 4  2 1003
-3.26537- 3-1.84302- 3                                            1056 4  2 1004
 0.00000+ 0 1.50000+ 7          0          0         20          01056 4  2 1005
 8.82215- 1 7.63772- 1 6.54435- 1 5.69849- 1 4.99340- 1 4.44670- 11056 4  2 1006
 3.92075- 1 3.47640- 1 3.00188- 1 2.56016- 1 2.00629- 1 1.36011- 11056 4  2 1007
 7.69032- 2 3.83782- 2 1.67299- 2 6.10909- 3 2.11053- 3 5.47474- 41056 4  2 1008
 1.73218- 4 4.66783- 5                                            1056 4  2 1009
 0.00000+ 0 2.00000+ 7          0          0         20          01056 4  2 1010
 8.82215- 1 7.63772- 1 6.54435- 1 5.69849- 1 4.99340- 1 4.44670- 11056 4  2 1011
 3.92075- 1 3.47640- 1 3.00188- 1 2.56016- 1 2.00629- 1 1.36011- 11056 4  2 1012
 7.69032- 2 3.83782- 2 1.67299- 2 6.10909- 3 2.11053- 3 5.47474- 41056 4  2 1013
 1.73218- 4 4.66783- 5                                            1056 4  2 1014
                                                                  1056 4  0 1015
 9.52410+ 4 2.38950+ 2          0          2          0          01056 4 18 1016
 0.00000+ 0 2.38950+ 2          0          1          0          01056 4 18 1017
 0.00000+ 0 0.00000+ 0          0          0          1          21056 4 18 1018
          2          2                                            1056 4 18 1019
 0.00000+ 0 1.00000- 5          0          0          1          21056 4 18 1020
          2          2                                            1056 4 18 1021
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1056 4 18 1022
 0.00000+ 0 2.00000+ 7          0          0          1          21056 4 18 1023
          2          2                                            1056 4 18 1024
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1056 4 18 1025
                                                                  1056 4  0 1026
 9.52410+ 4 2.38950+ 2          0          2          0          01056 4 91 1027
 0.00000+ 0 2.38950+ 2          0          2          0          01056 4 91 1028
 0.00000+ 0 0.00000+ 0          0          0          1          21056 4 91 1029
          2          2                                            1056 4 91 1030
 0.00000+ 0 4.20000+ 4          0          0          1          21056 4 91 1031
          2          2                                            1056 4 91 1032
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1056 4 91 1033
 0.00000+ 0 2.00000+ 7          0          0          1          21056 4 91 1034
          2          2                                            1056 4 91 1035
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1056 4 91 1036
                                                                  1056 4  0 1037
                                                                  1056 0  0 1038
 9.52410+ 4 2.38950+ 2          0          0          1          01056 5 18 1039
-3.00000+ 7 0.00000+ 0          0          7          1          21056 5 18 1040
          2          2                                            1056 5 18 1041
 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1056 5 18 1042
 0.00000+ 0 0.00000+ 0          0          0          1          31056 5 18 1043
          3          2                                            1056 5 18 1044
 1.00000- 5 1.37600+ 6 1.50000+ 7 1.37600+ 6 2.00000+ 7 1.37600+ 61056 5 18 1045
                                                                  1056 5  0 1046
 9.52410+ 4 2.38950+ 2          0          0          1          01056 5 91 1047
 4.20000+ 4 0.00000+ 0          0          9          1          21056 5 91 1048
          2          2                                            1056 5 91 1049
 4.20000+ 4 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1056 5 91 1050
 0.00000+ 0 0.00000+ 0          0          0          1         141056 5 91 1051
         14          5                                            1056 5 91 1052
 4.20000+ 4 1.00000+ 4 3.00000+ 5 1.15000+ 5 1.00000+ 6 2.11000+ 51056 5 91 1053
 2.00000+ 6 2.98000+ 5 3.00000+ 6 3.65000+ 5 4.00000+ 6 4.21000+ 51056 5 91 1054
 5.00000+ 6 4.71000+ 5 6.00000+ 6 5.16000+ 5 7.00000+ 6 5.58000+ 51056 5 91 1055
 8.00000+ 6 5.96000+ 5 9.00000+ 6 6.32000+ 5 1.00000+ 7 6.66000+ 51056 5 91 1056
 1.50000+ 7 8.02000+ 5 2.00000+ 7 9.15023+ 5                      1056 5 91 1057
                                                                  1056 5  0 1058
                                                                  1056 0  0 1059
                                                                     0 0  0 1060
 9.52430+ 4 2.40940+ 2          1          1          0         201057 1451    1
 0.00000+ 0 0.00000+ 0          1          1         82          01057 1451    2
 95-am-243 anc        eval-nov66 j.r.smith and r.a.grimesey       1057 1451    3
 pri.comm.(nov.1966)  dist-may74                                  1057 1451    4
 extended to 20 mev for endf/b version-iv   (apr74)               1057 1451    5
 added radioactive decay data (mf=1,mt=457) (apr74)               1057 1451    6
          *          *          *          *          *          *1057 1451    7
   mt=457 (rad. decay data) eval-feb74 by c.w.reich (anc)         1057 1451    8
             q(alpha)- 1973 revision of wapstra-gove mass table.  1057 1451    9
             half-life- n.e. holden chart of the nuclides (1973)  1057 1451   10
                         and private communication (jan. 1974).   1057 1451   11
             other-  y.a. ellis and a.h. wapstra, nuclear data    1057 1451   12
                      sheets b 3, no.2 , 1 (1969).                1057 1451   13
  (a) i. ahmad and m. wahlgren, nucl. instr. and methods 99, 333  1057 1451   14
         (1972).                                                  1057 1451   15
  (b) j.r. van hise and d. engelkemeir, phys.rev. 171, 1325(1968).1057 1451   16
  (c) a. artna-cohen, nuclear data b 6, no.6, 577(1971).          1057 1451   17
  (d) d. engelkemeir, phys. rev. 181, 1675(1969).                 1057 1451   18
   note  )e-alpha  = 5352. kev.                                   1057 1451   19
            this value includes the kinetic energy of the alpha   1057 1451   20
            particle and the recoil energy of the daughter nucleus1057 1451   21
   note  the intensities of the two most intense gamma rays are   1057 1451   22
         taken from ref. (a). those of the remaining gamma rays   1057 1451   23
         are taken from refs. (b) and (c). the internal-conversion1057 1451   24
         coefficients listed are theoretical values,derived either1057 1451   25
         from intensity-balance considerations (refs. (c) and (d))1057 1451   26
         or from the gamma-ray mixing ratios deduced from the     1057 1451   27
         measurements of ref. (d). (see also the values given in  1057 1451   28
         ref. (c), page 587.) where a gamma ray is observed in    1057 1451   29
         both the am-243 and the u-239 decays (cf. ref. (c)) and  1057 1451   30
         a more precise energy value is obtained in the latter    1057 1451   31
         decay, the more precise value is listed here.            1057 1451   32
          *          *          *          *          *          *1057 1451   33
 data modified june,1970 to conform to endf/b-ii formats          1057 1451   34
 *         *          *          *         *          *         * 1057 1451   35
americium 243 evaluated by idaho nuclear corp nrts                1057 1451   36
mf=1 mt=452 the constant term was pure guess,the slope is based on1057 1451   37
            the universal curve of j.c.hopkins and b.c.diven,     1057 1451   38
            nuc.phys. 48 433 1963.                                1057 1451   39
     mt=453 decay data from d.t.goldman and j.r.stehn, chart of   1057 1451   40
            the nuclides, 1965.  when branching occurs,           1057 1451   41
            only the major branch is followed.                    1057 1451   42
     mt=454 no yield data, used am 241 yield curve.               1057 1451   43
mf=2 mt=151 res params based on fit of s.pearlstein,cross sections1057 1451   44
            for transuranium element production,bnl 982 1966,     1057 1451   45
            g=.5,potential scattering cs is 10 barns,no 1/v       1057 1451   46
            smooth capture necessary, resolved res range extends  1057 1451   47
            into thermal region to .0001 ev. no data except       1057 1451   48
            fission above 16 ev therefore extended unresolved     1057 1451   49
            range to 10000 ev,unresolved parameters averaged for  1057 1451   50
            s wave neutrons only based on pearlstein resolved     1057 1451   51
            parameters, unresolved res calculation using these    1057 1451   52
            parameters gave a capture cs at 10kev of 1.493 barns  1057 1451   53
mf=3 mt=  1 total cs is sum of mt=2,4,18,102 no measurements above1057 1451   54
            16 ev                                                 1057 1451   55
     mt=  2 resonance range below 10kev,from 10kev to .1 mev      1057 1451   56
            set elastic to 10 barn potential scatt cs, above .1   1057 1451   57
            mev data is that for pu239 j.j. schmidt evaluation,   1057 1451   58
            kfk 120 karlsruhe,extrapolated to 15 mev.             1057 1451   59
     mt=  4 no data available, since level structure of am 243 is 1057 1451   60
            similar to u238,we used u238 total inelastic cs from  1057 1451   61
            j.j.schmidt evaluation karlsruhe.                     1057 1451   62
     mt= 18 above 10000 ev used smooth line through d.k.butler and1057 1451   63
            r.k.sjoblom data in bnl 325 supp2, extrapolated first 1057 1451   64
            d.k.butler point at .30 mev to .001 barn at 10000 ev. 1057 1451   65
     mt=102 smooth capture cs is 0.0 below 10kev, at 10kev capture1057 1451   66
            cs based on 1.493 barn unresolved cs at 10kev. this   1057 1451   67
            point is extrapolated linearly to point on d.t.goldman1057 1451   68
            trans.am.nucl.soc. 7 84 1964,curve at .3mev for np237,1057 1451   69
            above .3 mev capture cs follows d.t.goldman curve     1057 1451   70
            for np237 extrapolated to .001barn at 10mev.          1057 1451   71
    mt=251,252,253 mu-bar(l-system),xi,gamma calculated by chad   1057 1451   72
mf=4 mt=  2 angular distributions supplied by h.alter of ai,      1057 1451   73
            composed of a mixture of measured data for u235,u238, 1057 1451   74
            and pu239, values of gamma slowing down parameter     1057 1451   75
            above 10kev are suspect and are not to be used without1057 1451   76
            study.                                                1057 1451   77
mf=5 mt=  4 evaporation model specified for inelastic cs,temp     1057 1451   78
            calculated from 3230square rt(e/a). no level data     1057 1451   79
            available.                                            1057 1451   80
      mt=18 fission spectrum has maxwellian density with the temp 1057 1451   81
            based on terrells prescription (terrell,j.,physics    1057 1451   82
            and chemistry of fission,vol 2. iaea,1965). the therm 1057 1451   83
            value of nu was used to determine the temperature     1057 1451   84
                                1        451        104           1057 1451   85
                                1        452          3           1057 1451   86
                                1        453          9           1057 1451   87
                                1        454         33           1057 1451   88
                                1        457         38           1057 1451   89
                                2        151         21           1057 1451   90
                                3          1         24           1057 1451   91
                                3          2         12           1057 1451   92
                                3          4         14           1057 1451   93
                                3         18         10           1057 1451   94
                                3         91         14           1057 1451   95
                                3        102          6           1057 1451   96
                                3        251         16           1057 1451   97
                                3        252         16           1057 1451   98
                                3        253         16           1057 1451   99
                                4          2        199           1057 1451  100
                                4         18         10           1057 1451  101
                                4         91         10           1057 1451  102
                                5         18          7           1057 1451  103
                                5         91         11           1057 1451  104
                                                                  1057 1  0  105
 9.52430+ 4 2.40940+ 2          0          1          0          01057 1452  106
 0.00000+ 0 0.00000+ 0          0          0          2          01057 1452  107
 3.00000+ 0 1.60000- 7                                            1057 1452  108
                                                                  1057 1  0  109
 9.52430+ 4 2.40940+ 2          0          0          1          01057 1453  110
 9.52430+ 4 2.40940+ 2          0          0          2          31057 1453  111
 1.00000- 5 2.00000+ 7                                            1057 1453  112
 0.00000+ 0-6.37700+ 6          0          0          5          01057 1453  113
 1.60000+ 1 9.52420+ 4 1.20000- 6 1.00000+ 0 1.00000+ 0           1057 1453  114
 0.00000+ 0-1.19050+ 7          0          0          5          01057 1453  115
 1.70000+ 1 9.52410+ 4 4.79900-11 1.00000+ 0 1.00000+ 0           1057 1453  116
 0.00000+ 0 5.36400+ 6          0          0          5          01057 1453  117
 1.02000+ 2 9.52440+ 4 4.62000- 4 1.00000+ 0 1.00000+ 0           1057 1453  118
                                                                  1057 1  0  119
 9.52430+ 4 2.40940+ 2          1          0          0          01057 1454  120
 0.00000+ 0 0.00000+ 0          0          0        183         611057 1454  121
 3.70870+ 4 0.00000+ 0 2.00000- 3 3.80880+ 4 0.00000+ 0 4.60000- 31057 1454  122
 3.80890+ 4 0.00000+ 0 8.10000- 3 3.80900+ 4 0.00000+ 0 1.20000- 21057 1454  123
 3.80910+ 4 0.00000+ 0 1.65000- 2 4.00920+ 4 0.00000+ 0 2.20000- 21057 1454  124
 4.00930+ 4 0.00000+ 0 2.70000- 2 4.00940+ 4 0.00000+ 0 3.30000- 21057 1454  125
 4.00950+ 4 0.00000+ 0 3.90000- 2 4.00960+ 4 0.00000+ 0 4.30000- 21057 1454  126
 4.00970+ 4 0.00000+ 0 4.90000- 2 4.20980+ 4 0.00000+ 0 5.80000- 21057 1454  127
 4.20990+ 4 0.00000+ 0 6.50000- 2 4.21000+ 4 0.00000+ 0 6.90000- 21057 1454  128
 4.41010+ 4 0.00000+ 0 7.30000- 2 4.41020+ 4 0.00000+ 0 7.60000- 21057 1454  129
 4.41030+ 4 0.00000+ 0 7.70000- 2 4.41040+ 4 0.00000+ 0 7.20000- 21057 1454  130
 4.41050+ 4 0.00000+ 0 6.60000- 2 4.41060+ 4 0.00000+ 0 5.40000- 21057 1454  131
 4.51070+ 4 0.00000+ 0 4.20000- 2 4.51080+ 4 0.00000+ 0 3.10000- 21057 1454  132
 4.61070+ 4 0.00000+ 0 2.00000- 2 4.61100+ 4 0.00000+ 0 1.30000- 21057 1454  133
 4.61120+ 4 0.00000+ 0 4.00000- 3 4.71110+ 4 0.00000+ 0 9.00000- 31057 1454  134
 4.71130+ 4 0.00000+ 0 1.80000- 3 4.81150+ 4 0.00000+ 0 5.00000- 41057 1454  135
 4.81170+ 4 0.00000+ 0 4.30000- 4 4.91190+ 4 0.00000+ 0 4.30000- 41057 1454  136
 5.01210+ 4 0.00000+ 0 4.50000- 4 5.01230+ 4 0.00000+ 0 8.20000- 41057 1454  137
 5.01250+ 4 0.00000+ 0 1.90000- 3 5.01260+ 4 0.00000+ 0 3.00000- 31057 1454  138
 5.11270+ 4 0.00000+ 0 5.20000- 3 5.21280+ 4 0.00000+ 0 8.80000- 31057 1454  139
 5.21290+ 4 0.00000+ 0 1.48000- 2 5.21300+ 4 0.00000+ 0 2.20000- 21057 1454  140
 5.21320+ 4 0.00000+ 0 5.00000- 2 5.31310+ 4 0.00000+ 0 3.50000- 21057 1454  141
 5.41330+ 4 0.00000+ 0 6.30000- 2 5.41340+ 4 0.00000+ 0 7.40000- 21057 1454  142
 5.41350+ 4 0.00000+ 0 8.30000- 2 5.51360+ 4 0.00000+ 0 8.70000- 21057 1454  143
 5.51370+ 4 0.00000+ 0 8.60000- 2 5.61380+ 4 0.00000+ 0 7.90000- 21057 1454  144
 5.61390+ 4 0.00000+ 0 7.00000- 2 5.61400+ 4 0.00000+ 0 6.10000- 21057 1454  145
 5.81410+ 4 0.00000+ 0 5.40000- 2 5.81420+ 4 0.00000+ 0 4.50000- 21057 1454  146
 5.81440+ 4 0.00000+ 0 3.30000- 2 6.01430+ 4 0.00000+ 0 3.85000- 21057 1454  147
 6.01450+ 4 0.00000+ 0 2.84000- 2 6.01460+ 4 0.00000+ 0 2.44000- 21057 1454  148
 6.01470+ 4 0.00000+ 0 2.06000- 2 6.01480+ 4 0.00000+ 0 1.75000- 21057 1454  149
 6.21490+ 4 0.00000+ 0 1.52000- 2 6.21500+ 4 0.00000+ 0 1.30000- 21057 1454  150
 6.21510+ 4 0.00000+ 0 1.07000- 2 6.21520+ 4 0.00000+ 0 8.60000- 31057 1454  151
 6.21530+ 4 0.00000+ 0 7.60000- 4                                 1057 1454  152
                                                                  1057 1  0  153
 9.52430+ 4 2.40940+ 2          0          0          0          21057 1457  154
 2.32420+11 1.26144+ 9          0          0          6          31057 1457  155
 0.00000+ 0 0.00000+ 0 7.82300+ 4 0.00000+ 0 5.35200+ 6 0.00000+ 01057 1457  156
 9.52430+ 4 2.40940+ 2          0          0          6          11057 1457  157
 4.00000+ 0 0.00000+ 0 5.43810+ 6 1.00000+ 3 1.00000+ 0 0.00000+ 01057 1457  158
 4.00000+ 0 0.00000+ 0          0          0         96         151057 1457  159
 1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  160
 4.69500+ 6 3.00000+ 3 1.30000- 3 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  161
 4.91900+ 6 3.00000+ 3 8.50000- 5 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  162
 4.93000+ 6 3.00000+ 3 1.80000- 4 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  163
 4.94600+ 6 3.00000+ 3 3.40000- 4 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  164
 4.99700+ 6 3.00000+ 3 8.00000- 4 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  165
 5.00800+ 6 3.00000+ 3 8.00000- 4 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  166
 5.02900+ 6 3.00000+ 3 1.30000- 3 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  167
 5.03500+ 6 3.00000+ 3 9.00000- 4 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  168
 5.08800+ 6 3.00000+ 3 4.00000- 3 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  169
 5.11300+ 6 1.00000+ 3 5.40000- 3 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  170
 5.18100+ 6 1.00000+ 3 1.10000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 1457  171
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 2.82430- 4 2.20977- 6-2.15743- 7-6.10364- 9 0.00000+ 0 0.00000+ 01057 4  2  394
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  395
 2.34367-19-1.60319-16 1.09660-13-3.46860-11 8.66955- 9-1.66935- 61057 4  2  396
 2.35031- 4-2.17341- 2 9.99430- 1 2.58912- 2 3.34057- 4 2.84633- 61057 4  2  397
-1.40976- 7-2.40829- 9 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  398
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 5.34715-19-4.61354-161057 4  2  399
 2.00293-13-5.63201-11 1.26522- 8-2.20548- 6 2.82400- 4-2.38117- 21057 4  2  400
 9.99327- 1 2.79674- 2 3.90085- 4 3.60107- 6-1.50602- 7-7.87232- 91057 4  2  401
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  402
 0.00000+ 0 0.00000+ 0 1.37743-18-9.95155-16 3.44390-13-8.73800-111057 4  2  403
 1.78499- 8-2.84432- 6 3.34066- 4-2.58884- 2 9.99215- 1 3.00429- 21057 4  2  404
 4.50321- 4 4.46687- 6-7.27849- 9-3.03717-10 0.00000+ 0 0.00000+ 01057 4  2  405
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  406
 2.83816-18-1.89339-15 5.64133-13-1.30609-10 2.44851- 8-3.59480- 61057 4  2  407
 3.90031- 4-2.79642- 2 9.99095- 1 3.21177- 2 5.15020- 4 5.47537- 61057 4  2  408
-6.49275- 8-2.94912- 9 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  409
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 5.24594-18-3.33945-151057 4  2  410
 8.87874-13-1.89232-10 3.27988- 8-4.46583- 6 4.50294- 4-3.00392- 21057 4  2  411
 9.98966- 1 3.41918- 2 5.83799- 4 6.61165- 6-4.32601- 8-4.36203- 91057 4  2  412
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  413
 0.00000+ 0-1.77892-20 9.05260-18-5.58238-15 1.35117-12-2.66992-101057 4  2  414
 4.30504- 8-5.46634- 6 5.14853- 4-3.21134- 2 9.98828- 1 3.62652- 21057 4  2  415
 6.56959- 4 7.89665- 6 3.90746- 8 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  416
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0-3.06994-201057 4  2  417
 1.48643-17-8.95303-15 1.99792-12-3.68189-10 5.55176- 8-6.60524- 61057 4  2  418
 5.83708- 4-3.41869- 2 9.98682- 1 3.83380- 2 7.34477- 4 9.34193- 61057 4  2  419
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  420
 0.00000+ 0 0.00000+ 0 0.00000+ 0-5.03506-20 2.34776-17-1.38826-141057 4  2  421
 2.88153-12-4.97720-10 7.04971- 8-7.89144- 6 6.56859- 4-3.62597- 21057 4  2  422
 9.98527- 1 4.04101- 2 8.16240- 4 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  423
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  424
 0.00000+ 0-7.93800-20 3.59214-17-2.09235-14 4.06620-12-6.61116-101057 4  2  425
 8.83035- 8-9.33385- 6 7.34303- 4-3.83319- 2 9.98363- 1 4.24816- 21057 4  2  426
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01057 4  2  427
 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0-1.21180-191057 4  2  428
 5.35028-17-3.07735-14 5.62829-12-8.64580-10 1.09270- 7-1.09414- 51057 4  2  429
 8.16040- 4-4.04033- 2 9.98191- 1                                 1057 4  2  430
 0.00000+ 0 0.00000+ 0          0          0          1         391057 4  2  431
         39          3                                            1057 4  2  432
 0.00000+ 0 1.00000- 5          0          0          1          01057 4  2  433
 0.00000+ 0                                                       1057 4  2  434
 0.00000+ 0 1.00000+ 4          0          0          1          01057 4  2  435
 0.00000+ 0                                                       1057 4  2  436
 0.00000+ 0 5.00000+ 4          0          0          9          01057 4  2  437
 3.45463- 2 1.41376- 2-4.89222- 3 5.21115- 3-5.98587- 4-2.54581- 41057 4  2  438
 2.00060- 4-1.15404- 4 1.72304- 4                                 1057 4  2  439
 0.00000+ 0 1.00000+ 5          0          0          9          01057 4  2  440
 7.61954- 2 1.90280- 2 7.58588- 4-5.67662- 4 2.33595- 4 2.45645- 41057 4  2  441
-9.14024- 5-1.15372- 4-1.46715- 5                                 1057 4  2  442
 0.00000+ 0 2.07000+ 5          0          0          9          01057 4  2  443
 1.90193- 1 4.22135- 2-3.96458- 3 2.49946- 3-1.00324- 3-2.46498- 51057 4  2  444
 5.09447- 4-3.22708- 4 3.54128- 5                                 1057 4  2  445
 0.00000+ 0 3.00000+ 5          0          0          9          01057 4  2  446
 3.24290- 1 9.08160- 2 1.53375- 2 1.11803- 2 4.38686- 3-5.29180- 41057 4  2  447
 2.60174- 5 8.84191- 5 5.75832- 6                                 1057 4  2  448
 0.00000+ 0 3.50000+ 5          0          0          9          01057 4  2  449
 2.78978- 1 1.01001- 1 3.50701- 2 4.55946- 3-9.68728- 3-2.68220- 31057 4  2  450
 1.54395- 3-3.15965- 4-1.00448- 5                                 1057 4  2  451
 0.00000+ 0 4.00000+ 5          0          0          9          01057 4  2  452
 3.08847- 1 1.00906- 1 1.48973- 2-9.07750- 3-6.70775- 3 1.25086- 31057 4  2  453
 6.46627- 5-4.37997- 4 5.05789- 4                                 1057 4  2  454
 0.00000+ 0 4.50000+ 5          0          0          9          01057 4  2  455
 3.23252- 1 1.25275- 1 3.78155- 2 9.95484- 3-8.74056- 4-8.88078- 41057 4  2  456
 4.13486- 4-3.38320- 5 8.14289- 5                                 1057 4  2  457
 0.00000+ 0 4.70000+ 5          0          0          9          01057 4  2  458
 3.37494- 1 1.16204- 1 2.72127- 2 7.72741- 3 3.79737- 4-5.83046- 41057 4  2  459
 2.45091- 4-1.30359- 5 7.53133- 5                                 1057 4  2  460
 0.00000+ 0 5.00000+ 5          0          0          9          01057 4  2  461
 3.10778- 1 9.49037- 2 2.80901- 2-9.79990- 4-8.12803- 3-6.03644- 31057 4  2  462
-1.70360- 3 1.00086- 3 1.53695- 3                                 1057 4  2  463
 0.00000+ 0 5.50000+ 5          0          0          9          01057 4  2  464
 3.33499- 1 1.41931- 1 4.46051- 2 8.08038- 3-1.50068- 3-8.07506- 41057 4  2  465
 7.73154- 4 6.80699- 4-2.62907- 4                                 1057 4  2  466
 0.00000+ 0 5.70000+ 5          0          0          9          01057 4  2  467
 3.78969- 1 1.36038- 1 2.18667- 2-2.57259- 3 1.92470- 4 1.76305- 31057 4  2  468
-5.46111- 4-1.23431- 4 4.12725- 4                                 1057 4  2  469
 0.00000+ 0 6.00000+ 5          0          0          9          01057 4  2  470
 3.79179- 1 1.60847- 1 4.75280- 2 1.26422- 2 2.84058- 3 4.35786- 51057 4  2  471
-1.40310- 4 1.10445- 4 1.50040- 4                                 1057 4  2  472
 0.00000+ 0 6.50000+ 5          0          0          9          01057 4  2  473
 4.20443- 1 1.73443- 1 5.10157- 2 1.29274- 2 1.63751- 3-2.19692- 41057 4  2  474
 3.37553- 5 5.84845- 5 1.64814- 4                                 1057 4  2  475
 0.00000+ 0 7.00000+ 5          0          0          9          01057 4  2  476
 3.69841- 1 1.92349- 1 8.59634- 2 2.54658- 2-2.02899- 4-1.03040- 31057 4  2  477
 4.46471- 4-1.84445- 5 2.50438- 4                                 1057 4  2  478
 0.00000+ 0 7.50000+ 5          0          0          9          01057 4  2  479
 3.97769- 1 2.09825- 1 1.05081- 1 3.97872- 2 7.34262- 3 1.09708- 31057 4  2  480
-5.85362- 4-1.66722- 5 6.80032- 4                                 1057 4  2  481
 0.00000+ 0 7.75000+ 5          0          0          9          01057 4  2  482
 4.50913- 1 2.36963- 1 8.79392- 2 1.87719- 2 2.83208- 3 1.61216- 31057 4  2  483
-6.55481- 4 2.69932- 5 5.58702- 4                                 1057 4  2  484
 0.00000+ 0 8.00000+ 5          0          0          9          01057 4  2  485
 3.86000- 1 2.00040- 1 1.07249- 1 4.11048- 2 2.41910- 3-1.25869- 31057 4  2  486
 4.87663- 4-7.72329- 5 4.05549- 4                                 1057 4  2  487
 0.00000+ 0 8.50000+ 5          0          0          9          01057 4  2  488
 3.94518- 1 2.04052- 1 1.09070- 1 4.92385- 2 1.34170- 2 2.10312- 31057 4  2  489
-1.20776- 3 6.18284- 5 8.31156- 4                                 1057 4  2  490
 0.00000+ 0 9.00000+ 5          0          0          9          01057 4  2  491
 4.32578- 1 2.37751- 1 1.34152- 1 5.15560- 2 8.03460- 3 2.08049- 31057 4  2  492
-8.29790- 4-2.27734- 4 1.10874- 3                                 1057 4  2  493
 0.00000+ 0 9.50000+ 5          0          0          9          01057 4  2  494
 4.46607- 1 2.64977- 1 1.22226- 1 3.31196- 2 2.53548- 3 8.12435- 41057 4  2  495
-3.20350- 4-9.59325- 6 6.32208- 4                                 1057 4  2  496
 0.00000+ 0 1.00000+ 6          0          0          9          01057 4  2  497
 4.44036- 1 2.34427- 1 1.60385- 1 5.60398- 2-1.66255- 3-1.19733- 21057 4  2  498
-5.47596- 3-6.54808- 4-1.81102- 4                                 1057 4  2  499
 0.00000+ 0 1.05000+ 6          0          0          9          01057 4  2  500
 4.41276- 1 2.95561- 1 1.91881- 1 9.82002- 2 3.02872- 2 2.45372- 31057 4  2  501
-2.20543- 3 5.81421- 4 9.84641- 4                                 1057 4  2  502
 0.00000+ 0 1.10000+ 6          0          0          9          01057 4  2  503
 4.35165- 1 2.65842- 1 1.81954- 1 8.31117- 2 1.67715- 2 2.72754- 31057 4  2  504
-1.38186- 3-1.74019- 4 1.45669- 3                                 1057 4  2  505
 0.00000+ 0 1.15000+ 6          0          0          9          01057 4  2  506
 4.16839- 1 2.45080- 1 1.67122- 1 7.48796- 2 9.71660- 3-2.07436- 41057 4  2  507
-6.75760- 5-1.71672- 4 9.60077- 4                                 1057 4  2  508
 0.00000+ 0 1.20000+ 6          0          0          9          01057 4  2  509
 4.30179- 1 2.73304- 1 1.83373- 1 8.56124- 2 2.14650- 2 3.72234- 31057 4  2  510
-2.01216- 3-6.12140- 6 1.49193- 3                                 1057 4  2  511
 0.00000+ 0 1.25000+ 6          0          0          9          01057 4  2  512
 4.20688- 1 2.59980- 1 1.97871- 1 9.35682- 2 1.51488- 2 1.63747- 31057 4  2  513
-8.29056- 4-3.19795- 4 1.50728- 3                                 1057 4  2  514
 0.00000+ 0 1.29500+ 6          0          0          9          01057 4  2  515
 4.30705- 1 2.73546- 1 2.03596- 1 1.09004- 1 3.02946- 2 3.54913- 31057 4  2  516
-2.35442- 3 1.82121- 4 1.52007- 3                                 1057 4  2  517
 0.00000+ 0 1.35000+ 6          0          0          9          01057 4  2  518
 3.98358- 1 2.39171- 1 1.85083- 1 9.64841- 2 2.01074- 2 1.26862- 31057 4  2  519
-1.02350- 3-6.37440- 5 1.25881- 3                                 1057 4  2  520
 0.00000+ 0 1.40000+ 6          0          0          9          01057 4  2  521
 4.30662- 1 2.59630- 1 1.96530- 1 1.04192- 1 2.08869- 2-6.75852- 41057 4  2  522
-4.56102- 4 1.44862- 4 9.11551- 4                                 1057 4  2  523
 0.00000+ 0 1.45000+ 6          0          0          9          01057 4  2  524
 4.26523- 1 2.70130- 1 2.08551- 1 1.16101- 1 3.10470- 2 2.08351- 31057 4  2  525
-1.90302- 3 2.87671- 4 1.29242- 3                                 1057 4  2  526
 0.00000+ 0 1.49500+ 6          0          0          9          01057 4  2  527
 4.48826- 1 3.06650- 1 2.38702- 1 1.53640- 1 6.37323- 2 9.13384- 31057 4  2  528
-6.01040- 3 9.57001- 4 2.09428- 3                                 1057 4  2  529
 0.00000+ 0 2.00000+ 6          0          0          9          01057 4  2  530
 5.51404- 1 3.72565- 1 3.00695- 1 1.98353- 1 7.42062- 2 1.59169- 21057 4  2  531
-2.43779- 3-6.30132- 3-6.63877- 3                                 1057 4  2  532
 0.00000+ 0 2.50000+ 6          0          0          9          01057 4  2  533
 6.55613- 1 4.93352- 1 3.51640- 1 2.63128- 1 1.38256- 1 4.50684- 21057 4  2  534
 3.95270- 3-5.35058- 3-3.64636- 3                                 1057 4  2  535
 0.00000+ 0 4.10000+ 6          0          0          9          01057 4  2  536
 7.63418- 1 6.20854- 1 4.92776- 1 3.95979- 1 2.67223- 1 1.54076- 11057 4  2  537
 8.43991- 2 4.30327- 2 1.65042- 2                                 1057 4  2  538
 0.00000+ 0 7.00000+ 6          0          0         20          01057 4  2  539
 7.85369- 1 6.48133- 1 5.49672- 1 4.48463- 1 3.39480- 1 2.31379- 11057 4  2  540
 1.48663- 1 9.49746- 2 5.69390- 2 2.71378- 2 6.95825- 3-2.41052- 31057 4  2  541
-5.28045- 3-6.68533- 3-7.40794- 3-6.81612- 3-5.51271- 3-4.32058- 31057 4  2  542
-3.26537- 3-1.84302- 3                                            1057 4  2  543
 0.00000+ 0 1.50000+ 7          0          0         20          01057 4  2  544
 8.82215- 1 7.63772- 1 6.54435- 1 5.69849- 1 4.99340- 1 4.44670- 11057 4  2  545
 3.92075- 1 3.47640- 1 3.00188- 1 2.56016- 1 2.00629- 1 1.36011- 11057 4  2  546
 7.69032- 2 3.83782- 2 1.67299- 2 6.10909- 3 2.11053- 3 5.47474- 41057 4  2  547
 1.73218- 4 4.66783- 5                                            1057 4  2  548
 0.00000+ 0 2.00000+ 7          0          0         20          01057 4  2  549
 8.82215- 1 7.63772- 1 6.54435- 1 5.69849- 1 4.99340- 1 4.44670- 11057 4  2  550
 3.92075- 1 3.47640- 1 3.00188- 1 2.56016- 1 2.00629- 1 1.36011- 11057 4  2  551
 7.69032- 2 3.83782- 2 1.67299- 2 6.10909- 3 2.11053- 3 5.47474- 41057 4  2  552
 1.73218- 4 4.66783- 5                                            1057 4  2  553
                                                                  1057 4  0  554
 9.52430+ 4 2.40940+ 2          0          2          0          01057 4 18  555
 0.00000+ 0 2.40940+ 2          0          1          0          01057 4 18  556
 0.00000+ 0 0.00000+ 0          0          0          1          21057 4 18  557
          2          2                                            1057 4 18  558
 0.00000+ 0 1.00000- 5          0          0          1          21057 4 18  559
          2          2                                            1057 4 18  560
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1057 4 18  561
 0.00000+ 0 2.00000+ 7          0          0          1          21057 4 18  562
          2          2                                            1057 4 18  563
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1057 4 18  564
                                                                  1057 4  0  565
 9.52430+ 4 2.40940+ 2          0          2          0          01057 4 91  566
 0.00000+ 0 2.40940+ 2          0          2          0          01057 4 91  567
 0.00000+ 0 0.00000+ 0          0          0          1          21057 4 91  568
          2          2                                            1057 4 91  569
 0.00000+ 0 8.40000+ 4          0          0          1          21057 4 91  570
          2          2                                            1057 4 91  571
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1057 4 91  572
 0.00000+ 0 2.00000+ 7          0          0          1          21057 4 91  573
          2          2                                            1057 4 91  574
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1057 4 91  575
                                                                  1057 4  0  576
                                                                  1057 0  0  577
 9.52430+ 4 2.40940+ 2          0          0          1          01057 5 18  578
-3.00000+ 7 0.00000+ 0          0          7          1          21057 5 18  579
          2          2                                            1057 5 18  580
 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1057 5 18  581
 0.00000+ 0 0.00000+ 0          0          0          1          31057 5 18  582
          3          2                                            1057 5 18  583
 1.00000- 5 1.36600+ 6 1.50000+ 7 1.36600+ 6 2.00000+ 7 1.36600+ 61057 5 18  584
                                                                  1057 5  0  585
 9.52430+ 4 2.40940+ 2          0          0          1          01057 5 91  586
 8.40000+ 4 0.00000+ 0          0          9          1          21057 5 91  587
          2          2                                            1057 5 91  588
 8.40000+ 4 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1057 5 91  589
 0.00000+ 0 0.00000+ 0          0          0          1         131057 5 91  590
         13          5                                            1057 5 91  591
 8.40000+ 4 1.00000+ 4 4.00000+ 5 1.34000+ 5 2.00000+ 6 2.98000+ 51057 5 91  592
 3.00000+ 6 3.65000+ 5 4.00000+ 6 4.21000+ 5 5.00000+ 6 4.71000+ 51057 5 91  593
 6.00000+ 6 5.16000+ 5 7.00000+ 6 5.58000+ 5 8.00000+ 6 5.96000+ 51057 5 91  594
 9.00000+ 6 6.32000+ 5 1.00000+ 7 6.66000+ 5 1.50000+ 7 8.02000+ 51057 5 91  595
 2.00000+ 7 9.15023+ 5                                            1057 5 91  596
                                                                  1057 5  0  597
                                                                  1057 0  0  598
                                                                     0 0  0  599
 9.42420+ 4 2.40145+ 2          1          1          0         451161 1451    1
 0.00000+ 0 0.00000+ 0          1          0        124          01161 1451    2
 94-pu-242 ai + anc   eval-may67 alter and dunford(ai) mod.by anc 1161 1451    3
 naa-sr-12271(may-67) dist-may74  rev-nov74                       1161 1451    4
 extended to 20 mev for endf/b version-iv   (apr74)               1161 1451    5
 added radioactive decay data (mf=1,mt=457) (apr74)               1161 1451    6
          *          *          *          *          *          *1161 1451    7
   mt=457 (rad. decay data) eval-feb74 by c.w.reich (anc)         1161 1451    8
             q(alpha)- 1973 revision of wapstra-gove mass table   1161 1451    9
             half-life- n.e. holden, chart of the nuclides (1973) 1161 1451   10
                         and private communication (jan.,1974).   1161 1451   11
             other- y.a. ellis, nuclear data b4, no.6, 683(1970)  1161 1451   12
   note  )e-alpha  = 4973. kev                                    1161 1451   13
           this value includes the kinetic energy of the alpha    1161 1451   14
           particles and the recoil energy of the daughter nuclei.1161 1451   15
   note   the internal-conversion coefficient is a theoretical    1161 1451   16
          value. the listed gamma-ray intensity was chosen so that1161 1451   17
          the total transition intensity of the gamma ray would   1161 1451   18
          agree with the alpha-branching data.                    1161 1451   19
          *          *          *          *          *          *1161 1451   20
 *         *          *          *         *          *         * 1161 1451   21
 this material is a modified version of mat=1055                  1161 1451   22
 *         *          *          *         *          *         * 1161 1451   23
 pu-242  anc  revised  aug 71  t.e.young and r.a.grimesey         1161 1451   24
 resolved resonance parameters and thermal energy cross sections  1161 1451   25
 were revised.no changes made above 390 ev.                       1161 1451   26
 the total cs below 1.0 ev is from  refs.16 and 17. capture and   1161 1451   27
 elastic cs below 1.0 ev calculated directly from resolved params.1161 1451   28
 the bound level was adjusted to fit the total cs below 1 ev and  1161 1451   29
 to give the same elastic cs at 0.0253 ev as calculated using the 1161 1451   30
 2.68 ev res only. parameters of the 2.68 ev res are from ref 16. 1161 1451   31
 energies and parameters of resonances above 20 ev are averages   1161 1451   32
 of values given in refs.3,4,14-17. the 0.0253 ev total cs is     1161 1451   33
 26.9+- 1barn,absorption is 18.5+-1barn, scattering is 8.4+- 1barn1161 1451   34
 14.r.e.cote et.al. phys.rev.114, 505(1959)                       1161 1451   35
 15.p.a.egelstaff et.al. j.nucl.energy 6.303(1958)                1161 1451   36
 16.t.e.young s.d.reeder, nucl.sc1.engr.40,389(1970)              1161 1451   37
 17.t.e.yount et.al. nucl.sc1.engr.43,341(1971)                   1161 1451   38
 pu-242    ai         eval-may67 alter and dunford                1161 1451   39
 naa-sr-12271(may,67) dist-jul68 rev-apr70                        1161 1451   40
 *         *          *          *         *          *           1161 1451   41
  data modified for endf/b-ii formats (april, 1970)               1161 1451   42
 *         *          *          *         *          *           1161 1451   43
      plutonium-242   revised july 14,1967                        1161 1451   44
                                                                  1161 1451   45
                                                                  1161 1451   46
  mf=1                general information                         1161 1451   47
    mt=452 nubar   no experimental data available. correlation of 1161 1451   48
       reference 1 is used.                                       1161 1451   49
    mt=453 radioactive decay data   all masses and decay constants1161 1451   50
       from ref. 2.                                               1161 1451   51
                                                                  1161 1451   52
  mf=2                resonance parameters                        1161 1451   53
    mt=151 resolved resonances   parameters for 11 single-level   1161 1451   54
       resonances are given (ref. 3 and 4). the fission widths are1161 1451   55
       taken as zero.  potential scattering of 10.71 barns based  1161 1451   56
       on deformed optical model.                                 1161 1451   57
           unresolved resonances   average resonance parameters   1161 1451   58
       obtained from resolved resonances and deformed optical     1161 1451   59
       model.                                                     1161 1451   60
           this data gives a resonance integral of 1103.7 barns in1161 1451   61
       fair agreement with 1275 barns measured (ref.5).           1161 1451   62
                                                                  1161 1451   63
  mf=3                smooth cross sections                       1161 1451   64
    mt=1   total cross section   thermal region obtained from     1161 1451   65
       resonance parameters with 2 barn constant scattering and   1161 1451   66
       11 barn 1/v capture added. 2200m/s value 39.1b compared to 1161 1451   67
       39. reported in ref. 6. fast region from deformed optical  1161 1451   68
       model(dom).                                                1161 1451   69
    mt=2   elastic scattering   data obtained in procedure        1161 1451   70
       idenical to mt=1.                                          1161 1451   71
    mt=4   inelastic scattering   data results from the scattering1161 1451   72
       to 10 levels plus continuum. again a dom is used with a    1161 1451   73
       statistical compound nucleus model.                        1161 1451   74
    mt=16  n,2n   calculation based on evaporation model (ref. 7).1161 1451   75
    mt=17  n,3n   same as mt=16                                   1161 1451   76
    mt=18  fission   thermal and resonance fission is assumed to  1161 1451   77
       be negligible. fast region data calculated from compound   1161 1451   78
       nucleus theory using the hill/wheeler model (ref. 8).      1161 1451   79
       the data are about 10 percent lower than that reported by  1161 1451   80
       (ref. 9), but are in good agreement with a recent evalu-   1161 1451   81
       ation by davy (ref. 10).                                   1161 1451   82
    mt=102 capture   thermal data calculated from resonance       1161 1451   83
       parameters and an 11 barn 1/v cross section added. 2200m/s 1161 1451   84
       value is 30.0b to agree with ref. 11. fast region data from1161 1451   85
       a statistical model assuming dipole radiation.             1161 1451   86
    mt=251 mubar   calculated from dom angular distributions      1161 1451   87
    mt=252 xibar   calculated from dom angular distributions      1161 1451   88
    mt=253 gamma   calculated from dom angular distributions      1161 1451   89
                                                                  1161 1451   90
  mf=4                legendre polynomials                        1161 1451   91
    mt=2   elastic scattering   legendre coefficints for 15th     1161 1451   92
       order fit to calculated angular distributions (dom) are    1161 1451   93
       provided between 10 kev and 11 mev and 19th order between  1161 1451   94
       12 and 15 mev.                                             1161 1451   95
                                                                  1161 1451   96
  mf=5                secondary energy distributions              1161 1451   97
    mt=2   inelastic scattering   calculated data for 10 levels   1161 1451   98
       plus continuum. direct scattering for the first excited    1161 1451   99
       level from threshold to 15mev plus compound nucleus        1161 1451  100
       scattering to 3 mev for all levels is included. continuum  1161 1451  101
       inelastic scattering is given by a maxwellian with an      1161 1451  102
       energy dependent temperature calculated from ref. 7.       1161 1451  103
    mt=16  n,2n   nuclear temperature with energy dependence as in1161 1451  104
       reference 12.                                              1161 1451  105
    mt=17  n,3n   nuclear temperature with energy dependence as in1161 1451  106
       reference 12.                                              1161 1451  107
    mt=18  fission   maxwellian with constant temperature from    1161 1451  108
       correlation of ref. 13.                                    1161 1451  109
                                                                  1161 1451  110
                                                                  1161 1451  111
                      references                                  1161 1451  112
    1.  shuster, s., howerton, r., ucrl 7389(1963)                1161 1451  113
    2.  goldman, d., roesser, j.,  chart of the nuclides (1966)   1161 1451  114
    3.  pattenden, n., eandc-50-s (1965)                          1161 1451  115
    4.  auchampaugh, g., et. al., phys.rev. 146,840 (1966)        1161 1451  116
    5.  butler, j., et.al., can.j.phys. 35,147 (1957)             1161 1451  117
    6.  young, t., wash 1068(1966)                                1161 1451  118
    7.  pearlstein, s., bnl 897(1964)                             1161 1451  119
    8.  hill, d., wheeler, j., phys.rev. 89,1102(1953)            1161 1451  120
    9.  butler, d., phys.rev. 117,1305 (1960)                     1161 1451  121
   10.  davy, w., nse 26,149 (1966)                               1161 1451  122
   11.  fields, r., et.al., nse 1,62 (1956)                       1161 1451  123
   12.  parker, k., awre0-79/63(1964)                             1161 1451  124
   13.  barnard, e., et.al., nucl.phys. 71,228(1965)              1161 1451  125
                                                                  1161 1451  126
                                1        451        171           1161 1451  127
                                1        452          3           1161 1451  128
                                1        453          7           1161 1451  129
                                1        457         13           1161 1451  130
                                2        151         33           1161 1451  131
                                3          1         37           1161 1451  132
                                3          2         28           1161 1451  133
                                3          4         21           1161 1451  134
                                3         16          7           1161 1451  135
                                3         17          5           1161 1451  136
                                3         18         20           1161 1451  137
                                3         51         21           1161 1451  138
                                3         52         15           1161 1451  139
                                3         53         13           1161 1451  140
                                3         54         11           1161 1451  141
                                3         55         11           1161 1451  142
                                3         56         10           1161 1451  143
                                3         57          9           1161 1451  144
                                3         58          9           1161 1451  145
                                3         59          8           1161 1451  146
                                3         60          8           1161 1451  147
                                3         91         11           1161 1451  148
                                3        102         28           1161 1451  149
                                3        251         16           1161 1451  150
                                3        252         16           1161 1451  151
                                3        253         16           1161 1451  152
                                4          2        228           1161 1451  153
                                4         16         10           1161 1451  154
                                4         17         10           1161 1451  155
                                4         18         10           1161 1451  156
                                4         51         10           1161 1451  157
                                4         52         10           1161 1451  158
                                4         53         10           1161 1451  159
                                4         54         10           1161 1451  160
                                4         55         10           1161 1451  161
                                4         56         10           1161 1451  162
                                4         57         10           1161 1451  163
                                4         58         10           1161 1451  164
                                4         59         10           1161 1451  165
                                4         60         10           1161 1451  166
                                4         91         10           1161 1451  167
                                5         16         10           1161 1451  168
                                5         17          9           1161 1451  169
                                5         18          7           1161 1451  170
                                5         91          7           1161 1451  171
                                                                  1161 1  0  172
 9.42420+ 4 2.40145+ 2          0          1          0          01161 1452  173
 0.00000+ 0 0.00000+ 0          0          0          2          01161 1452  174
 2.80800+ 0 1.42000- 7                                            1161 1452  175
                                                                  1161 1  0  176
 9.42420+ 4 2.40145+ 2          0          0          1          01161 1453  177
 9.42420+ 4 2.40145+ 2          0          0          2          21161 1453  178
 1.00000- 5 2.00000+ 7                                            1161 1453  179
 0.00000+ 0-6.24000+ 6          0          0          5          01161 1453  180
 1.60000+ 1 9.42410+ 4 1.69000- 9 1.00000+ 0 1.00000+ 0           1161 1453  181
 0.00000+ 0-1.17800+ 7          0          0          5          01161 1453  182
 1.70000+ 1 9.42400+ 4 3.25000-12 1.00000+ 0 1.00000+ 0           1161 1453  183
                                                                  1161 1  0  184
 9.42420+ 4 2.40145+ 2          0          0          0          21161 1457  185
 1.22044+13 3.15360+10          0          0          6          31161 1457  186
 0.00000+ 0 0.00000+ 0 9.50000+ 3 0.00000+ 0 4.97300+ 6 0.00000+ 01161 1457  187
 9.42420+ 4 2.40145+ 2          0          0         12          21161 1457  188
 4.00000+ 0 0.00000+ 0 4.98170+ 6 1.20000+ 3 1.00000+ 0 0.00000+ 01161 1457  189
 6.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 5.50000- 6 0.00000+ 01161 1457  190
 4.00000+ 0 0.00000+ 0          0          0         18          21161 1457  191
 1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01161 1457  192
 4.85570+ 6 1.20000+ 3 2.11000+ 1 0.00000+ 0 0.00000+ 0 0.00000+ 01161 1457  193
 4.90000+ 6 1.20000+ 3 7.89000+ 1 0.00000+ 0 0.00000+ 0 0.00000+ 01161 1457  194
 0.00000+ 0 0.00000+ 0          0          0         12          11161 1457  195
 1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01161 1457  196
 4.50000+ 4 0.00000+ 0 3.40000- 2 0.00000+ 0 6.23000+ 2 0.00000+ 01161 1457  197
                                                                  1161 1  0  198
                                                                  1161 0  0  199
 9.42420+ 4 2.40145+ 2          0          0          1          01161 2151  200
 9.42420+ 4 1.00000+ 0          0          0          2          01161 2151  201
 1.00000+ 0 3.90000+ 2          1          1          0          01161 2151  202
 0.00000+ 0 9.22500- 1          0          0          1          01161 2151  203
 2.40145+ 2 0.00000+ 0          0          0        126         211161 2151  204
-7.00000+ 1 5.00000- 1 1.84565- 1 1.58965- 1 2.56000- 2 0.00000+ 01161 2151  205
 2.68000+ 0 5.00000- 1 2.69970- 2 1.99700- 3 2.50000- 2 0.00000+ 01161 2151  206
 2.25400+ 1 5.00000- 1 2.59000- 2 3.00000- 4 2.56000- 2 0.00000+ 01161 2151  207
 4.09300+ 1 5.00000- 1 2.60497- 2 4.49700- 4 2.56000- 2 0.00000+ 01161 2151  208
 5.37000+ 1 5.00000- 1 7.63976- 2 5.07976- 2 2.56000- 2 0.00000+ 01161 2151  209
 6.80000+ 1 5.00000- 1 2.97973- 2 4.19730- 3 2.56000- 2 0.00000+ 01161 2151  210
 8.91000+ 1 5.00000- 1 4.37043- 2 1.81043- 2 2.56000- 2 0.00000+ 01161 2151  211
 1.06000+ 2 5.00000- 1 2.61971- 2 5.97100- 4 2.56000- 2 0.00000+ 01161 2151  212
 1.07500+ 2 5.00000- 1 4.34950- 2 1.78950- 2 2.56000- 2 0.00000+ 01161 2151  213
 1.31800+ 2 5.00000- 1 3.19027- 2 6.30270- 3 2.56000- 2 0.00000+ 01161 2151  214
 1.50000+ 2 5.00000- 1 4.25993- 2 1.69993- 2 2.56000- 2 0.00000+ 01161 2151  215
 1.66000+ 2 5.00000- 1 2.65997- 2 9.99700- 4 2.56000- 2 0.00000+ 01161 2151  216
 2.05000+ 2 5.00000- 1 9.11039- 2 6.55039- 2 2.56000- 2 0.00000+ 01161 2151  217
 2.17000+ 2 5.00000- 1 3.04464- 2 4.84640- 3 2.56000- 2 0.00000+ 01161 2151  218
 2.35000+ 2 5.00000- 1 3.34947- 2 7.89470- 3 2.56000- 2 0.00000+ 01161 2151  219
 2.76000+ 2 5.00000- 1 4.01530- 2 1.45530- 2 2.56000- 2 0.00000+ 01161 2151  220
 3.06000+ 2 5.00000- 1 4.09060- 2 1.53060- 2 2.56000- 2 0.00000+ 01161 2151  221
 3.11000+ 2 5.00000- 1 3.66040- 2 1.10040- 2 2.56000- 2 0.00000+ 01161 2151  222
 3.23000+ 2 5.00000- 1 2.54602- 1 2.29002- 1 2.56000- 2 0.00000+ 01161 2151  223
 3.35000+ 2 5.00000- 1 1.20098- 1 9.44980- 2 2.56000- 2 0.00000+ 01161 2151  224
 3.86000+ 2 5.00000- 1 7.28900- 2 4.72900- 2 2.56000- 2 0.00000+ 01161 2151  225
 3.90000+ 2 1.00000+ 4          2          1          0          01161 2151  226
 0.00000+ 0 9.22800- 1          0          0          2          01161 2151  227
 2.40145+ 2 0.00000+ 0          0          0          6          11161 2151  228
 1.84000+ 1 5.00000- 1 1.00000+ 0 3.25000- 3 2.45000- 2 0.00000+ 01161 2151  229
 2.40145+ 2 0.00000+ 0          1          0         12          21161 2151  230
 1.84000+ 1 5.00000- 1 1.00000+ 0 1.90000- 3 2.45000- 2 0.00000+ 01161 2151  231
 9.20000+ 0 1.50000+ 0 1.00000+ 0 1.06000- 3 2.45000- 2 0.00000+ 01161 2151  232
                                                                  1161 2  0  233
                                                                  1161 0  0  234
 9.42420+ 4 2.40145+ 2          0         99          0          01161 3  1  235
 0.00000+ 0 0.00000+ 0          0          0          4         991161 3  1  236
         22          5         26          3         98          51161 3  1  237
         99          2                                            1161 3  1  238
 1.00000- 5 9.60000+ 2 1.00000- 4 2.97150+ 2 5.00000- 4 1.39000+ 21161 3  1  239
 1.00000- 3 9.97730+ 1 2.00000- 3 7.30570+ 1 4.00000- 3 5.41840+ 11161 3  1  240
 7.00000- 3 4.30810+ 1 1.00000- 2 3.74770+ 1 1.70000- 2 3.08060+ 11161 3  1  241
 2.53000- 2 2.68680+ 1 4.00000- 2 2.32290+ 1 6.00000- 2 2.06630+ 11161 3  1  242
 8.00000- 2 1.91540+ 1 1.00000- 1 1.81390+ 1 1.50000- 1 1.65980+ 11161 3  1  243
 2.00000- 1 1.57180+ 1 3.00000- 1 1.47490+ 1 4.50000- 1 1.40960+ 11161 3  1  244
 6.00000- 1 1.38590+ 1 8.00000- 1 1.39070+ 1 9.00000- 1 1.40590+ 11161 3  1  245
 1.00000+ 0 1.43000+ 1 1.00000+ 0 0.00000+ 0 9.69000+ 3 0.00000+ 01161 3  1  246
 1.00000+ 4 0.00000+ 0 1.00000+ 4 1.77890+ 1 1.06500+ 4 1.75900+ 11161 3  1  247
 1.20000+ 4 1.72220+ 1 1.50000+ 4 1.65600+ 1 1.50000+ 4 1.65600+ 11161 3  1  248
 2.00000+ 4 1.58490+ 1 2.20000+ 4 1.55540+ 1 3.00000+ 4 1.46300+ 11161 3  1  249
 4.00000+ 4 1.38500+ 1 4.00000+ 4 1.38500+ 1 4.51000+ 4 1.35310+ 11161 3  1  250
 4.80000+ 4 1.33700+ 1 5.00000+ 4 1.32700+ 1 5.50000+ 4 1.29900+ 11161 3  1  251
 5.80000+ 4 1.28760+ 1 6.50000+ 4 1.25700+ 1 7.50000+ 4 1.22100+ 11161 3  1  252
 9.00000+ 4 1.17600+ 1 1.00000+ 5 1.15100+ 1 1.20000+ 5 1.10780+ 11161 3  1  253
 1.50000+ 5 1.05500+ 1 1.60000+ 5 1.04060+ 1 1.70000+ 5 1.02660+ 11161 3  1  254
 1.80000+ 5 1.01350+ 1 2.00000+ 5 9.90300+ 0 2.50000+ 5 9.40600+ 01161 3  1  255
 3.00000+ 5 9.04500+ 0 3.14000+ 5 8.94910+ 0 4.00000+ 5 8.49000+ 01161 3  1  256
 5.00000+ 5 8.09900+ 0 6.00000+ 5 7.81000+ 0 6.50000+ 5 7.62940+ 01161 3  1  257
 7.00000+ 5 7.59600+ 0 7.50000+ 5 7.49040+ 0 8.00000+ 5 7.42400+ 01161 3  1  258
 8.50000+ 5 7.34340+ 0 9.00000+ 5 7.29390+ 0 9.69000+ 5 7.21860+ 01161 3  1  259
 1.00000+ 6 7.19400+ 0 1.01400+ 6 7.17960+ 0 1.06500+ 6 7.14080+ 01161 3  1  260
 1.10000+ 6 7.12020+ 0 1.11500+ 6 7.11180+ 0 1.15000+ 6 7.08880+ 01161 3  1  261
 1.20000+ 6 7.06200+ 0 1.25000+ 6 7.02130+ 0 1.30000+ 6 6.99700+ 01161 3  1  262
 1.40000+ 6 6.97400+ 0 1.50000+ 6 6.96900+ 0 1.60000+ 6 6.96620+ 01161 3  1  263
 1.70000+ 6 6.97480+ 0 1.75000+ 6 6.96960+ 0 1.80000+ 6 6.96510+ 01161 3  1  264
 2.00000+ 6 6.98800+ 0 2.20000+ 6 7.05400+ 0 2.50000+ 6 7.22700+ 01161 3  1  265
 3.00000+ 6 7.45100+ 0 4.00000+ 6 7.54600+ 0 5.00000+ 6 7.38900+ 01161 3  1  266
 6.00000+ 6 7.10500+ 0 6.28000+ 6 6.96770+ 0 6.50000+ 6 6.88160+ 01161 3  1  267
 6.60000+ 6 6.85000+ 0 7.00000+ 6 6.71300+ 0 8.00000+ 6 6.35200+ 01161 3  1  268
 9.00000+ 6 6.16200+ 0 1.00000+ 7 6.01100+ 0 1.10000+ 7 5.94300+ 01161 3  1  269
 1.18300+ 7 5.89500+ 0 1.20000+ 7 5.90110+ 0 1.30000+ 7 5.92400+ 01161 3  1  270
 1.40000+ 7 6.00800+ 0 1.50000+ 7 6.12900+ 0 2.00000+ 7 6.12900+ 01161 3  1  271
                                                                  1161 3  0  272
 9.42420+ 4 2.40145+ 2          0         99          0          01161 3  2  273
 0.00000+ 0 0.00000+ 0          0          0          4         721161 3  2  274
         22          5         25          3         71          51161 3  2  275
         72          2                                            1161 3  2  276
 1.00000- 5 8.41200+ 0 1.00000- 4 8.40400+ 0 5.00000- 4 8.40300+ 01161 3  2  277
 1.00000- 3 8.40300+ 0 2.00000- 3 8.40200+ 0 4.00000- 3 8.40100+ 01161 3  2  278
 7.00000- 3 8.39800+ 0 1.00000- 2 8.39600+ 0 1.70000- 2 8.39000+ 01161 3  2  279
 2.53000- 2 8.38300+ 0 4.00000- 2 8.37000+ 0 6.00000- 2 8.35300+ 01161 3  2  280
 8.00000- 2 8.33500+ 0 1.00000- 1 8.31800+ 0 1.50000- 1 8.27200+ 01161 3  2  281
 2.00000- 1 8.22500+ 0 3.00000- 1 8.12500+ 0 4.50000- 1 7.96100+ 01161 3  2  282
 6.00000- 1 7.77600+ 0 8.00000- 1 7.48900+ 0 9.00000- 1 7.32400+ 01161 3  2  283
 1.00000+ 0 7.14300+ 0 1.00000+ 0 0.00000+ 0 1.00000+ 4 0.00000+ 01161 3  2  284
 1.00000+ 4 1.69960+ 1 1.50000+ 4 1.59480+ 1 2.00000+ 4 1.52990+ 11161 3  2  285
 3.00000+ 4 1.41590+ 1 4.00000+ 4 1.34310+ 1 5.00000+ 4 1.29020+ 11161 3  2  286
 5.50000+ 4 1.25450+ 1 6.50000+ 4 1.20320+ 1 7.50000+ 4 1.16160+ 11161 3  2  287
 9.00000+ 4 1.10950+ 1 1.00000+ 5 1.08040+ 1 1.20000+ 5 1.03110+ 11161 3  2  288
 1.50000+ 5 9.68230+ 0 2.00000+ 5 8.88930+ 0 2.50000+ 5 8.26830+ 01161 3  2  289
 3.00000+ 5 7.82330+ 0 4.00000+ 5 7.09580+ 0 5.00000+ 5 6.53160+ 01161 3  2  290
 6.00000+ 5 6.04300+ 0 7.00000+ 5 5.60980+ 0 8.00000+ 5 5.16060+ 01161 3  2  291
 9.00000+ 5 4.83320+ 0 1.00000+ 6 4.59830+ 0 1.10000+ 6 4.41010+ 01161 3  2  292
 1.20000+ 6 4.42780+ 0 1.30000+ 6 4.15460+ 0 1.40000+ 6 4.04130+ 01161 3  2  293
 1.50000+ 6 4.05420+ 0 1.60000+ 6 4.02540+ 0 1.80000+ 6 3.90010+ 01161 3  2  294
 2.00000+ 6 3.79920+ 0 2.20000+ 6 3.77670+ 0 2.50000+ 6 3.75970+ 01161 3  2  295
 3.00000+ 6 3.74480+ 0 4.00000+ 6 3.75270+ 0 5.00000+ 6 3.64370+ 01161 3  2  296
 6.00000+ 6 3.44700+ 0 6.60000+ 6 3.38880+ 0 7.00000+ 6 3.20970+ 01161 3  2  297
 8.00000+ 6 2.97500+ 0 9.00000+ 6 2.84000+ 0 1.00000+ 7 2.71700+ 01161 3  2  298
 1.10000+ 7 2.70530+ 0 1.20000+ 7 2.73430+ 0 1.30000+ 7 2.81000+ 01161 3  2  299
 1.40000+ 7 2.92190+ 0 1.50000+ 7 3.05390+ 0 2.00000+ 7 2.99239+ 01161 3  2  300
                                                                  1161 3  0  301
 9.42420+ 4 2.40145+ 2          0         99          0          01161 3  4  302
 0.00000+ 0-4.49000+ 4          0          0          3         531161 3  4  303
          2          3         52          5         53          21161 3  4  304
 4.51000+ 4 0.00000+ 0 4.80000+ 4 1.89000- 3 5.50000+ 4 1.15600- 11161 3  4  305
 5.80000+ 4 1.90000- 1 6.50000+ 4 2.74700- 1 7.50000+ 4 3.61200- 11161 3  4  306
 9.00000+ 4 4.59700- 1 1.00000+ 5 5.12100- 1 1.50000+ 5 6.98000- 11161 3  4  307
 1.60000+ 5 7.39150- 1 1.70000+ 5 7.68850- 1 1.80000+ 5 7.95180- 11161 3  4  308
 2.00000+ 5 8.46980- 1 2.50000+ 5 9.64900- 1 3.00000+ 5 1.03270+ 01161 3  4  309
 3.14000+ 5 1.05000+ 0 4.00000+ 5 1.14750+ 0 5.00000+ 5 1.21050+ 01161 3  4  310
 6.00000+ 5 1.22420+ 0 6.50000+ 5 1.17410+ 0 7.00000+ 5 1.23010+ 01161 3  4  311
 7.50000+ 5 1.26060+ 0 8.00000+ 5 1.29410+ 0 8.50000+ 5 1.26080+ 01161 3  4  312
 9.00000+ 5 1.23310+ 0 9.69000+ 5 1.17400+ 0 1.00000+ 6 1.14850+ 01161 3  4  313
 1.01400+ 6 1.15080+ 0 1.06500+ 6 1.16880+ 0 1.10000+ 6 1.18380+ 01161 3  4  314
 1.11500+ 6 1.16550+ 0 1.20000+ 6 1.05820+ 0 1.30000+ 6 1.27150+ 01161 3  4  315
 1.40000+ 6 1.43660+ 0 1.50000+ 6 1.55440+ 0 1.70000+ 6 1.66610+ 01161 3  4  316
 2.00000+ 6 1.76160+ 0 2.20000+ 6 1.82330+ 0 2.50000+ 6 1.94330+ 01161 3  4  317
 3.00000+ 6 1.99720+ 0 4.00000+ 6 2.03810+ 0 5.00000+ 6 1.98610+ 01161 3  4  318
 6.00000+ 6 1.74930+ 0 7.00000+ 6 1.29530+ 0 8.00000+ 6 9.30400- 11161 3  4  319
 9.00000+ 6 7.55070- 1 1.00000+ 7 6.70600- 1 1.10000+ 7 6.21780- 11161 3  4  320
 1.20000+ 7 5.87430- 1 1.30000+ 7 5.64170- 1 1.40000+ 7 5.47720- 11161 3  4  321
 1.50000+ 7 5.32570- 1 2.00000+ 7 5.32570- 1                      1161 3  4  322
                                                                  1161 3  0  323
 9.42420+ 4 2.40145+ 2          0         99          0          01161 3 16  324
 0.00000+ 0-6.24000+ 6          0          0          3         121161 3 16  325
          2          3         11          5         12          21161 3 16  326
 6.28000+ 6 0.00000+ 0 6.50000+ 6 8.41000- 3 7.00000+ 6 2.05200- 11161 3 16  327
 8.00000+ 6 4.72400- 1 9.00000+ 6 6.21200- 1 1.00000+ 7 6.99000- 11161 3 16  328
 1.10000+ 7 7.28800- 1 1.20000+ 7 7.08200- 1 1.30000+ 7 4.58500- 11161 3 16  329
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 3.47980- 1 2.77546- 1 2.21647- 1 1.70943- 1 1.09256- 1 5.37925- 21161 4  2  774
 1.98248- 2 7.17982- 3 1.83440- 3                                 1161 4  2  775
 0.00000+ 0 1.10000+ 7          0          0         15          01161 4  2  776
 8.71896- 1 7.56715- 1 6.60345- 1 5.82268- 1 5.07038- 1 4.37361- 11161 4  2  777
 3.68895- 1 3.06277- 1 2.49966- 1 2.01570- 1 1.40870- 1 7.86577- 21161 4  2  778
 3.37422- 2 1.26639- 2 3.76156- 3                                 1161 4  2  779
 0.00000+ 0 1.20000+ 7          0          0         19          01161 4  2  780
 8.76529- 1 7.61090- 1 6.60600- 1 5.81161- 1 5.09426- 1 4.46811- 11161 4  2  781
 3.83635- 1 3.28026- 1 2.72829- 1 2.25413- 1 1.66808- 1 1.01725- 11161 4  2  782
 4.87190- 2 2.00394- 2 6.81945- 3 1.93949- 3 5.58202- 4 1.19536- 41161 4  2  783
 4.15263- 5                                                       1161 4  2  784
 0.00000+ 0 1.30000+ 7          0          0         19          01161 4  2  785
 8.84315- 1 7.73042- 1 6.69298- 1 5.87944- 1 5.16493- 1 4.57173- 11161 4  2  786
 3.97197- 1 3.45895- 1 2.91864- 1 2.44156- 1 1.87646- 1 1.22817- 11161 4  2  787
 6.48773- 2 2.97710- 2 1.15242- 2 3.81313- 3 1.19906- 3 2.82637- 41161 4  2  788
 9.47590- 5                                                       1161 4  2  789
 0.00000+ 0 1.40000+ 7          0          0         19          01161 4  2  790
 8.94725- 1 7.91368- 1 6.86588- 1 6.03820- 1 5.30166- 1 4.70936- 11161 4  2  791
 4.11947- 1 3.62146- 1 3.08795- 1 2.60079- 1 2.04965- 1 1.42263- 11161 4  2  792
 8.20511- 2 4.19360- 2 1.83414- 2 6.97521- 3 2.36752- 3 6.30354- 41161 4  2  793
 2.09091- 4                                                       1161 4  2  794
 0.00000+ 0 1.50000+ 7          0          0         19          01161 4  2  795
 9.06148- 1 8.12559- 1 7.09707- 1 6.26701- 1 5.49622- 1 4.88537- 11161 4  2  796
 4.28621- 1 3.78085- 1 3.24610- 1 2.74616- 1 2.19960- 1 1.59987- 11161 4  2  797
 9.93110- 2 5.57016- 2 2.71617- 2 1.15581- 2 4.24304- 3 1.28596- 31161 4  2  798
 4.36915- 4                                                       1161 4  2  799
 0.00000+ 0 2.00000+ 7          0          0         19          01161 4  2  800
 9.06148- 1 8.12559- 1 7.09707- 1 6.26701- 1 5.49622- 1 4.88537- 11161 4  2  801
 4.28621- 1 3.78085- 1 3.24610- 1 2.74616- 1 2.19960- 1 1.59987- 11161 4  2  802
 9.93110- 2 5.57016- 2 2.71617- 2 1.15581- 2 4.24304- 3 1.28596- 31161 4  2  803
 4.36915- 4                                                       1161 4  2  804
                                                                  1161 4  0  805
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 16  806
 0.00000+ 0 2.40145+ 2          0          1          0          01161 4 16  807
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 16  808
          2          2                                            1161 4 16  809
 0.00000+ 0 6.28000+ 6          0          0          1          21161 4 16  810
          2          2                                            1161 4 16  811
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 16  812
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 16  813
          2          2                                            1161 4 16  814
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 16  815
                                                                  1161 4  0  816
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 17  817
 0.00000+ 0 2.40145+ 2          0          1          0          01161 4 17  818
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 17  819
          2          2                                            1161 4 17  820
 0.00000+ 0 1.18300+ 7          0          0          1          21161 4 17  821
          2          2                                            1161 4 17  822
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 17  823
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 17  824
          2          2                                            1161 4 17  825
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 17  826
                                                                  1161 4  0  827
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 18  828
 0.00000+ 0 2.40145+ 2          0          1          0          01161 4 18  829
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 18  830
          2          2                                            1161 4 18  831
 0.00000+ 0 1.00000- 5          0          0          1          21161 4 18  832
          2          2                                            1161 4 18  833
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 18  834
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 18  835
          2          2                                            1161 4 18  836
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 18  837
                                                                  1161 4  0  838
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 51  839
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 51  840
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 51  841
          2          2                                            1161 4 51  842
 0.00000+ 0 4.51000+ 4          0          0          1          21161 4 51  843
          2          2                                            1161 4 51  844
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 51  845
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 51  846
          2          2                                            1161 4 51  847
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 51  848
                                                                  1161 4  0  849
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 52  850
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 52  851
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 52  852
          2          2                                            1161 4 52  853
 0.00000+ 0 1.50000+ 5          0          0          1          21161 4 52  854
          2          2                                            1161 4 52  855
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 52  856
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 52  857
          2          2                                            1161 4 52  858
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 52  859
                                                                  1161 4  0  860
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 53  861
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 53  862
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 53  863
          2          2                                            1161 4 53  864
 0.00000+ 0 3.14000+ 5          0          0          1          21161 4 53  865
          2          2                                            1161 4 53  866
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 53  867
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 53  868
          2          2                                            1161 4 53  869
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 53  870
                                                                  1161 4  0  871
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 54  872
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 54  873
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 54  874
          2          2                                            1161 4 54  875
 0.00000+ 0 6.50000+ 5          0          0          1          21161 4 54  876
          2          2                                            1161 4 54  877
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 54  878
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 54  879
          2          2                                            1161 4 54  880
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 54  881
                                                                  1161 4  0  882
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 55  883
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 55  884
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 55  885
          2          2                                            1161 4 55  886
 0.00000+ 0 7.00000+ 5          0          0          1          21161 4 55  887
          2          2                                            1161 4 55  888
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 55  889
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 55  890
          2          2                                            1161 4 55  891
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 55  892
                                                                  1161 4  0  893
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 56  894
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 56  895
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 56  896
          2          2                                            1161 4 56  897
 0.00000+ 0 8.00000+ 5          0          0          1          21161 4 56  898
          2          2                                            1161 4 56  899
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 56  900
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 56  901
          2          2                                            1161 4 56  902
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 56  903
                                                                  1161 4  0  904
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 57  905
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 57  906
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 57  907
          2          2                                            1161 4 57  908
 0.00000+ 0 9.69000+ 5          0          0          1          21161 4 57  909
          2          2                                            1161 4 57  910
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 57  911
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 57  912
          2          2                                            1161 4 57  913
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 57  914
                                                                  1161 4  0  915
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 58  916
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 58  917
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 58  918
          2          2                                            1161 4 58  919
 0.00000+ 0 1.01400+ 6          0          0          1          21161 4 58  920
          2          2                                            1161 4 58  921
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 58  922
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 58  923
          2          2                                            1161 4 58  924
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 58  925
                                                                  1161 4  0  926
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 59  927
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 59  928
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 59  929
          2          2                                            1161 4 59  930
 0.00000+ 0 1.06500+ 6          0          0          1          21161 4 59  931
          2          2                                            1161 4 59  932
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 59  933
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 59  934
          2          2                                            1161 4 59  935
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 59  936
                                                                  1161 4  0  937
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 60  938
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 60  939
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 60  940
          2          2                                            1161 4 60  941
 0.00000+ 0 1.11500+ 6          0          0          1          21161 4 60  942
          2          2                                            1161 4 60  943
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 60  944
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 60  945
          2          2                                            1161 4 60  946
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 60  947
                                                                  1161 4  0  948
 9.42420+ 4 2.40145+ 2          0          2          0          01161 4 91  949
 0.00000+ 0 2.40145+ 2          0          2          0          01161 4 91  950
 0.00000+ 0 0.00000+ 0          0          0          1          21161 4 91  951
          2          2                                            1161 4 91  952
 0.00000+ 0 1.20000+ 6          0          0          1          21161 4 91  953
          2          2                                            1161 4 91  954
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 91  955
 0.00000+ 0 2.00000+ 7          0          0          1          21161 4 91  956
          2          2                                            1161 4 91  957
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1161 4 91  958
                                                                  1161 4  0  959
                                                                  1161 0  0  960
 9.42420+ 4 2.40145+ 2          0          0          1          01161 5 16  961
 6.28000+ 6 0.00000+ 0          0          9          1          21161 5 16  962
          2          2                                            1161 5 16  963
 6.28000+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1161 5 16  964
 0.00000+ 0 0.00000+ 0          0          0          1         121161 5 16  965
         12          2                                            1161 5 16  966
 6.28000+ 6 1.00000+ 4 6.50000+ 6 5.20000+ 4 7.00000+ 6 1.52000+ 51161 5 16  967
 8.00000+ 6 2.94000+ 5 9.00000+ 6 3.76300+ 5 1.00000+ 7 4.59000+ 51161 5 16  968
 1.10000+ 7 5.42000+ 5 1.20000+ 7 6.24000+ 5 1.30000+ 7 7.07000+ 51161 5 16  969
 1.40000+ 7 7.90000+ 5 1.50000+ 7 8.73000+ 5 2.00000+ 7 1.28800+ 61161 5 16  970
                                                                  1161 5  0  971
 9.42420+ 4 2.40145+ 2          0          0          1          01161 5 17  972
 1.18300+ 7 0.00000+ 0          0          9          1          51161 5 17  973
          5          2                                            1161 5 17  974
 1.18300+ 7 1.00000+ 0 1.20000+ 7 1.00000+ 0 1.30000+ 7 1.00000+ 01161 5 17  975
 1.40000+ 7 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1161 5 17  976
 0.00000+ 0 0.00000+ 0          0          0          1          61161 5 17  977
          6          2                                            1161 5 17  978
 1.18300+ 7 1.00000+ 4 1.20000+ 7 4.40000+ 4 1.30000+ 7 2.44000+ 51161 5 17  979
 1.40000+ 7 3.27000+ 5 1.50000+ 7 4.10000+ 5 2.00000+ 7 8.25000+ 51161 5 17  980
                                                                  1161 5  0  981
 9.42420+ 4 2.40145+ 2          0          0          1          01161 5 18  982
-3.00000+ 7 0.00000+ 0          0          7          1          21161 5 18  983
          2          2                                            1161 5 18  984
 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1161 5 18  985
 0.00000+ 0 0.00000+ 0          0          0          1          31161 5 18  986
          3          5                                            1161 5 18  987
 1.00000- 5 1.33974+ 6 1.50000+ 7 1.33974+ 6 2.00000+ 7 1.33974+ 61161 5 18  988
                                                                  1161 5  0  989
 9.42420+ 4 2.40145+ 2          0          0          1          01161 5 91  990
 1.20000+ 6 0.00000+ 0          0          9          1          21161 5 91  991
          2          2                                            1161 5 91  992
 1.20000+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1161 5 91  993
 0.00000+ 0 0.00000+ 0          0          0          1          31161 5 91  994
          3          5                                            1161 5 91  995
 1.20000+ 6 2.24040+ 5 1.50000+ 7 7.61030+ 5 2.00000+ 7 8.74766+ 51161 5 91  996
                                                                  1161 5  0  997
                                                                  1161 0  0  998
                                                                     0 0  0  999
 9.62440+ 4 2.42133+ 2          1          1          0         451162 1451    1
 0.00000+ 0 0.00000+ 0          1          0        125          01162 1451    2
 96-cm-244 ai + anc   eval-may67 alter and dunford(ai) mod.by anc 1162 1451    3
 naa-sr-12271(may-67) dist-may74  rev-nov74                       1162 1451    4
 extended to 20 mev for endf/b version-iv   (apr74)               1162 1451    5
 added radioactive decay data (mf=1,mt=457) (apr74)               1162 1451    6
 *         *          *          *         *          *          *1162 1451    7
          *          *          *          *          *          *1162 1451    8
   mt=457 (rad. decay data) eval-feb74 by c.w.reich (anc)         1162 1451    9
 references  q(alpha)-1973 revision of wapstra-gove mass table.   1162 1451   10
             other- y.a.ellis and a.h. wapstra, nuclear data      1162 1451   11
                     b 3, no.2, 13 (1969)  see also,m.r. schmorak,1162 1451   12
           nuclear data b 4, no.6, 661 (1970)                     1162 1451   13
   note  )e-alpha  =  5892. kev.                                  1162 1451   14
          this value includes the alpha-particle kinetic energy   1162 1451   15
          and the daughter-nucleus recoil energy                  1162 1451   16
   note   the gamma-ray intensity data are taken from the two     1162 1451   17
          listed references. the intensities of the two lowest-   1162 1451   18
          energy gammas have been adjusted so that their total    1162 1451   19
          transition intensities agree with the alpha-branching   1162 1451   20
          (and using theoretical values for the associated        1162 1451   21
          internal-conversion coefficients). the higher-energy    1162 1451   22
          gammas have their intensities normalized so that        1162 1451   23
           i(597)+i(554)= 0.00014 percent per decay.              1162 1451   24
          *          *          *          *          *          *1162 1451   25
 this material is a modified version of mat=1058                  1162 1451   26
 *         *          *          *         *          *          *1162 1451   27
 cm-244  anc  revised aug 15-71   j.r.berreth and r.a.grimesey    1162 1451   28
 resonance and thermal cs revised by anc to 500 ev, unresolved    1162 1451   29
 parameters partially revised to conform to new resolved data.    1162 1451   30
 the low energy resonances to 85.8 ev are a composite of three    1162 1451   31
  sets of data,cote et.al.(3),m.s.moore et.al(9),j.r.berreth and  1162 1451   32
 f.b.simpson(10). the moore data are capture and fission measureme1162 1451   33
 nts,the other two are total cs measurements. the fission width   1162 1451   34
 for the 16.8 ev resonance is an indirect determination by m.s.   1162 1451   35
 moore. the fission width for the 7.66 ev resonance is an average 1162 1451   36
 of several large low lying resonances. the -1.48 ev resonance    1162 1451   37
 was adjusted to fit the measured total cs shape and the cs data  1162 1451   38
 at 0.0253 ev. smooth data below 3.0 ev are based on the          1162 1451   39
 resolved parameters in file  2 after reflecting all positive     1162 1451   40
 energy resonances to the negative axis to approximate bound      1162 1451   41
 states. the smooth data from 3.0 ev to 150 ev were obtained by   1162 1451   42
 subtracting the data for 1 bound state from the data for all     1162 1451   43
 bound states.the file 3 data for scattering is approximated      1162 1451   44
 above 5.0 ev.                                                    1162 1451   45
  9. m.s.moore and g.a.keyworth,phys.rev. 3. c1656(1971)          1162 1451   46
 10. j.r.berreth and f.b.simpson, anc to be published             1162 1451   47
 *         *          *          *         *          *         * 1162 1451   48
 data modified june,1970 to conform to endf/b-ii formats          1162 1451   49
 *         *          *          *         *          *         * 1162 1451   50
      curium-244      revised july 14,1967                        1162 1451   51
                                                                  1162 1451   52
  evaluated by atomics international                              1162 1451   53
  documentation - naa-sr-12271  may 1,1967 + supp. 1, july 14,19671162 1451   54
                                                                  1162 1451   55
  mf=1                general information                         1162 1451   56
    mt=452 nubar   no experimental data available. correlation of 1162 1451   57
       reference 1 is used.                                       1162 1451   58
    mt=453 radioactive decay data   all masses and decay constants1162 1451   59
       from ref. 2.                                               1162 1451   60
                                                                  1162 1451   61
  mf=2                resonance parameters                        1162 1451   62
    mt=151 resolved resonances   parameters for 15 single-level   1162 1451   63
       resonances are given (ref. 3). fission widths are taken as 1162 1451   64
       0.1 and 0.5 times the neutron width for large and small    1162 1451   65
       widths respectively.  potential scattering of 10.72 barns  1162 1451   66
       based on deformed optical model.                           1162 1451   67
           unresolved resonances   average resonance parameters   1162 1451   68
       obtained from resolved resonances and deformed optical     1162 1451   69
       model.                                                     1162 1451   70
           this data gives a resonance integral of 664.0 barns. no1162 1451   71
       experimental data available.                               1162 1451   72
                                                                  1162 1451   73
  mf=3                smooth cross sections                       1162 1451   74
    mt=1   total cross section   thermal region obtained from     1162 1451   75
       resonance parameters. 2200m/s value 36.42 barns. fast      1162 1451   76
       region from a deformed optical model calculation.          1162 1451   77
    mt=2   elastic scattering   data obtained in procedure        1162 1451   78
       idenical to mt=1.                                          1162 1451   79
    mt=4   inelastic scattering   data results from the scattering1162 1451   80
       to 10 levels plus continuum. again a dom is used with a    1162 1451   81
       statistical compound nucleus model.                        1162 1451   82
    mt=16  n,2n   calculation based on evaporation model (ref. 4).1162 1451   83
    mt=17  n,3n   same as mt=16                                   1162 1451   84
    mt=18  fission   thermal region data calculated from resonance1162 1451   85
       parameters. 2200m/s value is 1.674b calculated according to1162 1451   86
       the correlation of prince (ref. 5). fast region data       1162 1451   87
       calculated from compound nucleus theory using the hill-    1162 1451   88
       wheeler model(ref. 6).                                     1162 1451   89
    mt=102 capture   thermal data calculated from resonance       1162 1451   90
       parameters. 2200m/s value is 25.25b. fast region data from 1162 1451   91
       a statistical model assuming dipole radiation.             1162 1451   92
    mt=251 mubar   calculated from dom angular distributions      1162 1451   93
    mt=252 xibar   calculated from dom angular distributions      1162 1451   94
    mt=253 gamma   calculated from dom angular distributions      1162 1451   95
                                                                  1162 1451   96
  mf=4                legendre polynomials                        1162 1451   97
    mt=2   elastic scattering   legendre coefficints for 15th     1162 1451   98
       order fit to calculated angular distributions (dom) are    1162 1451   99
       provided between 10 kev and 11 mev and 19th order between  1162 1451  100
       12 and 15 mev.                                             1162 1451  101
                                                                  1162 1451  102
  mf=5                secondary energy distributions              1162 1451  103
    mt=2   inelastic scattering   calculated data for 10 levels   1162 1451  104
       plus continuum. direct scattering for the first excited    1162 1451  105
       level from threshold to 15mev plus compound nucleus        1162 1451  106
       scattering to 3 mev for all levels is included. continuum  1162 1451  107
       inelastic scattering is given by a maxwellian with an      1162 1451  108
       energy dependent temperature calculated from ref. 4.       1162 1451  109
    mt=16  n,2n   nuclear temperature with energy dependence as in1162 1451  110
       reference 7.                                               1162 1451  111
    mt=17  n,3n   nuclear temperature with energy dependence as in1162 1451  112
       reference 7.                                               1162 1451  113
    mt=18  fission   maxwellian with constant temperature from    1162 1451  114
       correlation of ref. 8.                                     1162 1451  115
                                                                  1162 1451  116
                                                                  1162 1451  117
                      references                                  1162 1451  118
    1.  gordeeva,l.,smirenkin,g., aere-trans. 956(1963)           1162 1451  119
    2.  goldman, d., roesser, j.,  chart of the nuclides (1966)   1162 1451  120
    3.  cote,r., et.al., phys.rev. 134, b1281(1964)               1162 1451  121
    4.  pearlstein, s., bnl 897(1964)                             1162 1451  122
    5.  prince,a., gemp-411(1966)                                 1162 1451  123
    6.  hill, d., wheeler, j., phys.rev. 89,1102(1953)            1162 1451  124
    7.  parker, k., awre0-79/63(1964)                             1162 1451  125
    8.  barnard, e., et.al., nucl.phys. 71,228(1965)              1162 1451  126
                                                                  1162 1451  127
                                1        451        172           1162 1451  128
                                1        452          3           1162 1451  129
                                1        453          7           1162 1451  130
                                1        457         31           1162 1451  131
                                2        151         55           1162 1451  132
                                3          1         39           1162 1451  133
                                3          2         34           1162 1451  134
                                3          4         21           1162 1451  135
                                3         16          7           1162 1451  136
                                3         17          5           1162 1451  137
                                3         18         34           1162 1451  138
                                3         51         21           1162 1451  139
                                3         52         18           1162 1451  140
                                3         53         16           1162 1451  141
                                3         54         15           1162 1451  142
                                3         55         14           1162 1451  143
                                3         56         13           1162 1451  144
                                3         57         12           1162 1451  145
                                3         58         12           1162 1451  146
                                3         59         11           1162 1451  147
                                3         60         11           1162 1451  148
                                3         91         11           1162 1451  149
                                3        102         34           1162 1451  150
                                3        251         16           1162 1451  151
                                3        252         16           1162 1451  152
                                3        253         16           1162 1451  153
                                4          2        235           1162 1451  154
                                4         16         10           1162 1451  155
                                4         17         10           1162 1451  156
                                4         18         10           1162 1451  157
                                4         51         10           1162 1451  158
                                4         52         10           1162 1451  159
                                4         53         10           1162 1451  160
                                4         54         10           1162 1451  161
                                4         55         10           1162 1451  162
                                4         56         10           1162 1451  163
                                4         57         10           1162 1451  164
                                4         58         10           1162 1451  165
                                4         59         10           1162 1451  166
                                4         60         10           1162 1451  167
                                4         91         10           1162 1451  168
                                5         16         10           1162 1451  169
                                5         17          9           1162 1451  170
                                5         18          7           1162 1451  171
                                5         91         13           1162 1451  172
                                                                  1162 1  0  173
 9.62440+ 4 2.42133+ 2          0          1          0          01162 1452  174
 0.00000+ 0 0.00000+ 0          0          0          2          01162 1452  175
 3.23000+ 0 1.30000- 7                                            1162 1452  176
                                                                  1162 1  0  177
 9.62440+ 4 2.42133+ 2          0          0          1          01162 1453  178
 9.62440+ 4 2.42133+ 2          0          0          2          21162 1453  179
 1.00000- 5 2.00000+ 7                                            1162 1453  180
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 1.60000+ 1 9.62430+ 4 6.87000-10 1.00000+ 0 1.00000+ 0           1162 1453  182
 0.00000+ 0-1.23600+ 7          0          0          5          01162 1453  183
 1.70000+ 1 9.62420+ 4 4.92000- 8 1.00000+ 0 1.00000+ 0           1162 1453  184
                                                                  1162 1  0  185
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 8.60700+ 5 0.00000+ 0 1.00000- 8 9.50000+ 6 0.00000+ 0 0.00000+ 01162 1457  216
                                                                  1162 1  0  217
                                                                  1162 0  0  218
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 5.00000+ 2 1.00000+ 4          2          1          0          01162 2151  260
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 5.00000+ 2 1.00000+ 4                                            1162 2151  262
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 1.30300- 3 1.62700- 2                                            1162 2151  266
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 1.30300- 3 1.62700- 2                                            1162 2151  270
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                                                                  1162 2  0  274
                                                                  1162 0  0  275
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        105          2                                            1162 3  1  279
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                                                                  1162 3  0  315
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 2.00000+ 7 2.99530+ 0                                            1162 3  2  349
                                                                  1162 3  0  350
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          2          2                                            1162 5 91 1096
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 0.00000+ 0 0.00000+ 0          0          0          1         191162 5 91 1098
         19          5                                            1162 5 91 1099
 1.00000+ 6 2.15515+ 5 1.50000+ 6 2.40953+ 5 1.70000+ 6 2.56514+ 51162 5 91 1100
 2.00000+ 6 2.78229+ 5 2.50000+ 6 3.11069+ 5 3.00000+ 6 3.40759+ 51162 5 91 1101
 4.00000+ 6 3.93475+ 5 5.00000+ 6 4.39918+ 5 6.00000+ 6 4.81906+ 51162 5 91 1102
 7.00000+ 6 5.20518+ 5 8.00000+ 6 5.56458+ 5 9.00000+ 6 5.90212+ 51162 5 91 1103
 1.00000+ 7 6.22138+ 5 1.10000+ 7 6.52504+ 5 1.20000+ 7 6.81519+ 51162 5 91 1104
 1.30000+ 7 7.09347+ 5 1.40000+ 7 7.36124+ 5 1.50000+ 7 7.61961+ 51162 5 91 1105
 2.00000+ 7 8.79838+ 5                                            1162 5 91 1106
                                                                  1162 5  0 1107
                                                                  1162 0  0 1108
                                                                     0 0  0 1109
 9.22360+ 4 2.34017+ 2          1          1          0         371163 1451    1
 0.00000+ 0 0.00000+ 0          1          0         55          01163 1451    2
 92-u -236 srl        eval-oct71 j. mccrosson                     1163 1451    3
                      dist-may74  rev-nov74                       1163 1451    4
 extended to 20 mev for endf/b version-iv   (apr74)               1163 1451    5
 added radioactive decay data (mf=1,mt=457) (apr74)               1163 1451    6
          *          *          *          *          *          *1163 1451    7
evaluation of u-236, oct. 1971 (savannah river lab)               1163 1451    8
    *         *         *         *         *         *         * 1163 1451    9
above 1 kev the evaluation of neutron cross sections is documented1163 1451   10
by drake and nichols in report ga-8135.  below 1 kev the neutron  1163 1451   11
cross sections are taken from measurements by carlson et al.      1163 1451   12
reported in ga-9057.                                              1163 1451   13
    *         *         *         *         *         *         * 1163 1451   14
mf= 1 mt=452   nu=2.37+.000000135e (same as u-234) ref.3          1163 1451   15
mf= 1 mt=453   decay data taken from 1965 chart of the nuclides   1163 1451   16
          *          *          *          *          *          *1163 1451   17
 mf= 1 mt=457 (rad. decay data) eval-feb74 by c.w.reich (anc)     1163 1451   18
             q(alpha)- 1973 revision of wapstra-gove mass table   1163 1451   19
             half-life- n.e. holden, chart of the nuclides (1973) 1163 1451   20
                         and private communication (jan.,1974).   1163 1451   21
             other- m.r. schmorak, nucl. data b 4,no.6, 623(1970).1163 1451   22
  note   )e-alpha  = 4556. kev.                                   1163 1451   23
          this value includes the kinetic energies of both the    1163 1451   24
          alpha particle and the recoiling daughter nucleus.      1163 1451   25
    note   the internal-conversion coefficients are theoretical   1163 1451   26
           values. the gamma-ray intensities are derived from     1163 1451   27
           these values, with the requirement that the total      1163 1451   28
           transition intensity agree with that given by the      1163 1451   29
           alpha-particle branching data.                         1163 1451   30
          *          *          *          *          *          *1163 1451   31
mf= 2 mt=151   resonance parameters taken from ref.2              1163 1451   32
mf= 3 mt=  1   total cross sections taken from ref. 1 and 4.      1163 1451   33
mf= 3 mt=  2   elastic cross sections, ref. 1 and 4.              1163 1451   34
mf= 3 mt=  4   inelas. cross sect.,ref. 1 and 4, q-value, ref. 5. 1163 1451   35
mf= 3 mt= 16   (n,2n) cross sect., ref. 1 and 4, q-value, ref. 6. 1163 1451   36
mf= 3 mt= 17   (n,3n) cross sect., ref. 1 and 4, q-value, ref. 7. 1163 1451   37
mf= 3 mt= 18   fission cross sect., ref. 1 and 4, q-value, ref. 8.1163 1451   38
mf= 3 mt=102   (n,gamma) cross sections, ref. 1.                  1163 1451   39
mf= 3 mt=251,252,253 calculated by chad                           1163 1451   40
mf= 4 mt=  2   diff. elast. same as for th-232, ref. 10.          1163 1451   41
mf= 5 mt=  4   data for 6 levels plus continuum, ref. 1 and 4.    1163 1451   42
mf= 5 mt=16    (n,2n) energy dist described by maxwellian.        1163 1451   43
mf= 5 mt=17    (n,3n) energy dist described by maxwellian.        1163 1451   44
mf= 5 mt=18    fiss. neutron energy dist given by simple fiss.    1163 1451   45
               spectrum plus maxwellian.                          1163 1451   46
    *         *         *    references     *         *         * 1163 1451   47
    1.   drake and nichols,ga-8135 (1967).                        1163 1451   48
    2.   carlson et al.,ga-9057 (1968).                           1163 1451   49
    3.   mather et al.,nucl. phys.,66 (1965).                     1163 1451   50
    4.   parker,awre-o-30/64 (1964).                              1163 1451   51
    5.   lederer et al.,table of isotopes,wiley,6th ed.(1968).    1163 1451   52
    6.   maples et al.,ucrl-16964 (1966).                         1163 1451   53
    7.   howerton et al.,ucrl-14000 (1964).                       1163 1451   54
    8.   a. prince, private communication (april 1968).           1163 1451   55
    9.   davey,nucl. sci. + eng.,26 (1966).                       1163 1451   56
   10.   drake and nichols,ga-6404 (1966).                        1163 1451   57
                                1        451         94           1163 1451   58
                                1        452          3           1163 1451   59
                                1        453          9           1163 1451   60
                                1        457         15           1163 1451   61
                                2        151         41           1163 1451   62
                                3          1         40           1163 1451   63
                                3          2         29           1163 1451   64
                                3          4         21           1163 1451   65
                                3         16         10           1163 1451   66
                                3         17          6           1163 1451   67
                                3         18         17           1163 1451   68
                                3         51         12           1163 1451   69
                                3         52         10           1163 1451   70
                                3         53          9           1163 1451   71
                                3         54          8           1163 1451   72
                                3         55          7           1163 1451   73
                                3         56          6           1163 1451   74
                                3         91         16           1163 1451   75
                                3        102         29           1163 1451   76
                                3        251         31           1163 1451   77
                                3        252         31           1163 1451   78
                                3        253         31           1163 1451   79
                                4          2        279           1163 1451   80
                                4         16         10           1163 1451   81
                                4         17         10           1163 1451   82
                                4         18         10           1163 1451   83
                                4         51         10           1163 1451   84
                                4         52         10           1163 1451   85
                                4         53         10           1163 1451   86
                                4         54         10           1163 1451   87
                                4         55         10           1163 1451   88
                                4         56         10           1163 1451   89
                                4         91         10           1163 1451   90
                                5         16          7           1163 1451   91
                                5         17          7           1163 1451   92
                                5         18          7           1163 1451   93
                                5         91          7           1163 1451   94
                                                                  1163 1  0   95
 9.22360+ 4 2.34017+ 2          0          1          0          01163 1452   96
 0.00000+ 0 0.00000+ 0          0          0          2          01163 1452   97
 2.37000+ 0 1.35000- 7                                            1163 1452   98
                                                                  1163 1  0   99
 9.22360+ 4 2.34017+ 2          0          0          1          01163 1453  100
 9.22360+ 4 2.34017+ 2          0          0          2          31163 1453  101
 1.00000- 5 2.00000+ 7                                            1163 1453  102
 0.00000+ 0-6.91040+ 6          0          0          5          01163 1453  103
 1.60000+ 1 9.22350+ 4 3.06800-16 1.00000+ 0 1.00000+ 0           1163 1453  104
 0.00000+ 0-1.16400+ 7          0          0          5          01163 1453  105
 1.70000+ 1 9.22340+ 4 8.82300-13 1.00000+ 0 1.00000+ 0           1163 1453  106
 0.00000+ 0 5.12440+ 6          0          0          5          01163 1453  107
 1.02000+ 2 9.22370+ 4 1.18300- 5 1.00000+ 0 1.00000+ 0           1163 1453  108
                                                                  1163 1  0  109
 9.22360+ 4 2.34017+ 2          0          0          0          21163 1457  110
 7.38573+14 9.46080+11          0          0          6          31163 1457  111
 0.00000+ 0 0.00000+ 0 1.34000+ 4 0.00000+ 0 4.55600+ 6 0.00000+ 01163 1457  112
 9.22360+ 4 2.34017+ 2          0          0         12          21163 1457  113
 4.00000+ 0 0.00000+ 0 4.56920+ 6 2.40000+ 3 1.00000+ 0 0.00000+ 01163 1457  114
 6.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 1.20000- 9 0.00000+ 01163 1457  115
 4.00000+ 0 0.00000+ 0          0          0         24          31163 1457  116
 1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01163 1457  117
 4.33100+ 6 8.00000+ 3 2.60000- 1 0.00000+ 0 0.00000+ 0 0.00000+ 01163 1457  118
 4.44300+ 6 5.00000+ 3 2.60000+ 1 0.00000+ 0 0.00000+ 0 0.00000+ 01163 1457  119
 4.49300+ 6 3.00000+ 3 7.40000+ 1 0.00000+ 0 0.00000+ 0 0.00000+ 01163 1457  120
 0.00000+ 0 0.00000+ 0          0          0         18          21163 1457  121
 1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01163 1457  122
 4.97500+ 4 2.50000+ 2 0.00000+ 0 8.30000- 2 3.17000+ 2 0.00000+ 01163 1457  123
 1.12700+ 5 0.00000+ 0 3.30000- 2 0.00000+ 0 6.80000+ 0 0.00000+ 01163 1457  124
                                                                  1163 1  0  125
                                                                  1163 0  0  126
 9.22360+ 4 2.34017+ 2          0          0          1          01163 2151  127
 9.22360+ 4 1.00000+ 0          0          0          2          01163 2151  128
 1.00000- 5 4.15000+ 2          1          1          0          01163 2151  129
 0.00000+ 0 9.35400- 1          0          0          1          01163 2151  130
 2.34017+ 2 0.00000+ 0          0          0        174         291163 2151  131
-9.70000+ 0 5.00000- 1 2.88800- 2 4.98300- 3 2.39000- 2 0.00000+ 01163 2151  132
 5.45000+ 0 5.00000- 1 2.66600- 2 2.16000- 3 2.45000- 2 0.00000+ 01163 2151  133
 2.97000+ 1 5.00000- 1 2.44800- 2 5.85000- 4 2.39000- 2 0.00000+ 01163 2151  134
 3.40000+ 1 5.00000- 1 2.32500- 2 2.35000- 3 2.09000- 2 0.00000+ 01163 2151  135
 4.37000+ 1 5.00000- 1 3.38000- 2 1.18000- 2 2.20000- 2 0.00000+ 01163 2151  136
 6.31000+ 1 5.00000- 1 2.39300- 2 3.40000- 5 2.39000- 2 0.00000+ 01163 2151  137
 7.11000+ 1 5.00000- 1 4.23000- 2 1.90000- 2 2.33000- 2 0.00000+ 01163 2151  138
 8.60000+ 1 5.00000- 1 5.03000- 2 2.60000- 2 2.43000- 2 0.00000+ 01163 2151  139
 1.01700+ 2 5.00000- 1 2.47000- 2 8.00000- 4 2.39000- 2 0.00000+ 01163 2151  140
 1.20200+ 2 5.00000- 1 7.58000- 2 5.18000- 2 2.40000- 2 0.00000+ 01163 2151  141
 1.24200+ 2 5.00000- 1 3.69000- 2 1.59000- 2 2.10000- 2 0.00000+ 01163 2151  142
 1.33700+ 2 5.00000- 1 2.49800- 2 1.08000- 3 2.39000- 2 0.00000+ 01163 2151  143
 1.37000+ 2 5.00000- 1 2.43800- 2 4.80000- 4 2.39000- 2 0.00000+ 01163 2151  144
 1.63700+ 2 5.00000- 1 2.59900- 2 2.09000- 3 2.39000- 2 0.00000+ 01163 2151  145
 1.92600+ 2 5.00000- 1 3.71000- 2 1.32000- 2 2.39000- 2 0.00000+ 01163 2151  146
 1.94000+ 2 5.00000- 1 7.00000- 2 5.20000- 2 1.80000- 2 0.00000+ 01163 2151  147
 2.12000+ 2 5.00000- 1 1.23000- 1 9.82000- 2 2.48000- 2 0.00000+ 01163 2151  148
 2.29000+ 2 5.00000- 1 2.62400- 2 2.34000- 3 2.39000- 2 0.00000+ 01163 2151  149
 2.43000+ 2 5.00000- 1 2.42000- 2 3.00000- 4 2.39000- 2 0.00000+ 01163 2151  150
 2.72400+ 2 5.00000- 1 7.65000- 2 5.50000- 2 2.15000- 2 0.00000+ 01163 2151  151
 2.88200+ 2 5.00000- 1 3.74000- 2 1.35000- 2 2.39000- 2 0.00000+ 01163 2151  152
 3.02500+ 2 5.00000- 1 1.09300- 1 8.35000- 2 2.58000- 2 0.00000+ 01163 2151  153
 3.20000+ 2 5.00000- 1 2.97000- 2 5.80000- 3 2.39000- 2 0.00000+ 01163 2151  154
 3.34400+ 2 5.00000- 1 3.00300- 2 6.13000- 3 2.39000- 2 0.00000+ 01163 2151  155
 3.56000+ 2 5.00000- 1 2.45400- 2 6.40000- 4 2.39000- 2 0.00000+ 01163 2151  156
 3.67800+ 2 5.00000- 1 2.43000- 2 4.00000- 4 2.39000- 2 0.00000+ 01163 2151  157
 3.71000+ 2 5.00000- 1 3.77000- 2 1.38000- 2 2.39000- 2 0.00000+ 01163 2151  158
 3.79000+ 2 5.00000- 1 1.54800- 1 1.30000- 1 2.48000- 2 0.00000+ 01163 2151  159
 4.15000+ 2 5.00000- 1 4.17000- 2 1.78000- 2 2.39000- 2 0.00000+ 01163 2151  160
 4.15000+ 2 1.00000+ 3          2          1          0          01163 2151  161
 0.00000+ 0 9.35400- 1          0          0          2          01163 2151  162
 2.34017+ 2 0.00000+ 0          0          0          6          11163 2151  163
 1.54000+ 1 5.00000- 1 1.00000+ 0 2.07900- 3 2.39000- 2 0.00000+ 01163 2151  164
 2.34017+ 2 0.00000+ 0          1          0         12          21163 2151  165
 1.54000+ 1 5.00000- 1 1.00000+ 0 1.77100- 3 2.39000- 2 0.00000+ 01163 2151  166
 7.70000+ 0 1.50000+ 0 1.00000+ 0 8.85500- 4 2.39000- 2 0.00000+ 01163 2151  167
                                                                  1163 2  0  168
                                                                  1163 0  0  169
 9.22360+ 4 2.34017+ 2          0         99          0          01163 3  1  170
 0.00000+ 0 0.00000+ 0          0          0          1        1101163 3  1  171
        110          2                                            1163 3  1  172
 1.00000- 5 0.00000+ 0 1.00000+ 3 0.00000+ 0 1.00000+ 3 2.85910+ 11163 3  1  173
 1.20000+ 3 2.63500+ 1 1.40000+ 3 2.45500+ 1 1.60000+ 3 2.32700+ 11163 3  1  174
 1.80000+ 3 2.23000+ 1 2.00000+ 3 2.14900+ 1 2.50000+ 3 2.01100+ 11163 3  1  175
 3.00000+ 3 1.91300+ 1 3.50000+ 3 1.84300+ 1 4.00000+ 3 1.79200+ 11163 3  1  176
 4.50000+ 3 1.74900+ 1 5.00000+ 3 1.71200+ 1 6.00000+ 3 1.66800+ 11163 3  1  177
 7.00000+ 3 1.63100+ 1 8.00000+ 3 1.60000+ 1 9.00000+ 3 1.58000+ 11163 3  1  178
 1.00000+ 4 1.55600+ 1 1.20000+ 4 1.52500+ 1 1.40000+ 4 1.49400+ 11163 3  1  179
 1.50000+ 4 1.47850+ 1 1.60000+ 4 1.47030+ 1 1.80000+ 4 1.45390+ 11163 3  1  180
 2.00000+ 4 1.43750+ 1 2.20000+ 4 1.41810+ 1 2.40000+ 4 1.39870+ 11163 3  1  181
 2.50000+ 4 1.38900+ 1 2.60000+ 4 1.38580+ 1 2.80000+ 4 1.37940+ 11163 3  1  182
 3.00000+ 4 1.37300+ 1 3.50000+ 4 1.35400+ 1 4.00000+ 4 1.33500+ 11163 3  1  183
 4.50000+ 4 1.31720+ 1 4.60000+ 4 1.31360+ 1 5.00000+ 4 1.30190+ 11163 3  1  184
 5.50000+ 4 1.28690+ 1 6.00000+ 4 1.27200+ 1 6.50000+ 4 1.26660+ 11163 3  1  185
 7.00000+ 4 1.26130+ 1 7.50000+ 4 1.25600+ 1 8.00000+ 4 1.25080+ 11163 3  1  186
 8.50000+ 4 1.24300+ 1 9.00000+ 4 1.23520+ 1 9.50000+ 4 1.23210+ 11163 3  1  187
 1.00000+ 5 1.22900+ 1 1.20000+ 5 1.20080+ 1 1.40000+ 5 1.17270+ 11163 3  1  188
 1.50000+ 5 1.15860+ 1 1.60000+ 5 1.14990+ 1 1.80000+ 5 1.13240+ 11163 3  1  189
 2.00000+ 5 1.11490+ 1 2.20000+ 5 1.09950+ 1 2.40000+ 5 1.08410+ 11163 3  1  190
 2.50000+ 5 1.07640+ 1 2.60000+ 5 1.06750+ 1 2.80000+ 5 1.04980+ 11163 3  1  191
 3.00000+ 5 1.03210+ 1 3.50000+ 5 9.95250+ 0 4.00000+ 5 9.58400+ 01163 3  1  192
 4.50000+ 5 9.31650+ 0 5.00000+ 5 9.04900+ 0 5.50000+ 5 8.84600+ 01163 3  1  193
 6.00000+ 5 8.64300+ 0 6.50000+ 5 8.43100+ 0 7.00000+ 5 8.21900+ 01163 3  1  194
 7.50000+ 5 8.04650+ 0 8.00000+ 5 7.87400+ 0 8.50000+ 5 7.79650+ 01163 3  1  195
 9.00000+ 5 7.71900+ 0 9.50000+ 5 7.70950+ 0 1.00000+ 6 7.70000+ 01163 3  1  196
 1.07000+ 6 7.66000+ 0 1.20000+ 6 7.55000+ 0 1.40000+ 6 7.42000+ 01163 3  1  197
 1.60000+ 6 7.34800+ 0 1.80000+ 6 7.45900+ 0 2.00000+ 6 7.54900+ 01163 3  1  198
 2.20000+ 6 7.58800+ 0 2.40000+ 6 7.59900+ 0 2.60000+ 6 7.59600+ 01163 3  1  199
 2.80000+ 6 7.63000+ 0 3.00000+ 6 7.65800+ 0 3.50000+ 6 7.73500+ 01163 3  1  200
 4.00000+ 6 7.63700+ 0 4.50000+ 6 7.69300+ 0 5.00000+ 6 7.66700+ 01163 3  1  201
 5.50000+ 6 7.41800+ 0 6.00000+ 6 7.08700+ 0 6.50000+ 6 6.89000+ 01163 3  1  202
 6.96800+ 6 6.59280+ 0 7.00000+ 6 6.72250+ 0 7.50000+ 6 6.69900+ 01163 3  1  203
 8.00000+ 6 6.47900+ 0 8.50000+ 6 6.47880+ 0 9.00000+ 6 6.40590+ 01163 3  1  204
 9.50000+ 6 6.34120+ 0 1.00000+ 7 6.24030+ 0 1.05000+ 7 6.11860+ 01163 3  1  205
 1.10000+ 7 6.00500+ 0 1.15000+ 7 5.94950+ 0 1.17380+ 7 5.90360+ 01163 3  1  206
 1.20000+ 7 5.89300+ 0 1.25000+ 7 5.80750+ 0 1.30000+ 7 5.74500+ 01163 3  1  207
 1.35000+ 7 5.72160+ 0 1.40000+ 7 5.67230+ 0 1.45000+ 7 5.73890+ 01163 3  1  208
 1.50000+ 7 5.61360+ 0 2.00000+ 7 5.65851+ 0                      1163 3  1  209
                                                                  1163 3  0  210
 9.22360+ 4 2.34017+ 2          0         99          0          01163 3  2  211
 0.00000+ 0 0.00000+ 0          0          0          1         761163 3  2  212
         76          2                                            1163 3  2  213
 1.00000- 5 0.00000+ 0 1.00000+ 3 0.00000+ 0 1.00000+ 3 2.51950+ 11163 3  2  214
 1.20000+ 3 2.32000+ 1 1.40000+ 3 2.17500+ 1 1.60000+ 3 2.07000+ 11163 3  2  215
 1.80000+ 3 1.99000+ 1 2.00000+ 3 1.92500+ 1 2.50000+ 3 1.81500+ 11163 3  2  216
 3.00000+ 3 1.73500+ 1 3.50000+ 3 1.68000+ 1 4.00000+ 3 1.64000+ 11163 3  2  217
 4.50000+ 3 1.60500+ 1 5.00000+ 3 1.57500+ 1 6.00000+ 3 1.54000+ 11163 3  2  218
 7.00000+ 3 1.51000+ 1 8.00000+ 3 1.48500+ 1 9.00000+ 3 1.47000+ 11163 3  2  219
 1.00000+ 4 1.45000+ 1 1.50000+ 4 1.39000+ 1 2.00000+ 4 1.36000+ 11163 3  2  220
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 5.00000+ 4 1.25140+ 1 6.00000+ 4 1.21750+ 1 7.00000+ 4 1.20280+ 11163 3  2  222
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 1.50000+ 5 1.03500+ 1 2.00000+ 5 9.74700+ 0 2.50000+ 5 9.25400+ 01163 3  2  224
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 6.00000+ 5 6.60300+ 0 7.00000+ 5 6.06200+ 0 8.00000+ 5 5.52400+ 01163 3  2  226
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 1.40000+ 6 4.43000+ 0 1.60000+ 6 4.40000+ 0 1.80000+ 6 4.42000+ 01163 3  2  228
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 2.60000+ 6 4.45200+ 0 2.80000+ 6 4.52000+ 0 3.00000+ 6 4.57000+ 01163 3  2  230
 3.50000+ 6 4.66000+ 0 4.00000+ 6 4.61000+ 0 4.50000+ 6 4.59000+ 01163 3  2  231
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 8.00000+ 6 3.26000+ 0 8.50000+ 6 3.16000+ 0 9.00000+ 6 3.06000+ 01163 3  2  234
 9.50000+ 6 3.02000+ 0 1.00000+ 7 2.98000+ 0 1.05000+ 7 2.92000+ 01163 3  2  235
 1.10000+ 7 2.85000+ 0 1.15000+ 7 2.84000+ 0 1.20000+ 7 2.83000+ 01163 3  2  236
 1.25000+ 7 2.79000+ 0 1.30000+ 7 2.76000+ 0 1.35000+ 7 2.77000+ 01163 3  2  237
 1.40000+ 7 2.78000+ 0 1.45000+ 7 2.89000+ 0 1.50000+ 7 2.80000+ 01163 3  2  238
 2.00000+ 7 2.94490+ 0                                            1163 3  2  239
                                                                  1163 3  0  240
 9.22360+ 4 2.34017+ 2          0         99          0          01163 3  4  241
 0.00000+ 0-4.52800+ 4          0          0          1         541163 3  4  242
         54          2                                            1163 3  4  243
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 7.00000+ 4 1.70000- 1 8.00000+ 4 3.60000- 1 9.00000+ 4 4.90000- 11163 3  4  245
 1.00000+ 5 6.00000- 1 1.50000+ 5 9.20000- 1 2.00000+ 5 1.11000+ 01163 3  4  246
 2.50000+ 5 1.23000+ 0 3.00000+ 5 1.31000+ 0 4.00000+ 5 1.46000+ 01163 3  4  247
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 0.00000+ 0 3.50000+ 6          0          0         10          01163 4  2  714
 7.40000- 1 5.97000- 1 4.79000- 1 3.82000- 1 2.45000- 1 1.29000- 11163 4  2  715
 5.50000- 2 1.90000- 2 2.40000- 3 5.00000- 4                      1163 4  2  716
 0.00000+ 0 4.00000+ 6          0          0         10          01163 4  2  717
 7.50000- 1 6.20000- 1 5.02000- 1 4.13000- 1 2.90000- 1 1.63000- 11163 4  2  718
 9.00000- 2 4.00000- 2 5.70000- 3 1.50000- 3                      1163 4  2  719
 0.00000+ 0 4.50000+ 6          0          0         10          01163 4  2  720
 7.46030- 1 6.19500- 1 5.08500- 1 4.21500- 1 3.03800- 1 1.80700- 11163 4  2  721
 1.06400- 1 5.44000- 2 1.37000- 2 6.00000- 3                      1163 4  2  722
 0.00000+ 0 5.00000+ 6          0          0         11          01163 4  2  723
 7.42200- 1 6.19000- 1 5.15000- 1 4.29700- 1 3.17700- 1 1.98100- 11163 4  2  724
 1.22600- 1 6.86000- 2 2.17000- 2 1.06000- 2 3.00000- 4           1163 4  2  725
 0.00000+ 0 5.50000+ 6          0          0         12          01163 4  2  726
 7.38400- 1 6.18500- 1 5.21500- 1 4.38100- 1 3.31600- 1 2.15600- 11163 4  2  727
 1.38800- 1 8.29000- 2 2.98000- 2 1.52000- 2 2.10000- 3 1.00000- 31163 4  2  728
 0.00000+ 0 6.00000+ 6          0          0         12          01163 4  2  729
 7.34600- 1 6.18000- 1 5.28000- 1 4.46400- 1 3.45400- 1 2.33100- 11163 4  2  730
 1.55300- 1 9.73000- 2 3.78000- 2 1.98000- 2 4.20000- 3 2.10000- 31163 4  2  731
 0.00000+ 0 6.50000+ 6          0          0         13          01163 4  2  732
 7.30800- 1 6.17500- 1 5.34500- 1 4.54800- 1 3.59200- 1 2.50600- 11163 4  2  733
 1.71600- 1 1.11500- 1 4.58000- 2 2.44000- 2 6.30000- 3 3.10000- 31163 4  2  734
 1.00000- 4                                                       1163 4  2  735
 0.00000+ 0 7.00000+ 6          0          0         13          01163 4  2  736
 7.27000- 1 6.17000- 1 5.41000- 1 4.63000- 1 3.73000- 1 2.68000- 11163 4  2  737
 1.88000- 1 1.26000- 1 5.39000- 2 2.89000- 2 8.50000- 3 4.20000- 31163 4  2  738
 2.00000- 4                                                       1163 4  2  739
 0.00000+ 0 7.50000+ 6          0          0         14          01163 4  2  740
 7.15000- 1 6.02000- 1 5.34000- 1 4.58000- 1 3.67000- 1 2.68000- 11163 4  2  741
 1.86000- 1 1.28000- 1 6.38000- 2 3.82000- 2 1.29000- 2 6.00000- 31163 4  2  742
 5.00000- 4 0.00000+ 0                                            1163 4  2  743
 0.00000+ 0 8.00000+ 6          0          0         14          01163 4  2  744
 7.00000- 1 5.89000- 1 5.22000- 1 4.48000- 1 3.57000- 1 2.65000- 11163 4  2  745
 1.81000- 1 1.28000- 1 7.30000- 2 4.80000- 2 1.88000- 2 7.80000- 31163 4  2  746
 1.40000- 3 2.00000- 4                                            1163 4  2  747
 0.00000+ 0 9.00000+ 6          0          0         14          01163 4  2  748
 6.71000- 1 5.56000- 1 4.84000- 1 4.19000- 1 3.36000- 1 2.54000- 11163 4  2  749
 1.73000- 1 1.27000- 1 9.30000- 2 7.00000- 2 3.40000- 2 1.33000- 21163 4  2  750
 3.30000- 3 1.40000- 3                                            1163 4  2  751
 0.00000+ 0 1.00000+ 7          0          0         14          01163 4  2  752
 6.43000- 1 5.16000- 1 4.34000- 1 3.87000- 1 3.15000- 1 2.46000- 11163 4  2  753
 1.75000- 1 1.30000- 1 1.13500- 1 9.52000- 2 5.44000- 2 2.25000- 21163 4  2  754
 6.80000- 3 3.20000- 3                                            1163 4  2  755
 0.00000+ 0 1.10000+ 7          0          0         15          01163 4  2  756
 6.20000- 1 4.75000- 1 3.90000- 1 3.54000- 1 2.92000- 1 2.42000- 11163 4  2  757
 1.87000- 1 1.45000- 1 1.34800- 1 1.22400- 1 7.93000- 2 3.55000- 21163 4  2  758
 1.32000- 2 5.40000- 3 0.00000+ 0                                 1163 4  2  759
 0.00000+ 0 1.20000+ 7          0          0         15          01163 4  2  760
 6.05000- 1 4.40000- 1 3.56000- 1 3.18000- 1 2.75000- 1 2.37000- 11163 4  2  761
 1.97000- 1 1.64000- 1 1.54800- 1 1.45300- 1 1.05100- 1 5.18000- 21163 4  2  762
 2.17000- 2 7.70000- 3 1.10000- 3                                 1163 4  2  763
 0.00000+ 0 1.30000+ 7          0          0         15          01163 4  2  764
 6.06000- 1 4.37000- 1 3.36000- 1 3.00000- 1 2.61000- 1 2.32000- 11163 4  2  765
 2.04000- 1 1.82000- 1 1.72000- 1 1.61700- 1 1.26700- 1 7.04000- 21163 4  2  766
 3.28000- 2 1.10000- 2 3.00000- 3                                 1163 4  2  767
 0.00000+ 0 1.40000+ 7          0          0         15          01163 4  2  768
 6.23000- 1 4.53000- 1 3.43000- 1 3.02000- 1 2.65000- 1 2.35000- 11163 4  2  769
 2.16000- 1 1.96000- 1 1.85000- 1 1.74900- 1 1.45000- 1 8.81000- 21163 4  2  770
 4.50000- 2 1.60000- 2 4.80000- 3                                 1163 4  2  771
 0.00000+ 0 1.50000+ 7          0          0         15          01163 4  2  772
 6.42000- 1 4.81000- 1 3.62000- 1 3.20000- 1 2.88000- 1 2.54000- 11163 4  2  773
 2.29000- 1 2.11000- 1 1.96000- 1 1.84000- 1 1.57000- 1 1.04000- 11163 4  2  774
 5.60000- 2 2.20000- 2 7.00000- 3                                 1163 4  2  775
 0.00000+ 0 2.00000+ 7          0          0         15          01163 4  2  776
 6.42000- 1 4.81000- 1 3.62000- 1 3.20000- 1 2.88000- 1 2.54000- 11163 4  2  777
 2.29000- 1 2.11000- 1 1.96000- 1 1.84000- 1 1.57000- 1 1.04000- 11163 4  2  778
 5.60000- 2 2.20000- 2 7.00000- 3                                 1163 4  2  779
                                                                  1163 4  0  780
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 16  781
 0.00000+ 0 2.34017+ 2          0          1          0          01163 4 16  782
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 16  783
          2          2                                            1163 4 16  784
 0.00000+ 0 6.96800+ 6          0          0          1          21163 4 16  785
          2          2                                            1163 4 16  786
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 16  787
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 16  788
          2          2                                            1163 4 16  789
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 16  790
                                                                  1163 4  0  791
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 17  792
 0.00000+ 0 2.34017+ 2          0          1          0          01163 4 17  793
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 17  794
          2          2                                            1163 4 17  795
 0.00000+ 0 1.17380+ 7          0          0          1          21163 4 17  796
          2          2                                            1163 4 17  797
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 17  798
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 17  799
          2          2                                            1163 4 17  800
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 17  801
                                                                  1163 4  0  802
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 18  803
 0.00000+ 0 2.34017+ 2          0          1          0          01163 4 18  804
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 18  805
          2          2                                            1163 4 18  806
 0.00000+ 0 1.00000- 5          0          0          1          21163 4 18  807
          2          2                                            1163 4 18  808
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 18  809
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 18  810
          2          2                                            1163 4 18  811
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 18  812
                                                                  1163 4  0  813
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 51  814
 0.00000+ 0 2.34017+ 2          0          2          0          01163 4 51  815
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 51  816
          2          2                                            1163 4 51  817
 0.00000+ 0 4.60000+ 4          0          0          1          21163 4 51  818
          2          2                                            1163 4 51  819
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 51  820
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 51  821
          2          2                                            1163 4 51  822
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 51  823
                                                                  1163 4  0  824
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 52  825
 0.00000+ 0 2.34017+ 2          0          2          0          01163 4 52  826
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 52  827
          2          2                                            1163 4 52  828
 0.00000+ 0 1.50000+ 5          0          0          1          21163 4 52  829
          2          2                                            1163 4 52  830
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 52  831
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 52  832
          2          2                                            1163 4 52  833
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 52  834
                                                                  1163 4  0  835
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 53  836
 0.00000+ 0 2.34017+ 2          0          2          0          01163 4 53  837
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 53  838
          2          2                                            1163 4 53  839
 0.00000+ 0 3.00000+ 5          0          0          1          21163 4 53  840
          2          2                                            1163 4 53  841
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 53  842
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 53  843
          2          2                                            1163 4 53  844
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 53  845
                                                                  1163 4  0  846
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 54  847
 0.00000+ 0 2.34017+ 2          0          2          0          01163 4 54  848
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 54  849
          2          2                                            1163 4 54  850
 0.00000+ 0 7.00000+ 5          0          0          1          21163 4 54  851
          2          2                                            1163 4 54  852
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 54  853
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 54  854
          2          2                                            1163 4 54  855
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 54  856
                                                                  1163 4  0  857
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 55  858
 0.00000+ 0 2.34017+ 2          0          2          0          01163 4 55  859
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 55  860
          2          2                                            1163 4 55  861
 0.00000+ 0 1.00000+ 6          0          0          1          21163 4 55  862
          2          2                                            1163 4 55  863
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 55  864
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 55  865
          2          2                                            1163 4 55  866
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 55  867
                                                                  1163 4  0  868
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 56  869
 0.00000+ 0 2.34017+ 2          0          2          0          01163 4 56  870
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 56  871
          2          2                                            1163 4 56  872
 0.00000+ 0 1.07000+ 6          0          0          1          21163 4 56  873
          2          2                                            1163 4 56  874
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 56  875
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 56  876
          2          2                                            1163 4 56  877
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 56  878
                                                                  1163 4  0  879
 9.22360+ 4 2.34017+ 2          0          2          0          01163 4 91  880
 0.00000+ 0 2.34017+ 2          0          2          0          01163 4 91  881
 0.00000+ 0 0.00000+ 0          0          0          1          21163 4 91  882
          2          2                                            1163 4 91  883
 0.00000+ 0 9.00000+ 5          0          0          1          21163 4 91  884
          2          2                                            1163 4 91  885
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 91  886
 0.00000+ 0 2.00000+ 7          0          0          1          21163 4 91  887
          2          2                                            1163 4 91  888
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1163 4 91  889
                                                                  1163 4  0  890
                                                                  1163 0  0  891
 9.22360+ 4 2.34017+ 2          0          0          1          01163 5 16  892
 6.96800+ 6 0.00000+ 0          0          9          1          21163 5 16  893
          2          5                                            1163 5 16  894
 6.96800+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1163 5 16  895
 0.00000+ 0 0.00000+ 0          0          0          1          31163 5 16  896
          3          5                                            1163 5 16  897
 5.00000+ 5 1.43900+ 5 1.50000+ 7 7.90600+ 5 2.00000+ 7 9.13144+ 51163 5 16  898
                                                                  1163 5  0  899
 9.22360+ 4 2.34017+ 2          0          0          1          01163 5 17  900
 1.17380+ 7 0.00000+ 0          0          9          1          21163 5 17  901
          2          5                                            1163 5 17  902
 1.17380+ 7 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1163 5 17  903
 0.00000+ 0 0.00000+ 0          0          0          1          31163 5 17  904
          3          5                                            1163 5 17  905
 5.00000+ 5 1.38600+ 5 1.50000+ 7 7.59000+ 5 2.00000+ 7 8.76404+ 51163 5 17  906
                                                                  1163 5  0  907
 9.22360+ 4 2.34017+ 2          0          0          1          01163 5 18  908
-2.00000+ 7 0.00000+ 0          0          7          1          21163 5 18  909
          2          2                                            1163 5 18  910
 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1163 5 18  911
 0.00000+ 0 0.00000+ 0          0          0          1          31163 5 18  912
          3          5                                            1163 5 18  913
 1.00000- 5 1.29550+ 6 1.50000+ 7 1.49230+ 6 2.00000+ 7 1.49447+ 61163 5 18  914
                                                                  1163 5  0  915
 9.22360+ 4 2.34017+ 2          0          0          1          01163 5 91  916
 4.50000+ 4 0.00000+ 0          0          9          1          21163 5 91  917
          2          2                                            1163 5 91  918
 9.00000+ 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1163 5 91  919
 0.00000+ 0 0.00000+ 0          0          0          1          31163 5 91  920
          3          2                                            1163 5 91  921
 9.00000+ 5 1.50700+ 5 1.50000+ 7 8.25700+ 5 2.00000+ 7 1.06506+ 61163 5 91  922
                                                                  1163 5  0  923
                                                                  1163 0  0  924
                                                                     0 0  0  925
 1.00100+ 3 9.99170- 1          0          0          6         121269 1451    1
 0.00000+ 0 0.00000+ 0          0          0        116          01269 1451    2
  1- h-  1  lasl      eval-aug70 l.stewart,r.j.labauve,p.g.young  1269 1451    3
 la-4574   (1971)     dist-may74                                  1269 1451    4
                                                                  1269 1451    5
 *****************   dna 4148 mod 2   *************************** 1269 1451    6
                                                                  1269 1451    7
     august  1973         comments and changes                    1269 1451    8
                                                                  1269 1451    9
           1.  recent total measurements by clement and stoler    1269 1451   10
               (rpi) and by heaton et al. (nbs) do not indicate   1269 1451   11
               the need for changes at this time.                 1269 1451   12
           2.  the lp=2 flag has been implemented in mf=12,       1269 1451   13
               mt=102 in version iv.                              1269 1451   14
                                                                  1269 1451   15
           3.  a new listing has been generated for the total     1269 1451   16
               cross section to insure that the summation of the  1269 1451   17
               partials is conserved to higher precision.         1269 1451   18
                                                                  1269 1451   19
           4.  the normalization and standards subcommittee of    1269 1451   20
               csewg reviewed this file in march, 1973 and        1269 1451   21
               recommended no changes to the scattering cross     1269 1451   22
               section for version iv.                            1269 1451   23
                                                                  1269 1451   24
                                                                  1269 1451   25
 *****************   dna 4148 mod 1   *************************** 1269 1451   26
                                                                  1269 1451   27
           this modification was made to enable the current       1269 1451   28
           dna library to conform to the endf/b-iii library       1269 1451   29
           and to add photon interaction data                     1269 1451   30
                                                                  1269 1451   31
           the data corresponds to the endf/b-iii evaluation      1269 1451   32
           with the mat number having the same last 3 digits.     1269 1451   33
                                                                  1269 1451   34
 ***************************************************************  1269 1451   35
                                                                  1269 1451   36
 *         *          *          *         *          *          *1269 1451   37
 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *1269 1451   38
 *                                                               *1269 1451   39
 * cross section standard    hydrogen scattering cross section   *1269 1451   40
 *                                                               *1269 1451   41
 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *1269 1451   42
 *                                                               *1269 1451   43
 * the scattering cross section has been recommended as a        *1269 1451   44
 *                                                               *1269 1451   45
 * standard by the csewg normalization and standards subcommittee*1269 1451   46
 *                                                               *1269 1451   47
 * for the energy range from 1 kev to 20 mev                     *1269 1451   48
 *                                                               *1269 1451   49
 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *1269 1451   50
                                                                  1269 1451   51
   hydrogen free atom cross sections as given in la-4574          1269 1451   52
      entry by l. stewart, r.j. labauve, and p.g. young           1269 1451   53
      los alamos scientific laboratory                            1269 1451   54
      los alamos,new mexico 87544                                 1269 1451   55
      october 20,1970                                             1269 1451   56
                                                                  1269 1451   57
  mf=1                                                            1269 1451   58
                                                                  1269 1451   59
    mt=451, atomic mass=1.007825                                  1269 1451   60
                                                                  1269 1451   61
  mf=2                                                            1269 1451   62
                                                                  1269 1451   63
  mt=151, scattering length=1.27565e-12 cm.                       1269 1451   64
                                                                  1269 1451   65
  mf=3                                                            1269 1451   66
                                                                  1269 1451   67
    mt=  1, total cross sections --- the total cross sections are 1269 1451   68
            obtained by adding the elastic scattering and         1269 1451   69
            radiative capture cross sections at all energies.     1269 1451   70
             1.0e-05 ev to 20 mev.                                1269 1451   71
                                                                  1269 1451   72
    mt=  2, elastic scattering --- from an extensive theoretical  1269 1451   73
            treatment of fast neutron measurements                1269 1451   74
            by j. c. hopkins(lasl) and g. breit(state             1269 1451   75
            university of new york). see n.d. a9, 145(1971).      1269 1451   76
             1.0e-05 ev to 20 mev.                                1269 1451   77
                                                                  1269 1451   78
    mt=102, radiative capture --- these cross sections are taken  1269 1451   79
            from the publication of a. horley where a value       1269 1451   80
            of 332 mb was adopted for the thermal value.  see     1269 1451   81
            n.d. a2, 243(1966) also p.c.                          1269 1451   82
             1.0e-05 ev to 20 mev.                                1269 1451   83
                                                                  1269 1451   84
    mt=251, average value of cosine of scattering angle           1269 1451   85
            in lab system (provided by bnl).                      1269 1451   86
             1.0e-05 ev t0 20 mev.                                1269 1451   87
                                                                  1269 1451   88
    mt=252, average logarithmic energy change per collison, taken 1269 1451   89
            as 1, from 1.0e-05 ev to 20 mev. (provided by bnl).   1269 1451   90
                                                                  1269 1451   91
    mt=253, gamma, taken as 1, from 1.0e-05 ev to 20 mev.         1269 1451   92
            (provided by bnl).                                    1269 1451   93
                                                                  1269 1451   94
  mf=4                                                            1269 1451   95
                                                                  1269 1451   96
    mt=  2, neutron elastic scattering angular distributions in   1269 1451   97
            the center of mass system--given as normalized        1269 1451   98
            pointwise probabilities.                              1269 1451   99
                                                                  1269 1451  100
                                                                  1269 1451  101
  mf=7                                                            1269 1451  102
                                                                  1269 1451  103
    mt=  4, .00001 to 5 ev free gas sigma=20.449 barns.           1269 1451  104
                                                                  1269 1451  105
  mf=12                                                           1269 1451  106
                                                                  1269 1451  107
    mt=102, gamma ray multiplicities --- multiplicity, (referred  1269 1451  108
            to mt=102, mf=3), is unity at all neutron energies.   1269 1451  109
            lp=2 now implemented,  therefore all gamma energies   1269 1451  110
            must be calculated.                                   1269 1451  111
                                                                  1269 1451  112
  mf=14                                                           1269 1451  113
                                                                  1269 1451  114
    mt=102, gamma ray angular distribution --- assumed isotropic  1269 1451  115
            at all neutron energies.                              1269 1451  116
                                                                  1269 1451  117
                                                                  1269 1451  118
                                1        451        130           1269 1451  119
                                2        151          4           1269 1451  120
                                3          1         48           1269 1451  121
                                3          2         48           1269 1451  122
                                3        102         48           1269 1451  123
                                3        251          8           1269 1451  124
                                3        252          4           1269 1451  125
                                3        253          4           1269 1451  126
                                4          2         88           1269 1451  127
                                7          4          4           1269 1451  128
                               12        102          4           1269 1451  129
                               14        102          1           1269 1451  130
                                                                  1269 1  0  131
                                                                  1269 0  0  132
 1.00100+ 3 9.99170- 1          0          0          1          01269 2151  133
 1.00100+ 3 1.00000+ 0          0          0          1          01269 2151  134
 1.00000- 5 1.00000+ 5          0          0          0          01269 2151  135
 5.00000- 1 1.27565+ 0          0          0          0          01269 2151  136
                                                                  1269 2  0  137
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-4.00000- 1 5.04340- 1-2.00000- 1 5.02070- 1 0.00000+ 0 4.99870- 11269 4  2  355
 2.00000- 1 4.97660- 1 4.00000- 1 4.95460- 1 6.00000- 1 4.93140- 11269 4  2  356
 8.00000- 1 4.90770- 1 1.00000+ 0 4.88180- 1                      1269 4  2  357
 0.00000+ 0 1.00000+ 7          0          0          1         111269 4  2  358
         11          2                                            1269 4  2  359
-1.00000+ 0 5.17270- 1-8.00000- 1 5.12010- 1-6.00000- 1 5.07940- 11269 4  2  360
-4.00000- 1 5.04610- 1-2.00000- 1 5.01680- 1 0.00000+ 0 4.99080- 11269 4  2  361
 2.00000- 1 4.96690- 1 4.00000- 1 4.94350- 1 6.00000- 1 4.92020- 11269 4  2  362
 8.00000- 1 4.89690- 1 1.00000+ 0 4.87160- 1                      1269 4  2  363
 0.00000+ 0 1.20000+ 7          0          0          1         121269 4  2  364
         12          2                                            1269 4  2  365
-1.00000+ 0 5.22720- 1-9.00000- 1 5.18250- 1-8.00000- 1 5.14640- 11269 4  2  366
-6.00000- 1 5.08980- 1-4.00000- 1 5.04750- 1-2.00000- 1 5.01290- 11269 4  2  367
 0.00000+ 0 4.98230- 1 2.00000- 1 4.95560- 1 4.00000- 1 4.93130- 11269 4  2  368
 6.00000- 1 4.90850- 1 8.00000- 1 4.88660- 1 1.00000+ 0 4.86540- 11269 4  2  369
 0.00000+ 0 1.40000+ 7          0          0          1         121269 4  2  370
         12          2                                            1269 4  2  371
-1.00000+ 0 5.28230- 1-9.00000- 1 5.21880- 1-8.00000- 1 5.16980- 11269 4  2  372
-6.00000- 1 5.09820- 1-4.00000- 1 5.04560- 1-2.00000- 1 5.00480- 11269 4  2  373
 0.00000+ 0 4.97030- 1 2.00000- 1 4.94310- 1 4.00000- 1 4.91950- 11269 4  2  374
 6.00000- 1 4.90050- 1 8.00000- 1 4.88330- 1 1.00000+ 0 4.86880- 11269 4  2  375
 0.00000+ 0 1.60000+ 7          0          0          1         121269 4  2  376
         12          2                                            1269 4  2  377
-1.00000+ 0 5.34330- 1-9.00000- 1 5.25750- 1-8.00000- 1 5.19240- 11269 4  2  378
-6.00000- 1 5.10240- 1-4.00000- 1 5.04040- 1-2.00000- 1 4.99390- 11269 4  2  379
 0.00000+ 0 4.95670- 1 2.00000- 1 4.92880- 1 4.00000- 1 4.90810- 11269 4  2  380
 6.00000- 1 4.89360- 1 8.00000- 1 4.88530- 1 1.00000+ 0 4.88330- 11269 4  2  381
 0.00000+ 0 1.80000+ 7          0          0          1         121269 4  2  382
         12          2                                            1269 4  2  383
-1.00000+ 0 5.40920- 1-9.00000- 1 5.29620- 1-8.00000- 1 5.21340- 11269 4  2  384
-6.00000- 1 5.10380- 1-4.00000- 1 5.03270- 1-2.00000- 1 4.98020- 11269 4  2  385
 0.00000+ 0 4.94060- 1 2.00000- 1 4.91260- 1 4.00000- 1 4.89630- 11269 4  2  386
 6.00000- 1 4.89050- 1 8.00000- 1 4.89400- 1 1.00000+ 0 4.90910- 11269 4  2  387
 0.00000+ 0 2.00000+ 7          0          0          1         121269 4  2  388
         12          2                                            1269 4  2  389
-1.00000+ 0 5.48070- 1-9.00000- 1 5.33480- 1-8.00000- 1 5.23320- 11269 4  2  390
-6.00000- 1 5.10290- 1-4.00000- 1 5.02210- 1-2.00000- 1 4.96350- 11269 4  2  391
 0.00000+ 0 4.92180- 1 2.00000- 1 4.89580- 1 4.00000- 1 4.88400- 11269 4  2  392
 6.00000- 1 4.88660- 1 8.00000- 1 4.90750- 1 1.00000+ 0 4.94660- 11269 4  2  393
                                                                  1269 4  0  394
                                                                  1269 0  0  395
 1.00100+ 3 9.99170- 1          0          0          0          01269 7  4  396
 0.00000+ 0 0.00000+ 0          0          0         12          11269 7  4  397
 0.00000+ 0 2.00000+ 2 9.99170- 1 5.00000+ 0 0.00000+ 0 0.00000+ 01269 7  4  398
 1.00000+ 0 2.04490+ 1 9.99170- 1 0.00000+ 0 0.00000+ 0 0.00000+ 01269 7  4  399
                                                                  1269 7  0  400
                                                                  1269 0  0  401
 1.00100+ 3 9.99170- 1          1          0          1          0126912102  402
 2.22460+ 6 0.00000+ 0          2          2          1          2126912102  403
          2          2                                            126912102  404
 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      126912102  405
                                                                  126912  0  406
                                                                  1269 0  0  407
 1.00100+ 3 9.99170- 1          1          0          1          0126914102  408
                                                                  126914  0  409
                                                                  1269 0  0  410
                                                                     0 0  0  411
 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
                                                                  1271 1  0  223
                                                                  1271 0  0  224
 3.00600+ 3 5.96340+ 0          0          0          1          01271 2151  225
 3.00600+ 3 1.00000+ 0          0          0          1          01271 2151  226
 1.00000- 5 1.00000+ 5          0          0          0          01271 2151  227
 1.00000+ 0 2.39740- 1          0          0          0          01271 2151  228
                                                                  1271 2  0  229
                                                                  1271 0  0  230
 3.00600+ 3 5.96340+ 0          0         99          0          01271 3  1  231
 0.00000+ 0 0.00000+ 0          0          0          2        1771271 3  1  232
         24          5        177          2                      1271 3  1  233
 1.00000- 5 4.72860+ 4 1.00000- 2 1.49590+ 3 2.53000- 2 9.40760+ 21271 3  1  234
 1.00000- 1 4.73560+ 2 1.00000+ 0 1.50230+ 2 1.00000+ 1 4.79880+ 11271 3  1  235
 1.00000+ 2 1.56560+ 1 4.00000+ 2 8.18240+ 0 1.00000+ 3 5.43680+ 01271 3  1  236
 2.00000+ 3 4.05440+ 0 4.00000+ 3 3.07900+ 0 6.50000+ 3 2.57340+ 01271 3  1  237
 1.00000+ 4 2.21890+ 0 1.50000+ 4 1.95120+ 0 2.00000+ 4 1.79460+ 01271 3  1  238
 2.50000+ 4 1.69030+ 0 3.00000+ 4 1.61580+ 0 3.50000+ 4 1.56040+ 01271 3  1  239
 4.00000+ 4 1.51840+ 0 4.50000+ 4 1.48620+ 0 5.00000+ 4 1.46190+ 01271 3  1  240
 6.00000+ 4 1.43140+ 0 7.00000+ 4 1.42090+ 0 8.00000+ 4 1.42810+ 01271 3  1  241
 9.00000+ 4 1.45300+ 0 1.00000+ 5 1.49760+ 0 1.10000+ 5 1.56540+ 01271 3  1  242
 1.20000+ 5 1.66210+ 0 1.30000+ 5 1.79580+ 0 1.40000+ 5 1.97870+ 01271 3  1  243
 1.50000+ 5 2.22770+ 0 1.60000+ 5 2.56690+ 0 1.70000+ 5 3.02990+ 01271 3  1  244
 1.80000+ 5 3.66150+ 0 1.90000+ 5 4.51600+ 0 2.00000+ 5 5.64280+ 01271 3  1  245
 2.05000+ 5 6.31320+ 0 2.10000+ 5 7.04550+ 0 2.15000+ 5 7.81940+ 01271 3  1  246
 2.16000+ 5 7.97650+ 0 2.17000+ 5 8.13360+ 0 2.18000+ 5 8.29040+ 01271 3  1  247
 2.19000+ 5 8.44650+ 0 2.20000+ 5 8.60140+ 0 2.21000+ 5 8.75480+ 01271 3  1  248
 2.22000+ 5 8.90620+ 0 2.23000+ 5 9.05510+ 0 2.24000+ 5 9.20120+ 01271 3  1  249
 2.25000+ 5 9.34380+ 0 2.26000+ 5 9.48270+ 0 2.27000+ 5 9.61720+ 01271 3  1  250
 2.28000+ 5 9.74690+ 0 2.29000+ 5 9.87130+ 0 2.30000+ 5 9.99000+ 01271 3  1  251
 2.31000+ 5 1.01030+ 1 2.32000+ 5 1.02090+ 1 2.33000+ 5 1.03080+ 11271 3  1  252
 2.34000+ 5 1.03990+ 1 2.35000+ 5 1.04830+ 1 2.36000+ 5 1.05600+ 11271 3  1  253
 2.37000+ 5 1.06280+ 1 2.38000+ 5 1.06870+ 1 2.39000+ 5 1.07380+ 11271 3  1  254
 2.40000+ 5 1.07800+ 1 2.41000+ 5 1.08140+ 1 2.42000+ 5 1.08390+ 11271 3  1  255
 2.43000+ 5 1.08550+ 1 2.44000+ 5 1.08630+ 1 2.45000+ 5 1.08610+ 11271 3  1  256
 2.46000+ 5 1.08520+ 1 2.47000+ 5 1.08340+ 1 2.48000+ 5 1.08090+ 11271 3  1  257
 2.49000+ 5 1.07760+ 1 2.50000+ 5 1.07350+ 1 2.51000+ 5 1.06870+ 11271 3  1  258
 2.52000+ 5 1.06330+ 1 2.53000+ 5 1.05720+ 1 2.54000+ 5 1.05050+ 11271 3  1  259
 2.55000+ 5 1.04330+ 1 2.56000+ 5 1.03550+ 1 2.57000+ 5 1.02720+ 11271 3  1  260
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 1.10000- 1 8.20970- 2                                            1271 4  2  696
 0.00000+ 0 3.60000+ 5          0          0          2          01271 4  2  697
 1.17970- 1 7.72770- 2                                            1271 4  2  698
 0.00000+ 0 3.80000+ 5          0          0          2          01271 4  2  699
 1.23600- 1 7.28200- 2                                            1271 4  2  700
 0.00000+ 0 4.00000+ 5          0          0          2          01271 4  2  701
 1.27520- 1 6.87390- 2                                            1271 4  2  702
 0.00000+ 0 4.50000+ 5          0          0          2          01271 4  2  703
 1.32520- 1 6.00350- 2                                            1271 4  2  704
 0.00000+ 0 5.00000+ 5          0          0          2          01271 4  2  705
 1.33740- 1 5.30640- 2                                            1271 4  2  706
 0.00000+ 0 5.50000+ 5          0          0          2          01271 4  2  707
 1.33230- 1 4.73590- 2                                            1271 4  2  708
 0.00000+ 0 6.00000+ 5          0          0          2          01271 4  2  709
 1.31970- 1 4.25710- 2                                            1271 4  2  710
 0.00000+ 0 6.50000+ 5          0          0          2          01271 4  2  711
 1.30430- 1 3.84560- 2                                            1271 4  2  712
 0.00000+ 0 7.00000+ 5          0          0          2          01271 4  2  713
 1.28870- 1 3.48430- 2                                            1271 4  2  714
 0.00000+ 0 8.00000+ 5          0          0          2          01271 4  2  715
 1.26030- 1 2.86680- 2                                            1271 4  2  716
 0.00000+ 0 9.00000+ 5          0          0          2          01271 4  2  717
 1.23710- 1 2.34280- 2                                            1271 4  2  718
 0.00000+ 0 1.00000+ 6          0          0          2          01271 4  2  719
 1.21780- 1 1.87910- 2                                            1271 4  2  720
 0.00000+ 0 1.10000+ 6          0          0          2          01271 4  2  721
 1.19900- 1 1.45860- 2                                            1271 4  2  722
 0.00000+ 0 1.20000+ 6          0          0          2          01271 4  2  723
 1.17720- 1 1.07630- 2                                            1271 4  2  724
 0.00000+ 0 1.30000+ 6          0          0          2          01271 4  2  725
 1.14860- 1 7.38250- 3                                            1271 4  2  726
 0.00000+ 0 1.40000+ 6          0          0          2          01271 4  2  727
 1.11040- 1 4.63180- 3                                            1271 4  2  728
 0.00000+ 0 1.50000+ 6          0          0          2          01271 4  2  729
 1.06090- 1 2.85480- 3                                            1271 4  2  730
 0.00000+ 0 1.60000+ 6          0          0          2          01271 4  2  731
 1.00140- 1 2.57110- 3                                            1271 4  2  732
 0.00000+ 0 1.70000+ 6          0          0          2          01271 4  2  733
 9.37080- 2 4.46000- 3                                            1271 4  2  734
 0.00000+ 0 1.80000+ 6          0          0          2          01271 4  2  735
 8.78430- 2 9.25780- 3                                            1271 4  2  736
 0.00000+ 0 2.25000+ 6          0          0          4          01271 4  2  737
 8.20000- 2 6.10000- 2-6.70000- 3 7.00000- 4                      1271 4  2  738
 0.00000+ 0 2.50000+ 6          0          0          4          01271 4  2  739
 1.03000- 1 1.00000- 1-3.10000- 2 4.00000- 3                      1271 4  2  740
 0.00000+ 0 3.50000+ 6          0          0          4          01271 4  2  741
 2.35000- 1 2.25000- 1 2.30000- 2 1.80000- 2                      1271 4  2  742
 0.00000+ 0 4.00000+ 6          0          0          4          01271 4  2  743
 3.00000- 1 2.45000- 1 5.00000- 2 2.50000- 2                      1271 4  2  744
 0.00000+ 0 4.83000+ 6          0          0          4          01271 4  2  745
 4.10000- 1 2.84000- 1 9.80000- 2 3.71000- 2                      1271 4  2  746
 0.00000+ 0 5.74000+ 6          0          0          4          01271 4  2  747
 5.00000- 1 3.35000- 1 1.37000- 1 5.44000- 2                      1271 4  2  748
 0.00000+ 0 7.50000+ 6          0          0          4          01271 4  2  749
 5.79000- 1 4.03000- 1 1.77000- 1 7.59000- 2                      1271 4  2  750
 0.00000+ 0 1.00000+ 7          0          0          8          01271 4  2  751
 6.83450- 1 4.50910- 1 2.17930- 1 8.19040- 2 1.98710- 2 4.15910- 31271 4  2  752
 7.65410- 4 1.21920- 4                                            1271 4  2  753
 0.00000+ 0 1.20000+ 7          0          0          8          01271 4  2  754
 7.24770- 1 4.84190- 1 2.61780- 1 1.07790- 1 3.11530- 2 7.69160- 31271 4  2  755
 1.68310- 3 3.27970- 4                                            1271 4  2  756
 0.00000+ 0 1.30000+ 7          0          0          8          01271 4  2  757
 7.41520- 1 4.99510- 1 2.80410- 1 1.20650- 1 3.76180- 2 9.96810- 31271 4  2  758
 2.34540- 3 4.93190- 4                                            1271 4  2  759
 0.00000+ 0 1.40000+ 7          0          0          8          01271 4  2  760
 7.56350- 1 5.14260- 1 2.97560- 1 1.33490- 1 4.45560- 2 1.25790- 21271 4  2  761
 3.16930- 3 7.15950- 4                                            1271 4  2  762
 0.00000+ 0 1.50000+ 7          0          0          8          01271 4  2  763
 7.69550- 1 5.28540- 1 3.13620- 1 1.46330- 1 5.19500- 2 1.55360- 21271 4  2  764
 4.14260- 3 9.71650- 4                                            1271 4  2  765
 0.00000+ 0 1.60000+ 7          0          0          8          01271 4  2  766
 7.81500- 1 5.42440- 1 3.28900- 1 1.59200- 1 5.98020- 2 1.88650- 21271 4  2  767
 5.30610- 3 1.30920- 3                                            1271 4  2  768
 0.00000+ 0 1.80000+ 7          0          0          8          01271 4  2  769
 8.02320- 1 5.69000- 1 3.57600- 1 1.84660- 1 7.63610- 2 2.64340- 21271 4  2  770
 8.21120- 3 2.23130- 3                                            1271 4  2  771
 0.00000+ 0 2.00000+ 7          0          0          8          01271 4  2  772
 8.19970- 1 5.93900- 1 3.84520- 1 2.09630- 1 9.38570- 2 3.51850- 21271 4  2  773
 1.19000- 2 3.49200- 3                                            1271 4  2  774
                                                                  1271 4  0  775
 3.00600+ 3 5.96340+ 0          0          2          0          01271 4 24  776
 0.00000+ 0 0.00000+ 0          0          1          0          01271 4 24  777
 0.00000+ 0 0.00000+ 0          0          0          1          21271 4 24  778
          2          2                                            1271 4 24  779
 0.00000+ 0 6.61400+ 6          0          0          1          21271 4 24  780
          2          2                                            1271 4 24  781
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1271 4 24  782
 0.00000+ 0 2.00000+ 7          0          0          1          21271 4 24  783
          2          2                                            1271 4 24  784
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1271 4 24  785
                                                                  1271 4  0  786
 3.00600+ 3 5.96340+ 0          0          2          0          01271 4 52  787
 0.00000+ 0 0.00000+ 0          0          2          0          01271 4 52  788
 0.00000+ 0 0.00000+ 0          0          0          1          21271 4 52  789
          2          2                                            1271 4 52  790
 0.00000+ 0 4.15800+ 6          0          0          1          21271 4 52  791
          2          2                                            1271 4 52  792
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1271 4 52  793
 0.00000+ 0 2.00000+ 7          0          0          1          21271 4 52  794
          2          2                                            1271 4 52  795
-1.00000+ 0 5.00000- 1 1.00000+ 0 5.00000- 1                      1271 4 52  796
                                                                  1271 4  0  797
 3.00600+ 3 5.96340+ 0          0          2          0          01271 4 91  798
 0.00000+ 0 0.00000+ 0          0          1          0          01271 4 91  799
 0.00000+ 0 0.00000+ 0          0          0          1         161271 4 91  800
         16          2                                            1271 4 91  801
 0.00000+ 0 1.71800+ 6          0          0          1         111271 4 91  802
         11          2                                            1271 4 91  803
-1.00000+ 0 3.05300- 1-8.00000- 1 3.09400- 1-6.00000- 1 3.26200- 11271 4 91  804
-4.00000- 1 3.69600- 1-2.00000- 1 4.29100- 1 0.00000+ 0 5.02200- 11271 4 91  805
 2.00000- 1 5.72100- 1 4.00000- 1 6.25200- 1 6.00000- 1 6.66900- 11271 4 91  806
 8.00000- 1 6.95100- 1 1.00000+ 0 7.03100- 1                      1271 4 91  807
 0.00000+ 0 4.15800+ 6          0          0          1         111271 4 91  808
         11          2                                            1271 4 91  809
-1.00000+ 0 2.33700- 1-8.00000- 1 2.44620- 1-6.00000- 1 2.62060- 11271 4 91  810
-4.00000- 1 2.92360- 1-2.00000- 1 3.34760- 1 0.00000+ 0 4.04760- 11271 4 91  811
 2.00000- 1 4.95680- 1 4.00000- 1 6.06190- 1 6.00000- 1 7.68520- 11271 4 91  812
 8.00000- 1 9.61390- 1 1.00000+ 0 1.02550+ 0                      1271 4 91  813
 0.00000+ 0 4.40000+ 6          0          0          1         111271 4 91  814
         11          2                                            1271 4 91  815
-1.00000+ 0 2.26600- 1-8.00000- 1 2.38200- 1-6.00000- 1 2.55700- 11271 4 91  816
-4.00000- 1 2.84700- 1-2.00000- 1 3.25400- 1 0.00000+ 0 3.95100- 11271 4 91  817
 2.00000- 1 4.88100- 1 4.00000- 1 6.04300- 1 6.00000- 1 7.78600- 11271 4 91  818
 8.00000- 1 9.87800- 1 1.00000+ 0 1.05750+ 0                      1271 4 91  819
 0.00000+ 0 5.10000+ 6          0          0          1         111271 4 91  820
         11          2                                            1271 4 91  821
-1.00000+ 0 2.69400- 1-8.00000- 1 2.64400- 1-6.00000- 1 2.84700- 11271 4 91  822
-4.00000- 1 3.15200- 1-2.00000- 1 3.66000- 1 0.00000+ 0 4.37200- 11271 4 91  823
 2.00000- 1 5.18600- 1 4.00000- 1 6.20200- 1 6.00000- 1 7.42200- 11271 4 91  824
 8.00000- 1 8.64300- 1 1.00000+ 0 9.04900- 1                      1271 4 91  825
 0.00000+ 0 5.40000+ 6          0          0          1         111271 4 91  826
         11          2                                            1271 4 91  827
-1.00000+ 0 2.02000- 1-8.00000- 1 2.02000- 1-6.00000- 1 2.21000- 11271 4 91  828
-4.00000- 1 2.84100- 1-2.00000- 1 3.91400- 1 0.00000+ 0 5.05100- 11271 4 91  829
 2.00000- 1 6.18700- 1 4.00000- 1 7.19700- 1 6.00000- 1 7.70200- 11271 4 91  830
 8.00000- 1 7.89100- 1 1.00000+ 0 7.95500- 1                      1271 4 91  831
 0.00000+ 0 5.80000+ 6          0          0          1         111271 4 91  832
         11          2                                            1271 4 91  833
-1.00000+ 0 1.51300- 1-8.00000- 1 1.95500- 1-6.00000- 1 2.52200- 11271 4 91  834
-4.00000- 1 3.15300- 1-2.00000- 1 3.78300- 1 0.00000+ 0 4.41400- 11271 4 91  835
 2.00000- 1 5.17000- 1 4.00000- 1 6.62000- 1 6.00000- 1 8.19700- 11271 4 91  836
 8.00000- 1 8.95300- 1 1.00000+ 0 8.95300- 1                      1271 4 91  837
 0.00000+ 0 6.50000+ 6          0          0          1         111271 4 91  838
         11          2                                            1271 4 91  839
-1.00000+ 0 2.38600- 1-8.00000- 1 2.64500- 1-6.00000- 1 3.00800- 11271 4 91  840
-4.00000- 1 3.42300- 1-2.00000- 1 3.83800- 1 0.00000+ 0 4.30500- 11271 4 91  841
 2.00000- 1 4.77200- 1 4.00000- 1 5.34200- 1 6.00000- 1 6.22400- 11271 4 91  842
 8.00000- 1 9.64700- 1 1.00000+ 0 1.12030+ 0                      1271 4 91  843
 0.00000+ 0 7.00000+ 6          0          0          1         111271 4 91  844
         11          2                                            1271 4 91  845
-1.00000+ 0 2.23500- 1-8.00000- 1 2.40700- 1-6.00000- 1 2.75100- 11271 4 91  846
-4.00000- 1 3.15200- 1-2.00000- 1 3.66800- 1 0.00000+ 0 4.24100- 11271 4 91  847
 2.00000- 1 4.92800- 1 4.00000- 1 5.73100- 1 6.00000- 1 6.64800- 11271 4 91  848
 8.00000- 1 9.39800- 1 1.00000+ 0 1.19200+ 0                      1271 4 91  849
 0.00000+ 0 7.50000+ 6          0          0          1         111271 4 91  850
         11          2                                            1271 4 91  851
-1.00000+ 0 1.86200- 1-8.00000- 1 2.12800- 1-6.00000- 1 2.52700- 11271 4 91  852
-4.00000- 1 2.92600- 1-2.00000- 1 3.45700- 1 0.00000+ 0 4.25500- 11271 4 91  853
 2.00000- 1 5.18600- 1 4.00000- 1 6.31600- 1 6.00000- 1 8.97600- 11271 4 91  854
 8.00000- 1 8.77700- 1 1.00000+ 0 9.04300- 1                      1271 4 91  855
 0.00000+ 0 8.00000+ 6          0          0          1         111271 4 91  856
         11          2                                            1271 4 91  857
-1.00000+ 0 2.19800- 1-8.00000- 1 2.47300- 1-6.00000- 1 2.88500- 11271 4 91  858
-4.00000- 1 3.43400- 1-2.00000- 1 4.05200- 1 0.00000+ 0 4.73900- 11271 4 91  859
 2.00000- 1 5.49500- 1 4.00000- 1 6.31900- 1 6.00000- 1 7.28000- 11271 4 91  860
 8.00000- 1 8.10400- 1 1.00000+ 0 8.24200- 1                      1271 4 91  861
 0.00000+ 0 9.30000+ 6          0          0          1         111271 4 91  862
         11          2                                            1271 4 91  863
-1.00000+ 0 2.31800- 1-8.00000- 1 2.31800- 1-6.00000- 1 2.40100- 11271 4 91  864
-4.00000- 1 2.48300- 1-2.00000- 1 2.64900- 1 0.00000+ 0 3.56000- 11271 4 91  865
 2.00000- 1 5.13200- 1 4.00000- 1 6.95400- 1 6.00000- 1 8.77500- 11271 4 91  866
 8.00000- 1 9.60300- 1 1.00000+ 0 9.93400- 1                      1271 4 91  867
 0.00000+ 0 1.06000+ 7          0          0          1         111271 4 91  868
         11          2                                            1271 4 91  869
-1.00000+ 0 1.51500- 1-8.00000- 1 1.61000- 1-6.00000- 1 1.89400- 11271 4 91  870
-4.00000- 1 2.55700- 1-2.00000- 1 3.78800- 1 0.00000+ 0 5.30300- 11271 4 91  871
 2.00000- 1 6.53400- 1 4.00000- 1 7.57600- 1 6.00000- 1 8.14400- 11271 4 91  872
 8.00000- 1 8.04900- 1 1.00000+ 0 7.57600- 1                      1271 4 91  873
 0.00000+ 0 1.20000+ 7          0          0          1         111271 4 91  874
         11          2                                            1271 4 91  875
-1.00000+ 0 2.98500- 1-8.00000- 1 3.07300- 1-6.00000- 1 3.16100- 11271 4 91  876
-4.00000- 1 3.33600- 1-2.00000- 1 3.68700- 1 0.00000+ 0 4.21400- 11271 4 91  877
 2.00000- 1 4.91700- 1 4.00000- 1 5.97000- 1 6.00000- 1 7.37500- 11271 4 91  878
 8.00000- 1 8.42800- 1 1.00000+ 0 8.69200- 1                      1271 4 91  879
 0.00000+ 0 1.40000+ 7          0          0          1         111271 4 91  880
         11          2                                            1271 4 91  881
-1.00000+ 0 3.76600- 1-8.00000- 1 3.76600- 1-6.00000- 1 3.87000- 11271 4 91  882
-4.00000- 1 4.07900- 1-2.00000- 1 4.39300- 1 0.00000+ 0 4.81200- 11271 4 91  883
 2.00000- 1 5.23000- 1 4.00000- 1 5.96200- 1 6.00000- 1 6.27600- 11271 4 91  884
 8.00000- 1 6.48500- 1 1.00000+ 0 6.48500- 1                      1271 4 91  885
 0.00000+ 0 1.50000+ 7          0          0          1         111271 4 91  886
         11          2                                            1271 4 91  887
-1.00000+ 0 4.07200- 1-8.00000- 1 4.15000- 1-6.00000- 1 4.26000- 11271 4 91  888
-4.00000- 1 4.45000- 1-2.00000- 1 4.71000- 1 0.00000+ 0 5.00500- 11271 4 91  889
 2.00000- 1 5.32000- 1 4.00000- 1 5.55000- 1 6.00000- 1 5.73000- 11271 4 91  890
 8.00000- 1 5.84500- 1 1.00000+ 0 5.89000- 1                      1271 4 91  891
 0.00000+ 0 2.00000+ 7          0          0          1         111271 4 91  892
         11          2                                            1271 4 91  893
-1.00000+ 0 5.68000- 1-8.00000- 1 5.73000- 1-6.00000- 1 5.82000- 11271 4 91  894
-4.00000- 1 6.11000- 1-2.00000- 1 6.11000- 1 0.00000+ 0 6.26000- 11271 4 91  895
 2.00000- 1 5.87000- 1 4.00000- 1 3.46500- 1 6.00000- 1 2.89000- 11271 4 91  896
 8.00000- 1 3.27000- 1 1.00000+ 0 3.27000- 1                      1271 4 91  897
                                                                  1271 4  0  898
                                                                  1271 0  0  899
 3.00600+ 3 5.96340+ 0          0          0          1          01271 5 24  900
 6.61400+ 6 0.00000+ 0          0          9          1          21271 5 24  901
          2          2                                            1271 5 24  902
 6.61400+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1271 5 24  903
 0.00000+ 0 0.00000+ 0          0          0          1          21271 5 24  904
          2          5                                            1271 5 24  905
 6.61400+ 6 5.40100+ 5 2.00000+ 7 9.39090+ 5                      1271 5 24  906
                                                                  1271 5  0  907
 3.00600+ 3 5.96340+ 0          0          0          1          01271 5 91  908
 1.47100+ 6 0.00000+ 0          0          9          1          21271 5 91  909
          2          2                                            1271 5 91  910
 1.71800+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1271 5 91  911
 0.00000+ 0 0.00000+ 0          0          0          1          31271 5 91  912
          3          2                                            1271 5 91  913
 1.71800+ 6 5.00000+ 4 4.10000+ 6 7.50000+ 5 2.00000+ 7 8.40000+ 61271 5 91  914
                                                                  1271 5  0  915
                                                                  1271 0  0  916
 3.00600+ 3 5.96340+ 0          1          0          1          0127112 52  917
 3.56200+ 6 3.56200+ 6          0          2          1          2127112 52  918
          2          2                                            127112 52  919
 4.15800+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      127112 52  920
                                                                  127112  0  921
 3.00600+ 3 5.96340+ 0          1          0          3          0127112102  922
 0.00000+ 0 0.00000+ 0          0          0          1          2127112102  923
          2          2                                            127112102  924
 1.00000- 5 1.39000+ 0 2.00000+ 7 1.39000+ 0                      127112102  925
 7.25000+ 6 0.00000+ 0          2          2          1          2127112102  926
          2          2                                            127112102  927
 1.00000- 5 6.10000- 1 2.00000+ 7 6.10000- 1                      127112102  928
 6.77300+ 6 0.00000+ 0          2          2          1          2127112102  929
          2          2                                            127112102  930
 1.00000- 5 3.90000- 1 2.00000+ 7 3.90000- 1                      127112102  931
 4.77600+ 5 0.00000+ 0          1          2          1          2127112102  932
          2          2                                            127112102  933
 1.00000- 5 3.90000- 1 2.00000+ 7 3.90000- 1                      127112102  934
                                                                  127112  0  935
                                                                  1271 0  0  936
 3.00600+ 3 5.96340+ 0          1          0          1          0127114 52  937
                                                                  127114  0  938
 3.00600+ 3 5.96340+ 0          1          0          3          0127114102  939
                                                                  127114  0  940
                                                                  1271 0  0  941
                                                                     0 0  0  942
 3.00700+ 3 6.95570+ 0          0          0          0         261272 1451    1
 0.00000+ 0 0.00000+ 0          0          0        137          01272 1451    2
  3-li-  7 lasl       eval-oct72 r.j.labauve, l.stewart, m.battat 1272 1451    3
                      dist-may74                                  1272 1451    4
* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 1272 1451    5
*                                                               * 1272 1451    6
*       photon production added by labauve and stewart at       * 1272 1451    7
*                        lasl. oct. 1972.                       * 1272 1451    8
*                                                               * 1272 1451    9
*       total cross section evaluation above 0.5 mev by foster  * 1272 1451   10
*       also added.  data from 0.5 to 1.3 mev based on measure- * 1272 1451   11
*       ments of me70. above 1.3 mev, based on go71, slightly   * 1272 1451   12
*       normalized to improve agreement with fo71, br58, co52,  * 1272 1451   13
*       and pe60. accuracy is approximately 2 percent at 0.5    * 1272 1451   14
*       mev and 1 percent above 1 mev.   polynomial smoothing   * 1272 1451   15
*       throughout. version 3 nonelastic subtracted from new    * 1272 1451   16
*       total to get new elastic cross section.                 * 1272 1451   17
*                                                               * 1272 1451   18
* br58  a.bratenahl et al, phys.rev. 110,927 (1958)             * 1272 1451   19
* co52  j.h.coon et al, phys.rev. 88,562 (1952)                 * 1272 1451   20
* fo71  d.g.foster,jr., d.w.glasgow, phys.rev. c3,576 (1971)    * 1272 1451   21
* go71  c.a.goulding et al, (rpi) private communication (1971)  * 1272 1451   22
* me70  j.w.meadows, j.f.whalen, nucl.sci.eng. 41,351 (1970)    * 1272 1451   23
* pe60  j.m.peterson et al, phys.rev. 120,521 (1960)            * 1272 1451   24
*                                                               * 1272 1451   25
* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 1272 1451   26
 li-7      lasl       eval-sep69 m.e.battat and r.j.labauve       1272 1451   27
                      dist-jan72 rev-mar71                        1272 1451   28
 *         *          *          *         *          *          *1272 1451   29
                                                                  1272 1451   30
lithium-7 cross sections  material 1006  endf/b  september 1969   1272 1451   31
                                                                  1272 1451   32
******  data modified for endf/b-ii format, march 1971.       **  1272 1451   33
data submitted by m. e. battat and r. j. labauve, lasl.           1272 1451   34
                                                                  1272 1451   35
unless otherwise noted, the li-7 data - data file number (dfn)    1272 1451   36
 215, mark label a - in the ukaea nuclear data library are        1272 1451   37
 tabulated.   energy range is 1.0e-5 ev to 15 mev.                1272 1451   38
                                                                  1272 1451   39
basic reference for this nuclide is awre report o-61/64 (july     1272 1451   40
 1964), which gives data for dfn-176.  as per awre report o-55/65 1272 1451   41
 (april 1965), dfn 215 has same data as dfn-176 but with slightly 1272 1451   42
 lower elastic cross sections between 0.01 and 0.2 mev.  data     1272 1451   43
 below 0.001 ev were added at aee, winfrith, in january 1967 and  1272 1451   44
 nuclide identified as 215a (see aeew-m 802, february 1968).  in  1272 1451   45
 august 1967, temperature was revised to zero degrees kelvin and  1272 1451   46
 nuclide identified as 215d.  at this date, listing of 215d was   1272 1451   47
 not available at lasl.  it has been assumed that this change is  1272 1451   48
 a flag for the ukaea processing codes and no cross section       1272 1451   49
 changes were made in 215d.                                       1272 1451   50
                                                                  1272 1451   51
                                                                  1272 1451   52
data for this material are summarized below - -                   1272 1451   53
                                                                  1272 1451   54
**mf = 1**  general information and comment cards                 1272 1451   55
                                                                  1272 1451   56
**mf = 2**  scattering radius only.                               1272 1451   57
                                                                  1272 1451   58
**mf = 3**  smooth cross sections                                 1272 1451   59
            mt=  1  total                                         1272 1451   60
            mt=  2  elastic                                       1272 1451   61
            mt=  4  (n,n prime)gamma + (n,n prime)alpha-t         1272 1451   62
            mt= 16  (n,2n)                                        1272 1451   63
            mt= 24  (n,2n)alpha-d                                 1272 1451   64
            mt= 51  (n,n prime)gamma                              1272 1451   65
            mt= 91  (n,n prime)alpha-t                            1272 1451   66
            mt=102  (n,gamma)                                     1272 1451   67
            mt=104  (n,d)                                         1272 1451   68
            mt=251  mu-bar--average cosine of scattering angle    1272 1451   69
            mt=252  xi-average logarithmic energy decrement       1272 1451   70
            mt=253  gamma                                         1272 1451   71
                                                                  1272 1451   72
**mf = 4**  secondary angular distributions                       1272 1451   73
                                                                  1272 1451   74
            mt=  2  legendre/(c) system/transformation matrix     1272 1451   75
                    given.  data from h. alter of a-i.  (private  1272 1451   76
                    communication).                               1272 1451   77
                                                                  1272 1451   78
            mt= 16  tabular/(l) system.  8.300 to 15 mev.         1272 1451   79
                                                                  1272 1451   80
            mt= 24  tabular/(l) system.  10.00 to 15 mev.         1272 1451   81
                                                                  1272 1451   82
            mt= 51  tabular/(c) system.  0.550 to 15 mev.         1272 1451   83
                                                                  1272 1451   84
            mt= 91  tabular/(l) system.  2.821 to 15 mev.         1272 1451   85
                                                                  1272 1451   86
**mf = 5**  secondary energy distributions                        1272 1451   87
                                                                  1272 1451   88
            mt= 16  (n,2n).  energy range is 8.3 to 15 mev.       1272 1451   89
                    distribution appro.imated by endf/b law 9,    1272 1451   90
                    with theta (mev) equal                        1272 1451   91
                        0.21 * sqrt(e)                            1272 1451   92
                    this corresponds to an average theta of 0.7   1272 1451   93
                    mev in the 8.3 to 15 mev energy interval.     1272 1451   94
                                                                  1272 1451   95
            mt= 24  (n, 2n)alpha-d.  energy range is 10 to 15     1272 1451   96
                    mev.  distribution appro.imated by endf/b law 1272 1451   97
                    9, with theta (mev) equal                     1272 1451   98
                        0.1133 * sqrt(e).                         1272 1451   99
                    this corresponds to an average theta of 0.4   1272 1451  100
                    mev in the 10 to 15 mev energy interval.      1272 1451  101
                                                                  1272 1451  102
            mt= 91  (n, n prime)alpha-t.  distributions appro.-   1272 1451  103
                    imated using law 9.  theta values obtained    1272 1451  104
                    by linear interpolation between following     1272 1451  105
                    points - - -                                  1272 1451  106
                        e = 2.821 mev, theta =0.10 mev            1272 1451  107
                        e = 5.8   mev, theta =0.70 mev            1272 1451  108
                        e = 8.0   mev, theta =2.80 mev            1272 1451  109
                        e =15.0   mev, theta =5.35 mev            1272 1451  110
                                                                  1272 1451  111
                    data include the cross section to the second  1272 1451  112
                    level and do not always conserve energy.      1272 1451  113
                                                                  1272 1451  114
mf=12                                                             1272 1451  115
                                                                  1272 1451  116
                                                                  1272 1451  117
            mt= 51  the first level in li-7 is the only known     1272 1451  118
                    level which is a gamma emitter.               1272 1451  119
                                                                  1272 1451  120
            mt=102  measurements in the thermal capture spectra   1272 1451  121
                    are inconclusive, so much so that selove and  1272 1451  122
                    lauritsen make no recommendations in their    1272 1451  123
                    recent review article (p.c., to be published).1272 1451  124
                    therefore, the transition probabilities are   1272 1451  125
                    guessed using the energies of selove and      1272 1451  126
                    lauritsen.                                    1272 1451  127
                                                                  1272 1451  128
    the lp flag was used to describe the mt=102 photons           1272 1451  129
                                                                  1272 1451  130
mf=14                                                             1272 1451  131
                                                                  1272 1451  132
            mt= 51  according to spin and parity assignments,     1272 1451  133
                    the gammas should be emitted isotropically.   1272 1451  134
                                                                  1272 1451  135
            mt=102  all gammas are assumed to be emitted          1272 1451  136
                    isotropically.                                1272 1451  137
                                                                  1272 1451  138
                                                                  1272 1451  139
                                1        451        165           1272 1451  140
                                2        151          4           1272 1451  141
                                3          1         59           1272 1451  142
                                3          2         59           1272 1451  143
                                3          4         23           1272 1451  144
                                3         16          8           1272 1451  145
                                3         24          7           1272 1451  146
                                3         51         23           1272 1451  147
                                3         91         17           1272 1451  148
                                3        102         11           1272 1451  149
                                3        104          8           1272 1451  150
                                3        251          9           1272 1451  151
                                3        252          9           1272 1451  152
                                3        253          9           1272 1451  153
                                4          2         84           1272 1451  154
                                4         16         10           1272 1451  155
                                4         24         10           1272 1451  156
                                4         51         10           1272 1451  157
                                4         91         79           1272 1451  158
                                5         16          7           1272 1451  159
                                5         24          7           1272 1451  160
                                5         91          8           1272 1451  161
                               12         51          4           1272 1451  162
                               12        102         13           1272 1451  163
                               14         51          1           1272 1451  164
                               14        102          1           1272 1451  165
                                                                  1272 1  0  166
                                                                  1272 0  0  167
 3.00700+ 3 6.95570+ 0          0          0          1          01272 2151  168
 3.00700+ 3 1.00000+ 0          0          0          1          01272 2151  169
 1.00000- 5 1.00000+ 5          0          0          0          01272 2151  170
 1.50000+ 0 2.89060- 1          0          0          0          01272 2151  171
                                                                  1272 2  0  172
                                                                  1272 0  0  173
 3.00700+ 3 6.95570+ 0          0         99          0          01272 3  1  174
 0.00000+ 0 0.00000+ 0          0          0          2        1661272 3  1  175
         47          5        166          2                      1272 3  1  176
 1.00000- 5 2.76000+ 0 1.00000- 3 1.22100+ 0 2.00000- 3 1.17300+ 01272 3  1  177
 4.00000- 3 1.13700+ 0 5.00000- 3 1.12800+ 0 6.00000- 3 1.12200+ 01272 3  1  178
 7.00000- 3 1.11700+ 0 8.00000- 3 1.11200+ 0 9.00000- 3 1.10900+ 01272 3  1  179
 1.00000- 2 1.10600+ 0 2.00000- 2 1.09000+ 0 2.53000- 2 1.08600+ 01272 3  1  180
 1.00000- 1 1.06800+ 0 1.00000+ 0 1.05500+ 0 1.00000+ 1 1.05100+ 01272 3  1  181
 1.00000+ 2 1.05000+ 0 1.00000+ 3 1.05000+ 0 1.00000+ 4 1.05000+ 01272 3  1  182
 1.00000+ 5 9.29900- 1 1.30000+ 5 9.60000- 1 1.50000+ 5 1.05000+ 01272 3  1  183
 1.70000+ 5 1.20000+ 0 1.85000+ 5 1.38000+ 0 2.00000+ 5 1.70000+ 01272 3  1  184
 2.10000+ 5 2.03000+ 0 2.20000+ 5 2.50000+ 0 2.30000+ 5 4.50000+ 01272 3  1  185
 2.40000+ 5 6.30000+ 0 2.50000+ 5 1.05000+ 1 2.58000+ 5 1.09000+ 11272 3  1  186
 2.60000+ 5 1.05000+ 1 2.70000+ 5 6.80000+ 0 2.80000+ 5 4.75000+ 01272 3  1  187
 2.90000+ 5 3.60000+ 0 3.00000+ 5 2.72000+ 0 3.10000+ 5 2.25000+ 01272 3  1  188
 3.20000+ 5 2.05000+ 0 3.30000+ 5 1.80000+ 0 3.40000+ 5 1.60000+ 01272 3  1  189
 3.50000+ 5 1.46000+ 0 3.60000+ 5 1.38000+ 0 3.70000+ 5 1.32000+ 01272 3  1  190
 3.80000+ 5 1.28000+ 0 3.90000+ 5 1.25000+ 0 4.00000+ 5 1.22590+ 01272 3  1  191
 4.50000+ 5 1.12000+ 0 5.00000+ 5 1.05400+ 0 5.30000+ 5 1.03540+ 01272 3  1  192
 5.50000+ 5 1.02300+ 0 6.00000+ 5 1.03300+ 0 6.50000+ 5 1.06500+ 01272 3  1  193
 7.00000+ 5 1.11500+ 0 8.00000+ 5 1.22300+ 0 9.00000+ 5 1.38000+ 01272 3  1  194
 1.00000+ 6 1.57300+ 0 1.10000+ 6 1.69000+ 0 1.20000+ 6 1.73800+ 01272 3  1  195
 1.30000+ 6 1.75500+ 0 1.40000+ 6 1.72200+ 0 1.50000+ 6 1.70500+ 01272 3  1  196
 1.60000+ 6 1.70900+ 0 1.70000+ 6 1.70300+ 0 1.80000+ 6 1.71600+ 01272 3  1  197
 1.90000+ 6 1.74000+ 0 2.00000+ 6 1.75500+ 0 2.10000+ 6 1.78600+ 01272 3  1  198
 2.20000+ 6 1.82700+ 0 2.30000+ 6 1.86700+ 0 2.40000+ 6 1.90100+ 01272 3  1  199
 2.50000+ 6 1.93200+ 0 2.60000+ 6 1.96600+ 0 2.70000+ 6 1.98800+ 01272 3  1  200
 2.80000+ 6 2.01300+ 0 2.82100+ 6 2.01720+ 0 2.90000+ 6 2.03300+ 01272 3  1  201
 3.00000+ 6 2.05000+ 0 3.10000+ 6 2.06400+ 0 3.20000+ 6 2.06800+ 01272 3  1  202
 3.30000+ 6 2.07800+ 0 3.40000+ 6 2.09800+ 0 3.50000+ 6 2.13100+ 01272 3  1  203
 3.60000+ 6 2.17200+ 0 3.70000+ 6 2.21600+ 0 3.80000+ 6 2.26500+ 01272 3  1  204
 3.90000+ 6 2.31700+ 0 4.00000+ 6 2.37000+ 0 4.10000+ 6 2.42500+ 01272 3  1  205
 4.20000+ 6 2.47200+ 0 4.30000+ 6 2.51000+ 0 4.40000+ 6 2.53500+ 01272 3  1  206
 4.50000+ 6 2.54400+ 0 4.60000+ 6 2.53700+ 0 4.70000+ 6 2.51900+ 01272 3  1  207
 4.80000+ 6 2.48200+ 0 4.90000+ 6 2.43100+ 0 5.00000+ 6 2.38200+ 01272 3  1  208
 5.10000+ 6 2.32700+ 0 5.20000+ 6 2.25800+ 0 5.30000+ 6 2.16300+ 01272 3  1  209
 5.40000+ 6 2.11100+ 0 5.50000+ 6 2.09900+ 0 5.60000+ 6 2.11100+ 01272 3  1  210
 5.70000+ 6 2.13500+ 0 5.80000+ 6 2.15800+ 0 5.90000+ 6 2.15800+ 01272 3  1  211
 6.00000+ 6 2.14700+ 0 6.10000+ 6 2.12900+ 0 6.20000+ 6 2.10800+ 01272 3  1  212
 6.30000+ 6 2.08500+ 0 6.40000+ 6 2.06200+ 0 6.50000+ 6 2.04000+ 01272 3  1  213
 6.60000+ 6 2.02000+ 0 6.70000+ 6 2.00100+ 0 6.80000+ 6 1.98300+ 01272 3  1  214
 6.90000+ 6 1.96500+ 0 7.00000+ 6 1.94800+ 0 7.10000+ 6 1.93200+ 01272 3  1  215
 7.20000+ 6 1.91700+ 0 7.30000+ 6 1.90300+ 0 7.40000+ 6 1.88900+ 01272 3  1  216
 7.50000+ 6 1.87600+ 0 7.60000+ 6 1.86400+ 0 7.70000+ 6 1.85300+ 01272 3  1  217
 7.80000+ 6 1.84200+ 0 7.90000+ 6 1.83200+ 0 8.00000+ 6 1.82200+ 01272 3  1  218
 8.20000+ 6 1.80500+ 0 8.30000+ 6 1.79800+ 0 8.40000+ 6 1.79100+ 01272 3  1  219
 8.60000+ 6 1.77900+ 0 8.80000+ 6 1.77000+ 0 8.88000+ 6 1.76400+ 01272 3  1  220
 9.00000+ 6 1.75500+ 0 9.20000+ 6 1.74000+ 0 9.40000+ 6 1.72500+ 01272 3  1  221
 9.60000+ 6 1.71000+ 0 9.80000+ 6 1.69500+ 0 1.00000+ 7 1.68000+ 01272 3  1  222
 1.02000+ 7 1.66500+ 0 1.04000+ 7 1.65000+ 0 1.05000+ 7 1.64300+ 01272 3  1  223
 1.06000+ 7 1.63600+ 0 1.08000+ 7 1.62300+ 0 1.10000+ 7 1.61400+ 01272 3  1  224
 1.12000+ 7 1.60600+ 0 1.14000+ 7 1.59800+ 0 1.15000+ 7 1.59350+ 01272 3  1  225
 1.16000+ 7 1.58900+ 0 1.18000+ 7 1.58000+ 0 1.20000+ 7 1.57100+ 01272 3  1  226
 1.25000+ 7 1.54600+ 0 1.30000+ 7 1.51800+ 0 1.35000+ 7 1.48500+ 01272 3  1  227
 1.40000+ 7 1.45400+ 0 1.45000+ 7 1.42500+ 0 1.50000+ 7 1.39900+ 01272 3  1  228
 1.55000+ 7 1.38000+ 0 1.60000+ 7 1.36000+ 0 1.65000+ 7 1.34100+ 01272 3  1  229
 1.70000+ 7 1.32100+ 0 1.75000+ 7 1.30200+ 0 1.80000+ 7 1.28200+ 01272 3  1  230
 1.85000+ 7 1.26200+ 0 1.90000+ 7 1.24100+ 0 1.95000+ 7 1.22100+ 01272 3  1  231
 2.00000+ 7 1.20200+ 0                                            1272 3  1  232
                                                                  1272 3  0  233
 3.00700+ 3 6.95570+ 0          0          0          0          01272 3  2  234
 0.00000+ 0 0.00000+ 0          0          0          1        1661272 3  2  235
        166          2                                            1272 3  2  236
 1.00000- 5 1.05000+ 0 1.00000- 3 1.05000+ 0 2.00000- 3 1.05000+ 01272 3  2  237
 4.00000- 3 1.04950+ 0 5.00000- 3 1.04950+ 0 6.00000- 3 1.05000+ 01272 3  2  238
 7.00000- 3 1.05000+ 0 8.00000- 3 1.04950+ 0 9.00000- 3 1.04950+ 01272 3  2  239
 1.00000- 2 1.04950+ 0 2.00000- 2 1.04980+ 0 2.53000- 2 1.05000+ 01272 3  2  240
 1.00000- 1 1.04980+ 0 1.00000+ 0 1.04920+ 0 1.00000+ 1 1.04920+ 01272 3  2  241
 1.00000+ 2 1.04940+ 0 1.00000+ 3 1.04980+ 0 1.00000+ 4 1.04990+ 01272 3  2  242
 1.00000+ 5 9.29880- 1 1.30000+ 5 9.59980- 1 1.50000+ 5 1.05000+ 01272 3  2  243
 1.70000+ 5 1.20000+ 0 1.85000+ 5 1.38000+ 0 2.00000+ 5 1.70000+ 01272 3  2  244
 2.10000+ 5 2.03000+ 0 2.20000+ 5 2.50000+ 0 2.30000+ 5 4.50000+ 01272 3  2  245
 2.40000+ 5 6.30000+ 0 2.50000+ 5 1.05000+ 1 2.58000+ 5 1.09000+ 11272 3  2  246
 2.60000+ 5 1.05000+ 1 2.70000+ 5 6.80000+ 0 2.80000+ 5 4.75000+ 01272 3  2  247
 2.90000+ 5 3.60000+ 0 3.00000+ 5 2.72000+ 0 3.10000+ 5 2.25000+ 01272 3  2  248
 3.20000+ 5 2.05000+ 0 3.30000+ 5 1.80000+ 0 3.40000+ 5 1.60000+ 01272 3  2  249
 3.50000+ 5 1.46000+ 0 3.60000+ 5 1.38000+ 0 3.70000+ 5 1.32000+ 01272 3  2  250
 3.80000+ 5 1.28000+ 0 3.90000+ 5 1.25000+ 0 4.00000+ 5 1.22590+ 01272 3  2  251
 4.50000+ 5 1.12000+ 0 5.00000+ 5 1.05400+ 0 5.30000+ 5 1.03540+ 01272 3  2  252
 5.50000+ 5 1.02300+ 0 6.00000+ 5 1.01300+ 0 6.50000+ 5 1.03280+ 01272 3  2  253
 7.00000+ 5 1.06500+ 0 8.00000+ 5 1.14300+ 0 9.00000+ 5 1.26500+ 01272 3  2  254
 1.00000+ 6 1.41800+ 0 1.10000+ 6 1.52000+ 0 1.20000+ 6 1.54800+ 01272 3  2  255
 1.30000+ 6 1.56000+ 0 1.40000+ 6 1.52400+ 0 1.50000+ 6 1.50500+ 01272 3  2  256
 1.60000+ 6 1.50900+ 0 1.70000+ 6 1.50400+ 0 1.80000+ 6 1.51800+ 01272 3  2  257
 1.90000+ 6 1.54400+ 0 2.00000+ 6 1.56000+ 0 2.10000+ 6 1.59200+ 01272 3  2  258
 2.20000+ 6 1.63400+ 0 2.30000+ 6 1.67300+ 0 2.40000+ 6 1.70600+ 01272 3  2  259
 2.50000+ 6 1.73650+ 0 2.60000+ 6 1.77000+ 0 2.70000+ 6 1.78920+ 01272 3  2  260
 2.80000+ 6 1.81150+ 0 2.82100+ 6 1.81520+ 0 2.90000+ 6 1.82440+ 01272 3  2  261
 3.00000+ 6 1.83300+ 0 3.10000+ 6 1.83560+ 0 3.20000+ 6 1.82800+ 01272 3  2  262
 3.30000+ 6 1.82460+ 0 3.40000+ 6 1.83100+ 0 3.50000+ 6 1.85500+ 01272 3  2  263
 3.60000+ 6 1.88700+ 0 3.70000+ 6 1.92600+ 0 3.80000+ 6 1.97000+ 01272 3  2  264
 3.90000+ 6 2.01700+ 0 4.00000+ 6 2.06500+ 0 4.10000+ 6 2.11200+ 01272 3  2  265
 4.20000+ 6 2.14900+ 0 4.30000+ 6 2.17700+ 0 4.40000+ 6 2.18900+ 01272 3  2  266
 4.50000+ 6 2.18300+ 0 4.60000+ 6 2.16000+ 0 4.70000+ 6 2.12200+ 01272 3  2  267
 4.80000+ 6 2.06190+ 0 4.90000+ 6 1.98700+ 0 5.00000+ 6 1.91000+ 01272 3  2  268
 5.10000+ 6 1.82420+ 0 5.20000+ 6 1.72300+ 0 5.30000+ 6 1.60520+ 01272 3  2  269
 5.40000+ 6 1.53000+ 0 5.50000+ 6 1.49900+ 0 5.60000+ 6 1.49750+ 01272 3  2  270
 5.70000+ 6 1.50800+ 0 5.80000+ 6 1.52560+ 0 5.90000+ 6 1.52030+ 01272 3  2  271
 6.00000+ 6 1.50400+ 0 6.10000+ 6 1.48370+ 0 6.20000+ 6 1.46040+ 01272 3  2  272
 6.30000+ 6 1.43520+ 0 6.40000+ 6 1.41000+ 0 6.50000+ 6 1.38890+ 01272 3  2  273
 6.60000+ 6 1.36970+ 0 6.70000+ 6 1.35160+ 0 6.80000+ 6 1.33440+ 01272 3  2  274
 6.90000+ 6 1.31720+ 0 7.00000+ 6 1.30100+ 0 7.10000+ 6 1.28770+ 01272 3  2  275
 7.20000+ 6 1.27530+ 0 7.30000+ 6 1.26390+ 0 7.40000+ 6 1.25250+ 01272 3  2  276
 7.50000+ 6 1.24200+ 0 7.60000+ 6 1.23290+ 0 7.70000+ 6 1.22470+ 01272 3  2  277
 7.80000+ 6 1.21650+ 0 7.90000+ 6 1.20930+ 0 8.00000+ 6 1.20200+ 01272 3  2  278
 8.20000+ 6 1.19370+ 0 8.30000+ 6 1.19100+ 0 8.40000+ 6 1.18720+ 01272 3  2  279
 8.60000+ 6 1.18150+ 0 8.80000+ 6 1.17860+ 0 8.88000+ 6 1.17500+ 01272 3  2  280
 9.00000+ 6 1.16900+ 0 9.20000+ 6 1.15980+ 0 9.40000+ 6 1.15010+ 01272 3  2  281
 9.60000+ 6 1.13980+ 0 9.80000+ 6 1.12880+ 0 1.00000+ 7 1.11700+ 01272 3  2  282
 1.02000+ 7 1.10510+ 0 1.04000+ 7 1.09280+ 0 1.05000+ 7 1.08700+ 01272 3  2  283
 1.06000+ 7 1.08380+ 0 1.08000+ 7 1.07780+ 0 1.10000+ 7 1.07500+ 01272 3  2  284
 1.12000+ 7 1.07260+ 0 1.14000+ 7 1.06980+ 0 1.15000+ 7 1.06760+ 01272 3  2  285
 1.16000+ 7 1.06600+ 0 1.18000+ 7 1.06230+ 0 1.20000+ 7 1.05800+ 01272 3  2  286
 1.25000+ 7 1.04270+ 0 1.30000+ 7 1.02700+ 0 1.35000+ 7 9.99990- 11272 3  2  287
 1.40000+ 7 9.73990- 1 1.45000+ 7 9.50990- 1 1.50000+ 7 9.30990- 11272 3  2  288
 1.55000+ 7 9.18580- 1 1.60000+ 7 9.05170- 1 1.65000+ 7 8.92760- 11272 3  2  289
 1.70000+ 7 8.79350- 1 1.75000+ 7 8.66940- 1 1.80000+ 7 8.53530- 11272 3  2  290
 1.85000+ 7 8.40120- 1 1.90000+ 7 8.25710- 1 1.95000+ 7 8.12300- 11272 3  2  291
 2.00000+ 7 7.99900- 1                                            1272 3  2  292
                                                                  1272 3  0  293
 3.00700+ 3 6.95570+ 0          0         99          0          01272 3  4  294
 0.00000+ 0-4.78000+ 5          0          0          3         591272 3  4  295
          2          3         58          5         59          21272 3  4  296
 5.50000+ 5 0.00000+ 0 6.00000+ 5 2.00000- 2 7.00000+ 5 5.00000- 21272 3  4  297
 8.00000+ 5 8.00000- 2 9.00000+ 5 1.15000- 1 1.00000+ 6 1.55000- 11272 3  4  298
 1.10000+ 6 1.70000- 1 1.20000+ 6 1.90000- 1 1.30000+ 6 1.95000- 11272 3  4  299
 1.40000+ 6 1.98000- 1 1.50000+ 6 2.00000- 1 1.60000+ 6 2.00000- 11272 3  4  300
 1.70000+ 6 1.99000- 1 1.80000+ 6 1.98000- 1 1.90000+ 6 1.96000- 11272 3  4  301
 2.00000+ 6 1.95000- 1 2.20000+ 6 1.93000- 1 2.40000+ 6 1.95000- 11272 3  4  302
 2.60000+ 6 1.96000- 1 2.82100+ 6 2.02000- 1 3.00000+ 6 2.17000- 11272 3  4  303
 3.20000+ 6 2.40000- 1 3.40000+ 6 2.67000- 1 3.60000+ 6 2.85000- 11272 3  4  304
 3.80000+ 6 2.95000- 1 4.00000+ 6 3.05000- 1 4.10000+ 6 3.13000- 11272 3  4  305
 4.20000+ 6 3.23000- 1 4.30000+ 6 3.33000- 1 4.40000+ 6 3.46000- 11272 3  4  306
 4.50000+ 6 3.61000- 1 4.60000+ 6 3.77000- 1 4.70000+ 6 3.97000- 11272 3  4  307
 4.90000+ 6 4.44000- 1 5.00000+ 6 4.72000- 1 5.20000+ 6 5.35000- 11272 3  4  308
 5.40000+ 6 5.81000- 1 5.50000+ 6 6.00000- 1 5.70000+ 6 6.27000- 11272 3  4  309
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         11          2                                            1272 4 91  555
-1.00000+ 0 2.40200- 1-8.00000- 1 2.49200- 1-6.00000- 1 2.70200- 11272 4 91  556
-4.00000- 1 3.22700- 1-2.00000- 1 3.90300- 1 0.00000+ 0 4.68300- 11272 4 91  557
 2.00000- 1 5.55400- 1 4.00000- 1 6.53000- 1 6.00000- 1 7.50500- 11272 4 91  558
 8.00000- 1 8.07600- 1 1.00000+ 0 8.25600- 1                      1272 4 91  559
 0.00000+ 0 5.40000+ 6          0          0          1         111272 4 91  560
         11          2                                            1272 4 91  561
-1.00000+ 0 1.96500- 1-8.00000- 1 2.21700- 1-6.00000- 1 2.52600- 11272 4 91  562
-4.00000- 1 2.95700- 1-2.00000- 1 3.64900- 1 0.00000+ 0 4.56600- 11272 4 91  563
 2.00000- 1 5.61400- 1 4.00000- 1 6.73700- 1 6.00000- 1 7.82200- 11272 4 91  564
 8.00000- 1 8.51400- 1 1.00000+ 0 8.83200- 1                      1272 4 91  565
 0.00000+ 0 5.80000+ 6          0          0          1         111272 4 91  566
         11          2                                            1272 4 91  567
-1.00000+ 0 2.43600- 1-8.00000- 1 2.52300- 1-6.00000- 1 2.69700- 11272 4 91  568
-4.00000- 1 3.05400- 1-2.00000- 1 3.56700- 1 0.00000+ 0 4.27200- 11272 4 91  569
 2.00000- 1 5.22000- 1 4.00000- 1 6.49000- 1 6.00000- 1 7.79500- 11272 4 91  570
 8.00000- 1 8.63100- 1 1.00000+ 0 9.06600- 1                      1272 4 91  571
 0.00000+ 0 6.50000+ 6          0          0          1         111272 4 91  572
         11          2                                            1272 4 91  573
-1.00000+ 0 1.45900- 1-8.00000- 1 1.85300- 1-6.00000- 1 2.31700- 11272 4 91  574
-4.00000- 1 3.02000- 1-2.00000- 1 3.94700- 1 0.00000+ 0 5.04500- 11272 4 91  575
 2.00000- 1 6.16100- 1 4.00000- 1 7.12200- 1 6.00000- 1 7.72300- 11272 4 91  576
 8.00000- 1 8.01400- 1 1.00000+ 0 8.13500- 1                      1272 4 91  577
 0.00000+ 0 7.00000+ 6          0          0          1         111272 4 91  578
         11          2                                            1272 4 91  579
-1.00000+ 0 1.82500- 1-8.00000- 1 2.11600- 1-6.00000- 1 2.48100- 11272 4 91  580
-4.00000- 1 3.10900- 1-2.00000- 1 4.01400- 1 0.00000+ 0 4.86100- 11272 4 91  581
 2.00000- 1 5.76600- 1 4.00000- 1 6.72900- 1 6.00000- 1 7.66300- 11272 4 91  582
 8.00000- 1 8.17400- 1 1.00000+ 0 8.34900- 1                      1272 4 91  583
 0.00000+ 0 7.50000+ 6          0          0          1         111272 4 91  584
         11          2                                            1272 4 91  585
-1.00000+ 0 2.58600- 1-8.00000- 1 2.61300- 1-6.00000- 1 2.72200- 11272 4 91  586
-4.00000- 1 2.99400- 1-2.00000- 1 3.67400- 1 0.00000+ 0 4.60000- 11272 4 91  587
 2.00000- 1 5.59300- 1 4.00000- 1 6.65500- 1 6.00000- 1 7.62100- 11272 4 91  588
 8.00000- 1 8.08400- 1 1.00000+ 0 8.30200- 1                      1272 4 91  589
 0.00000+ 0 8.00000+ 6          0          0          1         111272 4 91  590
         11          2                                            1272 4 91  591
-1.00000+ 0 2.31100- 1-8.00000- 1 2.46100- 1-6.00000- 1 2.68600- 11272 4 91  592
-4.00000- 1 3.15400- 1-2.00000- 1 3.81000- 1 0.00000+ 0 4.67200- 11272 4 91  593
 2.00000- 1 5.79600- 1 4.00000- 1 6.84600- 1 6.00000- 1 7.49500- 11272 4 91  594
 8.00000- 1 7.88900- 1 1.00000+ 0 8.07000- 1                      1272 4 91  595
 0.00000+ 0 9.30000+ 6          0          0          1         111272 4 91  596
         11          2                                            1272 4 91  597
-1.00000+ 0 2.12900- 1-8.00000- 1 2.18700- 1-6.00000- 1 2.30200- 11272 4 91  598
-4.00000- 1 2.67000- 1-2.00000- 1 3.45300- 1 0.00000+ 0 4.46600- 11272 4 91  599
 2.00000- 1 5.64000- 1 4.00000- 1 6.97500- 1 6.00000- 1 8.05700- 11272 4 91  600
 8.00000- 1 8.65600- 1 1.00000+ 0 9.06900- 1                      1272 4 91  601
 0.00000+ 0 1.06000+ 7          0          0          1         111272 4 91  602
         11          2                                            1272 4 91  603
-1.00000+ 0 2.33300- 1-8.00000- 1 2.49400- 1-6.00000- 1 2.81600- 11272 4 91  604
-4.00000- 1 3.34700- 1-2.00000- 1 4.02300- 1 0.00000+ 0 4.82700- 11272 4 91  605
 2.00000- 1 5.72000- 1 4.00000- 1 6.53300- 1 6.00000- 1 7.24900- 11272 4 91  606
 8.00000- 1 7.78800- 1 1.00000+ 0 8.07700- 1                      1272 4 91  607
 0.00000+ 0 1.20000+ 7          0          0          1         111272 4 91  608
         11          2                                            1272 4 91  609
-1.00000+ 0 2.15200- 1-8.00000- 1 2.30900- 1-6.00000- 1 2.56500- 11272 4 91  610
-4.00000- 1 2.95400- 1-2.00000- 1 3.48400- 1 0.00000+ 0 4.40300- 11272 4 91  611
 2.00000- 1 5.62700- 1 4.00000- 1 6.92700- 1 6.00000- 1 7.94400- 11272 4 91  612
 8.00000- 1 8.40800- 1 1.00000+ 0 8.60600- 1                      1272 4 91  613
 0.00000+ 0 1.50000+ 7          0          0          1         111272 4 91  614
         11          2                                            1272 4 91  615
-1.00000+ 0 4.53600- 1-8.00000- 1 4.91800- 1-6.00000- 1 5.07600- 11272 4 91  616
-4.00000- 1 5.05400- 1-2.00000- 1 4.81900- 1 0.00000+ 0 4.56100- 11272 4 91  617
 2.00000- 1 4.23600- 1 4.00000- 1 4.16100- 1 6.00000- 1 4.48800- 11272 4 91  618
 8.00000- 1 5.40900- 1 1.00000+ 0 1.00260+ 0                      1272 4 91  619
 0.00000+ 0 2.00000+ 7          0          0          1         111272 4 91  620
         11          2                                            1272 4 91  621
-1.00000+ 0 4.53600- 1-8.00000- 1 4.91800- 1-6.00000- 1 5.07600- 11272 4 91  622
-4.00000- 1 5.05400- 1-2.00000- 1 4.81900- 1 0.00000+ 0 4.56100- 11272 4 91  623
 2.00000- 1 4.23600- 1 4.00000- 1 4.16100- 1 6.00000- 1 4.48800- 11272 4 91  624
 8.00000- 1 5.40900- 1 1.00000+ 0 1.00260+ 0                      1272 4 91  625
                                                                  1272 4  0  626
                                                                  1272 0  0  627
 3.00700+ 3 6.95570+ 0          0          0          1          01272 5 16  628
 8.30000+ 6 0.00000+ 0          0          9          1          21272 5 16  629
          2          2                                            1272 5 16  630
 8.30000+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1272 5 16  631
 0.00000+ 0 0.00000+ 0          0          0          1          21272 5 16  632
          2          5                                            1272 5 16  633
 8.30000+ 6 6.05000+ 5 2.00000+ 7 9.39110+ 5                      1272 5 16  634
                                                                  1272 5  0  635
 3.00700+ 3 6.95570+ 0          0          0          1          01272 5 24  636
 1.00000+ 7 0.00000+ 0          0          9          1          21272 5 24  637
          2          2                                            1272 5 24  638
 1.00000+ 7 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1272 5 24  639
 0.00000+ 0 0.00000+ 0          0          0          1          21272 5 24  640
          2          5                                            1272 5 24  641
 1.00000+ 7 3.58300+ 5 2.00000+ 7 5.06660+ 5                      1272 5 24  642
                                                                  1272 5  0  643
 3.00700+ 3 6.95570+ 0          0          0          1          01272 5 91  644
 2.46600+ 6 0.00000+ 0          0          9          1          21272 5 91  645
          2          2                                            1272 5 91  646
 2.82100+ 6 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1272 5 91  647
 0.00000+ 0 0.00000+ 0          0          0          1          41272 5 91  648
          4          2                                            1272 5 91  649
 2.82100+ 6 1.00000+ 5 5.80000+ 6 7.00000+ 5 8.00000+ 6 2.80000+ 61272 5 91  650
 2.00000+ 7 7.17140+ 6                                            1272 5 91  651
                                                                  1272 5  0  652
                                                                  1272 0  0  653
 3.00700+ 3 6.95570+ 0          1          0          1          0127212 51  654
 4.77600+ 5 4.77600+ 5          0          2          1          2127212 51  655
          2          2                                            127212 51  656
 5.50000+ 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      127212 51  657
                                                                  127212  0  658
 3.00700+ 3 6.95570+ 0          1          0          3          0127212102  659
 0.00000+ 0 0.00000+ 0          0          0          1          2127212102  660
          2          2                                            127212102  661
 1.00000- 5 1.10000+ 0 2.00000+ 7 1.10000+ 0                      127212102  662
 2.03270+ 6 0.00000+ 0          2          2          1          2127212102  663
          2          2                                            127212102  664
 1.00000- 5 9.00000- 1 2.00000+ 7 9.00000- 1                      127212102  665
 1.05190+ 6 0.00000+ 0          2          2          1          2127212102  666
          2          2                                            127212102  667
 1.00000- 5 1.00000- 1 2.00000+ 7 1.00000- 1                      127212102  668
 9.80800+ 5 0.00000+ 0          1          2          1          2127212102  669
          2          2                                            127212102  670
 1.00000- 5 1.00000- 1 2.00000+ 7 1.00000- 1                      127212102  671
                                                                  127212  0  672
                                                                  1272 0  0  673
 3.00700+ 3 6.95570+ 0          1          0          1          0127214 51  674
                                                                  127214  0  675
 3.00700+ 3 6.95570+ 0          1          0          3          0127214102  676
                                                                  127214  0  677
                                                                  1272 0  0  678
                                                                     0 0  0  679
 5.01000+ 3 9.92690+ 0          0          0          0         951273 1451    1
 0.00000+ 0 0.00000+ 0          0          0        211          01273 1451    2
  5-b - 10 lasl       eval-nov73 g.m.hale, r.a.nisley, p.g.young  1273 1451    3
                      dist-may74                                  1273 1451    4
                                                                  1273 1451    5
 b-10 free atom eval., nov. 1973, g.m.hale, r.a.nisley, p.g.young 1273 1451    6
                       los alamos scientific laboratory           1273 1451    7
                                                                  1273 1451    8
 mf=2 --------- resonance parameters ---------------------------- 1273 1451    9
                                                                  1273 1451   10
   mt=151  effective scattering radius = 0.40937e-12 cm           1273 1451   11
                                                                  1273 1451   12
                                                                  1273 1451   13
 mf=3 --------- smooth cross sections --------------------------- 1273 1451   14
                                                                  1273 1451   15
      the 2200 m/s cross sections are as follows,                 1273 1451   16
          mt=1    sigma = 3838.6   barns                          1273 1451   17
          mt=2    sigma = 2.1058   barns                          1273 1451   18
          mt=103  sigma = 0.000566 barns                          1273 1451   19
          mt=107  sigma = 3836.5   barns                          1273 1451   20
          mt=113  sigma = 0.000566 barns                          1273 1451   21
          mt=700  sigma = 0.000566 barns                          1273 1451   22
          mt=780  sigma = 240.51   barns                          1273 1451   23
          mt=781  sigma = 3596.0   barns                          1273 1451   24
                                                                  1273 1451   25
   mt=1        total cross section                                1273 1451   26
      0 to 1 mev, calculated from r-matrix parameters obtained by 1273 1451   27
          fitting simultaneously data from the reactions b10(n,n),1273 1451   28
          b10(n,alpha0), b10(n,alpha1), li7(alpha,alpha0), and    1273 1451   29
          li7(alpha,alpha1). total neutron cross section measure- 1273 1451   30
          ments included in the fit are those of di67. the        1273 1451   31
          li7+alpha data used in the fit are from cu67 and bi57.  1273 1451   32
      1 to 20 mev, smooth curve through measurements of di67,bo52,1273 1451   33
          ts62,fo61,co52, and co54, constrained to match          1273 1451   34
          r-matrix fit at 1 mev.                                  1273 1451   35
                                                                  1273 1451   36
   mt=2     elastic scattering cross section                      1273 1451   37
      0 to 1 mev, calculated from the r-matrix parameters         1273 1451   38
          described for mt=1. experimental elastic scattering data1273 1451   39
          included in the fit are those of as70 and la71.         1273 1451   40
      1 to 7 mev, smooth curve through measurements of la71, po70,1273 1451   41
          and ho69, constrained to be consistent with total and   1273 1451   42
          reaction cross section measurements.                    1273 1451   43
      7 to 14 mev, smooth curve through measurements of ho69,co69,1273 1451   44
          te62,va70, and va65.                                    1273 1451   45
      14 to 20 mev, optical model extrapolation from 14 mev data  1273 1451   46
                                                                  1273 1451   47
   mt=4     inelastic cross section                               1273 1451   48
      thres.to 20 mev, sum of mt=51-85                            1273 1451   49
                                                                  1273 1451   50
   mt=51-61 inelastic cross sections to discrete states           1273 1451   51
      mt=51 q=-0.717 mev   mt=55 q=-4.774 mev   mt=59 q=-5.923 mev1273 1451   52
         52   -1.740          56   -5.114          60   -6.029    1273 1451   53
         53   -2.154          57   -5.166          61   -6.133    1273 1451   54
         54   -3.585          58   -5.183                         1273 1451   55
      thres.to 20 mev, based on (n,nprime) measurements of po70,  1273 1451   56
          co69,ho69, and va70, and the (n,xgamma) measurements of 1273 1451   57
          da56,da60, and ne70 using a gamma-ray decay scheme      1273 1451   58
          deduced from la66,al66,se66a, and se66b. hauser-feshbach1273 1451   59
          calculations were used to estimate shapes and relative  1273 1451   60
          magnitudes where experimental data were lacking         1273 1451   61
                                                                  1273 1451   62
   mt=62-85 inelastic cross sections to groups of levels in       1273 1451   63
            0.5-mev wide bands centered about the q-values given  1273 1451   64
            below (used in lieu of mt=91 and file 5)              1273 1451   65
      mt=62 q=-6.5 mev     mt=70 q=-10.5 mev    mt=78 q=-14.5 mev 1273 1451   66
         63   -7.0            71   -11.0           79    15.0     1273 1451   67
         64   -7.5            72   -11.5           80    15.5     1273 1451   68
         65   -8.0            73   -12.0           81    16.0     1273 1451   69
         66   -8.5            74   -12.5           82    16.5     1273 1451   70
         67   -9.0            75   -13.0           83    17.0     1273 1451   71
         68   -9.5            76   -13.5           84    17.5     1273 1451   72
         69  -10.0            77   -14.0           85    18.0     1273 1451   73
      thres. to 20 mev, integrated cross section obtained by sub- 1273 1451   74
          tracting the sum of mt=2,51-61,103,104,107,and 113 from 1273 1451   75
          mt=1.  cross section distributed among the bands with   1273 1451   76
          an evaporation model using a nuclear temperature given  1273 1451   77
          by t=0.9728*sqrt(en) in mev,taken from ir67.            1273 1451   78
                                                                  1273 1451   79
   mt=103   (n,p) cross section                                   1273 1451   80
      thres.to 20 mev, sum of mt=700-703                          1273 1451   81
                                                                  1273 1451   82
   mt=104   (n,d) cross section                                   1273 1451   83
      thres. to 20 mev, based on be9(d,n)b11 measurements of si65 1273 1451   84
          and ba60, and the (n,d) measurement of va65.            1273 1451   85
                                                                  1273 1451   86
   mt=107   (n,alpha) cross section                               1273 1451   87
      0 to 20 mev, sum of mt=720,721.                             1273 1451   88
                                                                  1273 1451   89
   mt=113   (n,t2alpha) cross section                             1273 1451   90
      0 to 2.3 mev, based on a single-level fit to the resonance  1273 1451   91
          measured at 2 mev by da61, assuming l=0 incoming neu-   1273 1451   92
          trons and l=2 outgoing tritons.                         1273 1451   93
      2.3 to 20 mev, smooth curve through measurements of fr56    1273 1451   94
          and wy58, following general shape of da61 measurement   1273 1451   95
          from 4 to 9 mev.                                        1273 1451   96
                                                                  1273 1451   97
   mt=700-703   (n,p) cross section to discrete levels            1273 1451   98
      0 to 20 mev,  crudely estimated from the calculations       1273 1451   99
          of po70 and the (n,xgamma) measurements of ne70. cross  1273 1451  100
          section for mt=700 assumed identical to mt=113 below    1273 1451  101
          1 mev.  gamma-ray decay scheme for be-10 from la66.     1273 1451  102
                                                                  1273 1451  103
   mt=780     (n,alpha0) cross section                            1273 1451  104
      0 to 1 mev, calculated from the r-matrix parameters         1273 1451  105
          described for mt=1. experimental (n,alpha0) data input  1273 1451  106
          to the fit were those of ma68 and da61. in addition, the1273 1451  107
          angular distributions of va72 for the inverse reaction  1273 1451  108
          were included in the analysis.                          1273 1451  109
      1 to 20 mev, based on da61 measurements, with smooth extra- 1273 1451  110
          polation from 8 to 20 mev. da61 measurement above       1273 1451  111
          approximately 2 mev was renormalized by factor of 1.4.  1273 1451  112
                                                                  1273 1451  113
   mt=781     (n,alpha1) cross section                            1273 1451  114
      0 to 1 mev, calculated from the r-matrix parameters         1273 1451  115
          described for mt=1. experimental (n,alpha1) data in-    1273 1451  116
          cluded in the fit are those of fr72.                    1273 1451  117
      1 to 20 mev, smooth curve through measurements of da61 and  1273 1451  118
          ne70, with smooth extrapolation from 15 to 20 mev. the  1273 1451  119
          da61 data above approximately 2 mev were renormalized   1273 1451  120
          by a factor of 1.4.                                     1273 1451  121
                                                                  1273 1451  122
                                                                  1273 1451  123
 mf=4---------- neutron angular distributions ------------------- 1273 1451  124
                                                                  1273 1451  125
   mt=2   elastic angular distributions                           1273 1451  126
      0 to 1 mev, calculated from the r-matrix parameters         1273 1451  127
          described for mf=1,mt=1. experimental angular distri-   1273 1451  128
          butions input to the fit for both the elastic scatter-  1273 1451  129
          ing cross section and polarization were obtained from   1273 1451  130
          the measurements of la71. assignments for resonances    1273 1451  131
          above the neutron threshold are based on la71.          1273 1451  132
      1 to 14 mev, smoothed representation of legendre coeffi-    1273 1451  133
          cients derived from the measurements of la71, ha73,     1273 1451  134
          po70, ho69, co69, va69, and va65, constrained to match  1273 1451  135
          the r-matrix calculations at en=1 mev.                  1273 1451  136
      14 to 20 mev, optical model extrapolation of 14-mev data    1273 1451  137
                                                                  1273 1451  138
   mt=51-85  inelastic angular distributions                      1273 1451  139
      thres. to 20 mev, assumed isotropic in center of mass       1273 1451  140
                                                                  1273 1451  141
                                                                  1273 1451  142
 mf=12 -------- gamma ray multiplicities ------------------------ 1273 1451  143
                                                                  1273 1451  144
   mt=781  0.4776-mev photon from the (n,alpha1) reaction         1273 1451  145
      0 to 20 mev, multiplicity of 1.0 at all energies            1273 1451  146
                                                                  1273 1451  147
                                                                  1273 1451  148
 mf=13 -------- gamma-ray production cross sections ------------- 1273 1451  149
                                                                  1273 1451  150
   mt=4   (n,ngamma) cross section                                1273 1451  151
      thres. to 20 mev, obtained from mt=51-61 using b-10 decay   1273 1451  152
          scheme deduced from la66,al66,se66a, and se66b.         1273 1451  153
                                                                  1273 1451  154
   mt=103  (n,pgamma) cross sections                              1273 1451  155
      thres. to 20 mev, obtained from mt=701-703 using be-10      1273 1451  156
          decay scheme deduced from la66.                         1273 1451  157
                                                                  1273 1451  158
                                                                  1273 1451  159
 mf=14 -------- gamma ray angular distributions ----------------- 1273 1451  160
                                                                  1273 1451  161
   mt=4   (n,ngamma) angular distributions                        1273 1451  162
      thres. to 20 mev, assumed isotropic                         1273 1451  163
                                                                  1273 1451  164
   mt=103 (n,pgamma) angular distributions                        1273 1451  165
      thres. to 20 mev, assumed isotropic                         1273 1451  166
                                                                  1273 1451  167
   mt=781 (n,alpha1/gamma) angular distribution                   1273 1451  168
      0 to 20 mev, assumed isotropic                              1273 1451  169
                                                                  1273 1451  170
                                                                  1273 1451  171
 ----------------------- references ----------------------------- 1273 1451  172
                                                                  1273 1451  173
 al66   d.e. alburger et al.,phys.rev. 143,692 (1966)             1273 1451  174
 as70   a. asami and m.c. moxon, j.nucl.energy 24,85 (1970)       1273 1451  175
 ba60   r.bardes and g.e. owen, phys.rev.120,1369 (1960)          1273 1451  176
 be56   r.l. becker and h.h. barschall, phys.rev.102,1384 (1956)  1273 1451  177
 bi57   h.bichsel and t.w.bonner,phys.rev.108,1025 (1957)         1273 1451  178
 bo51   c.k.bockelman et al., phys.rev. 84,69 (1951)              1273 1451  179
 bo69   d.bogart and l.l.nichols, nucl.phys.a125,463 (1969)       1273 1451  180
 co52   j.h.coon et al., phys.rev. 88,562 (1952)                  1273 1451  181
 co54   c.f.cook and t.w. bonner,phys.rev. 94,651 (1954)          1273 1451  182
 co67   s.a. cox and f.r. pontet, j.nucl.energy 21,271 (1967)     1273 1451  183
 co69   j.a. cookson and j.g.locke,nucl.phys.a146,417(1970)       1273 1451  184
 co73   m.s. coates et al., priv. comm. to l.stewart (1973)       1273 1451  185
 cu65   r.y.cusson, thesis, calif. instit. tech. (1965)           1273 1451  186
 da56   r.b.day,phys.rev.102,767 (1956)                           1273 1451  187
 da60   r.b. day and m.walt,phys.rev.117,1330 (1960)              1273 1451  188
 da61   e.a. davis et al., nucl.phys.27,448 (1961)                1273 1451  189
 di67   k.m. diment, aere-r-5224 (1967)                           1273 1451  190
 fo61   d.m. fossan et al., phys.rev. 123,209 (1961)              1273 1451  191
 fr56   g.m. frye and j.h. gammel,phys.rev. 103,328 (1956)        1273 1451  192
 fr72   s.j. friesenhahn et al., gulf-rt-a12210 (1972)            1273 1451  193
 ha73   s.l.hausladen, thesis, ohio univ. coo-1717-5 (1973)       1273 1451  194
 ho69   j.c. hopkins, priv. comm. lasl (1969)                     1273 1451  195
 ir67   d.c.irving, ornl-tm-1872 (1967)                           1273 1451  196
 la66   t.lauritsen and f.ajzenberg-selove,nucl.phys.78,1(1966)   1273 1451  197
 la71   r.o. lane et al., phys.rev.c4,380 (1971)                  1273 1451  198
 ma68   r.l.macklin and j.h.gibbons,phys.rev.165,1147 (1968)      1273 1451  199
 mo66   f.p.mooring et al.,nucl.phys.82,16 (1966)                 1273 1451  200
 ne54   n.g.nereson,la-1655 (1954)                                1273 1451  201
 ne70   d.o.nellis et al., phys.rev. c1,847 (1970)                1273 1451  202
 po70   d.porter et al., awre o 45/70 (1970)                      1273 1451  203
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                                4          2        231           1273 1451  267
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                               12        781          4           1273 1451  303
                               13          4        368           1273 1451  304
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                                                                  1273 3  0 1899
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                                                                  1273 3  0 1935
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                                                                  1273 3  0 1964
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                                                                  1273 3  0 1993
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 6.80000+ 6 1.65500- 2 6.90000+ 6 1.66410- 2 7.00000+ 6 1.67520- 2127313103 3241
 7.10000+ 6 1.67930- 2 7.20000+ 6 1.70170- 2 7.30000+ 6 1.76190- 2127313103 3242
 7.40000+ 6 1.85980- 2 7.50000+ 6 1.97600- 2 7.60000+ 6 2.08490- 2127313103 3243
 7.80000+ 6 2.29780- 2 8.00000+ 6 2.47360- 2 8.20000+ 6 2.55430- 2127313103 3244
 8.40000+ 6 2.59420- 2 8.60000+ 6 2.61340- 2 8.80000+ 6 2.61920- 2127313103 3245
 9.00000+ 6 2.61700- 2 9.20000+ 6 2.60680- 2 9.40000+ 6 2.59130- 2127313103 3246
 9.60000+ 6 2.57220- 2 9.80000+ 6 2.55030- 2 1.00000+ 7 2.52470- 2127313103 3247
 1.05000+ 7 2.44260- 2 1.10000+ 7 2.35610- 2 1.15000+ 7 2.26790- 2127313103 3248
 1.20000+ 7 2.17940- 2 1.25000+ 7 2.09110- 2 1.30000+ 7 2.00280- 2127313103 3249
 1.35000+ 7 1.91450- 2 1.40000+ 7 1.82620- 2 1.45000+ 7 1.73790- 2127313103 3250
 1.50000+ 7 1.64960- 2 1.55000+ 7 1.56120- 2 1.60000+ 7 1.47290- 2127313103 3251
 1.65000+ 7 1.38460- 2 1.70000+ 7 1.29630- 2 1.75000+ 7 1.20800- 2127313103 3252
 1.80000+ 7 1.11970- 2 1.85000+ 7 1.03130- 2 1.90000+ 7 9.43030- 3127313103 3253
 1.95000+ 7 8.54720- 3 2.00000+ 7 7.66400- 3                      127313103 3254
 2.59300+ 6 5.95900+ 6          0          2          1         47127313103 3255
         47          2                                            127313103 3256
 6.30900+ 6 0.00000+ 0 6.40000+ 6 2.97140- 5 6.50000+ 6 6.23670- 5127313103 3257
 6.55000+ 6 7.86940- 5 6.60000+ 6 9.50220- 5 6.70000+ 6 1.27670- 4127313103 3258
 6.80000+ 6 1.86980- 4 6.90000+ 6 2.94880- 4 7.00000+ 6 4.32000- 4127313103 3259
 7.10000+ 6 4.91040- 4 7.20000+ 6 7.40160- 4 7.30000+ 6 1.37380- 3127313103 3260
 7.40000+ 6 2.39180- 3 7.50000+ 6 3.60000- 3 7.60000+ 6 4.76060- 3127313103 3261
 7.80000+ 6 7.05310- 3 8.00000+ 6 9.00000- 3 8.20000+ 6 9.99630- 3127313103 3262
 8.40000+ 6 1.05890- 2 8.60000+ 6 1.09700- 2 8.80000+ 6 1.12130- 2127313103 3263
 9.00000+ 6 1.13760- 2 9.20000+ 6 1.14580- 2 9.40000+ 6 1.14880- 2127313103 3264
 9.60000+ 6 1.14810- 2 9.80000+ 6 1.14470- 2 1.00000+ 7 1.13760- 2127313103 3265
 1.05000+ 7 1.10160- 2 1.10000+ 7 1.06130- 2 1.15000+ 7 1.01920- 2127313103 3266
 1.20000+ 7 9.76950- 3 1.25000+ 7 9.34830- 3 1.30000+ 7 8.92640- 3127313103 3267
 1.35000+ 7 8.50480- 3 1.40000+ 7 8.08320- 3 1.45000+ 7 7.66160- 3127313103 3268
 1.50000+ 7 7.24000- 3 1.55000+ 7 6.81840- 3 1.60000+ 7 6.39680- 3127313103 3269
 1.65000+ 7 5.97520- 3 1.70000+ 7 5.55360- 3 1.75000+ 7 5.13200- 3127313103 3270
 1.80000+ 7 4.71040- 3 1.85000+ 7 4.28880- 3 1.90000+ 7 3.86720- 3127313103 3271
 1.95000+ 7 3.44560- 3 2.00000+ 7 3.02400- 3                      127313103 3272
                                                                  127313  0 3273
                                                                  1273 0  0 3274
 5.01000+ 3 9.92690+ 0          1          0         13          0127314  4 3275
                                                                  127314  0 3276
 5.01000+ 3 9.92690+ 0          1          0          4          0127314103 3277
                                                                  127314  0 3278
 5.01000+ 3 9.92690+ 0          1          0          1          0127314781 3279
                                                                  127314  0 3280
                                                                  1273 0  0 3281
                                                                     0 0  0 3282
 4.00900+ 3 8.93480+ 0          0          0          6         411289 1451    1
 0.00000+ 0 0.00000+ 0          0          0        281          01289 1451    2
  4-be-  9  lll       eval-dec71 howerton, perkins                1289 1451    3
                      dist-may74  rev-nov74                       1289 1451    4
                                                                  1289 1451    5
 *********************   dna 4154 mod 2   *********************   1289 1451    6
                                                                  1289 1451    7
 the (n,2n) reaction was described using format modification 73-4 1289 1451    8
 which allows the representation of individual neutrons from      1289 1451    9
 sequential (n,2n) reactions. this was done utilizing mt=6-9 and  1289 1451   10
 46-49 in files 3 and 4, and mt=46-49 in file 5.                  1289 1451   11
 mt = 105 now includes (n,t0) in addition to (n,t1) data.         1289 1451   12
 the (n,t) reaction was split into (n,t0) and (n,t1) components   1289 1451   13
 using mt = 740 and 741.                                          1289 1451   14
                                                                  1289 1451   15
 **************************************************************   1289 1451   16
                                                                  1289 1451   17
                                                                  1289 1451   18
 **********************    dna 4154 mod 1     ******************  1289 1451   19
                                                                  1289 1451   20
        1. the energy range was extended down to 1.0e-05 ev.      1289 1451   21
                                                                  1289 1451   22
        2. gamma ray production for (n,g) and (n,t) are now       1289 1451   23
           represented as mt=102 and mt=105, respectivly,         1289 1451   24
           in files 12 and 15.  the photon spectrum from          1289 1451   25
           capture was assumed independent of incident neutron    1289 1451   26
           energy with the multiplicity varied with incident      1289 1451   27
           neutron energy to conserve energy.                     1289 1451   28
                                                                  1289 1451   29
      **********************************************************  1289 1451   30
                                                                  1289 1451   31
              be-9 evaluated neutron cross sections               1289 1451   32
                 for endf/b iv and dna library                    1289 1451   33
            evaluated by r.j.howerton and s.t.perkins             1289 1451   34
          lawrence livermore laboratory, livermore, ca.           1289 1451   35
                         september, 1973                          1289 1451   36
                                                                  1289 1451   37
                        general comments                          1289 1451   38
      the neutron energy range covered extends from .00001 ev to  1289 1451   39
 20 mev. in addition to elastic scattering which of course is     1289 1451   40
 everywhere energetically possible, the following reactions have  1289 1451   41
 thresholds (ucrl 50400, vol. 9) at energies less than 20 mev     1289 1451   42
              reaction               threshold (mev)              1289 1451   43
              n,2n                    1.85                        1289 1451   44
              n,p                    14.26                        1289 1451   45
              n,np                   18.76                        1289 1451   46
              n,d                    16.29                        1289 1451   47
              n,nd                   18.55                        1289 1451   48
              n,t                    11.60                        1289 1451   49
              n,nt                   19.65                        1289 1451   50
              n,alpha                 0.67                        1289 1451   51
              n,n alpha               2.74                        1289 1451   52
              n,gamma                exoergic                     1289 1451   53
      for the (n,np), (n,nd), and (n,nt) reactions, there are     1289 1451   54
 no measurements and since the thresholds are sufficiently        1289 1451   55
 high, these cross sections will be considered negligible. the    1289 1451   56
 (n,n alpha) reaction is in reality a decay mode for the (n,2n)   1289 1451   57
 reaction since he-5 is unstable, decaying immediately to a       1289 1451   58
 neutron and an alpha particle. additionally, the inelastic       1289 1451   59
 scattering reaction is also a decay mode for the (n,2n) reaction 1289 1451   60
 since the be-9* recoil nucleus always decays to the final end    1289 1451   61
 products of a neutron and two alpha particles. the way in which  1289 1451   62
 the cross sections are selected for elastic scattering, (n,2n),  1289 1451   63
 (n,p), (n,d), (n,t), (n, alpha), (n, gamma), as well as the      1289 1451   64
 (n,x gamma) reaction is discussed below.                         1289 1451   65
                                                                  1289 1451   66
                elastic scattering cross section                  1289 1451   67
      in keeping with the principle established for the entire    1289 1451   68
 lll evaluated cross section library, the free atom cross section 1289 1451   69
 is used for all energies below the usual upper limit of the      1289 1451   70
 molecular binding energy (about 10 ev). this is effectively only 1289 1451   71
 the nuclear part of the cross section of a stationary target at  1289 1451   72
 zero degrees kelvin. it is stroncly emphasized that the numbers  1289 1451   73
 are meaningless in the absence of a proper thermal treatment by  1289 1451   74
 either the processing code or the neutronics code which uses     1289 1451   75
 these numbers. they are likewise meaningless if the materials for1289 1451   76
 which they are to be used are bound in molecules unless molecular1289 1451   77
 binding is taken into account.                                   1289 1451   78
      the scattering cross section was taken equal to 6 barns     1289 1451   79
 from 0.00001 ev to 0.01 mev. from .01 mev to the                 1289 1451   80
 (n,alpha) threshold at 0.67 mev, the scattering cross section is 1289 1451   81
 equal to the total cross section since the (n,gamma) cross       1289 1451   82
 section is negligible.  the cross section was                    1289 1451   83
 based on data of refs. 63, 92, 720, 772 and 1002.                1289 1451   84
      above the (n,alpha) threshold, the scattering cross section 1289 1451   85
 was taken as the difference between the total and the nonelastic,1289 1451   86
  with the nonelastic being equal to the sum of its parts. up to 21289 1451   87
 mev, the total cross section was based on the previously         1289 1451   88
 mentioned data, as well as that from refs. 72, 336 and 1642.     1289 1451   89
 above this energy, we relied on the results of ref. 3088         1289 1451   90
 over the 2.7 mev resonance, and ref. 750 up to 15 mev. the       1289 1451   91
 extension to 20 mev utilized data from refs. 107, 673 and 682.   1289 1451   92
                                                                  1289 1451   93
              elastic scattering angular distributions,           1289 1451   94
             (normalized probabilities)                           1289 1451   95
      up to 7 mev, there are experimental differential scattering 1289 1451   96
 data in refs. 121, 151, 231, 296, 500, 571, 945, 1643, 1645, 16461289 1451   97
 and 1647. these results were used to determine the normalized    1289 1451   98
 probabilities. in be below the (n,2n) threshold, the total       1289 1451   99
 scattering data is equivalent to that for elastic scattering,    1289 1451  100
 since there is no inelastic scattering.  the change in           1289 1451  101
 shape of the angular distribution going through the scattering   1289 1451  102
 resonances was taken into account. at 14 mev, the probabilities  1289 1451  103
 were based on the results of ref. 402, 2585 and 3106. a smooth   1289 1451  104
 extrapolation was made to 20 mev.                                1289 1451  105
                                                                  1289 1451  106
                      (n,2n) cross section                        1289 1451  107
      the total (n,2n) cross section is based on the (n,2n)       1289 1451  108
 cross sections, and nonelastic minus absorption cross sections   1289 1451  109
 referenced in perkins (an-1443, 1965), as well as the new n,2n   1289 1451  110
 data given in ref. 763 and 3320 and the new nonelastic results of1289 1451  111
 ref. 2595 and 3321. the 20 mev point was based on interpolating  1289 1451  112
 nonelastic cross sections between the 14 mev value and the value 1289 1451  113
 at 25.5 mev quoted in ref. 356. the total (n,2n) cross section   1289 1451  114
 was then subdivided into 4 partial reactions which were described1289 1451  115
 by time-sequential decays, be-9(n,n1)be-9*(n2)be-8*.             1289 1451  116
 levels excited were at 1.68, 2.43, 6.76, and 11.28 mev in be-9*, 1289 1451  117
 and 0., 2.94, and 11.4 mev in be-8*. branching ratios were taken 1289 1451  118
 from perkins (an-1443,1965) with, however, the be-9* (9.1)       1289 1451  119
 transition being replaced by be-9* (11.28).                      1289 1451  120
                                                                  1289 1451  121
                   (n,2n) first neutron                           1289 1451  122
      for each of the partial (n,2n) reactions, the first         1289 1451  123
 neutron is described as an inelastic scattering event. the       1289 1451  124
 center of mass angular distribution of the (n,nprime)            1289 1451  125
 neutron from be-9*(2.43) was described by a p6 legendre          1289 1451  126
 expansion - data taken from perkins (an-1443,1965) and smoothly  1289 1451  127
 extrapolated to 20 mev. all other reactions were assumed         1289 1451  128
 isotropic in their center of mass systems.                       1289 1451  129
                                                                  1289 1451  130
                   (n,2n) second neutron                          1289 1451  131
      the description of the second neutron from each             1289 1451  132
 partial reaction neglects the energy-angle correction. this      1289 1451  133
 is a valid approximation for this reaction, as has been          1289 1451  134
 discussed previously (nse 31,156(1968)). the energy spectra      1289 1451  135
 are given by pi0(e to e2) with the lab system angular            1289 1451  136
 distributions described by a p9 expansion of the transference    1289 1451  137
 function. except for be-9* (2.43) and be-8*(0.), all levels were 1289 1451  138
 described by single level dispersion theory (widths taken        1289 1451  139
 from lap-117,1973 and lap-118,1973). all moments of the          1289 1451  140
 transference function were then integrated over the level        1289 1451  141
 distributions (equations in an-1443,1965). the integration       1289 1451  142
 scheme used bins of equal probability which has introduced       1289 1451  143
 some discontinuties into the output spectra, particularly        1289 1451  144
 at low incident neutron energies.                                1289 1451  145
                                                                  1289 1451  146
                       (n,p) cross section                        1289 1451  147
      this cross section was estimated from the known threshold   1289 1451  148
 value and the single measurement at 15.5 mev given in ref. 913.  1289 1451  149
                                                                  1289 1451  150
                       (n,d) cross section                        1289 1451  151
     this cross section is based in its entirety on the data      1289 1451  152
 between  16.5 and 18.8 mev reported in ref. 3101.                1289 1451  153
                                                                  1289 1451  154
                       (n,t) cross section                        1289 1451  155
      the cross section for the (n,t) reaction is based on a      1289 1451  156
 (n,t0) and a(n,t1) component, which proceed through the 0. and   1289 1451  157
 the 0.477 mev levels in li-7* respectively. the total (n,t)      1289 1451  158
 cross section near 14 mev was determined from ref. 496 and 650.  1289 1451  159
 the results of ref. 494 were neglected due to the large          1289 1451  160
 uncertanties.                                                    1289 1451  161
      the (n,t1) cross section was based on the work in ref. 605  1289 1451  162
 from 13.6 - 14.7 mev. above this energy, there is a resonance    1289 1451  163
 structure seen in the total cross section reported in ref. 107   1289 1451  164
 and 682. this was assumed to be due to the (n,t1) reaction and is1289 1451  165
 not in conflict with the rapid increase in the cross section     1289 1451  166
 above 14.5 mev seen by ref. 605.                                 1289 1451  167
                                                                  1289 1451  168
                     (n,alpha) cross section                      1289 1451  169
      the cross section was based on the measurements reported    1289 1451  170
 in ref. 160, 494 and 733 up to neutron energies of 8.6 mev. it   1289 1451  171
 was then tied into the three values given at 14 mev, refs. 86,   1289 1451  172
 650 and 2367, and then smoothly extrapolated to 20. mev. note    1289 1451  173
 that the  measured cross section is to he-6(0. mev) which beta   1289 1451  174
 decays to li-6, higher states in he-6 decay to alpha + 2n.       1289 1451  175
                                                                  1289 1451  176
                     (n,gamma) cross section                      1289 1451  177
     the cross section was assumed to be 1/v below 100 ev with    1289 1451  178
 a 2200 m/sec cross section of 9.5 mb. it was then extrapolated   1289 1451  179
 linearly on a log-log basis to 0.1 mb at 1 kev, and then held    1289 1451  180
 constant at this value up to 20 mev.                             1289 1451  181
                                                                  1289 1451  182
                   (n,x gamma) cross section                      1289 1451  183
      gamma rays in be-9 are produced by the (n,gamma) and the    1289 1451  184
 (n,t) reactions. at thermal energies, ref. 2415 quotes gamma ray 1289 1451  185
 energies of 0.8535, 2.59, 3.368, 3.444, 5.958 and 6.81 mev and   1289 1451  186
 the corresponding (n,x gamma) cross sections.                    1289 1451  187
 the photon spectrum from this work was used at all neutron       1289 1451  188
 energies. the multiplicity varied with neutron energy as         1289 1451  189
 m(e)=m(0)(ecm+q)/q.    m(0) is the multiplicity at thermal       1289 1451  190
 and q is the (n,gamma) q value. this combination of spectra      1289 1451  191
 and multiplicity conserves energy. there are no doubt other      1289 1451  192
 levels in be-10 with energies greater than 6.81 mev excited as   1289 1451  193
 the incident neutron energy is increased. the energies of the    1289 1451  194
 higher states have not yet been determined so we use this        1289 1451  195
 artifact to conserve energy. the component resulting from the    1289 1451  196
 (n,t) reaction is equal to the (n,t1) cross section since its    1289 1451  197
 multiplicity is unity.                                           1289 1451  198
                                                                  1289 1451  199
                           references                             1289 1451  200
     (reference numbers quoted here refer to data in the lll      1289 1451  201
 experimental neutron cross section library. see ucrl-50400, vol. 1289 1451  202
 2 and 3 for comments and indexes to the data).                   1289 1451  203
   63. phys. rev. 80, 1011 (1950) c.k. bockelman.                 1289 1451  204
   72. phys. rev. 84, 69 (1951) c.k. bockelman, d.w. miller,      1289 1451  205
       r.k. adair, h.h. barschall.                        r       1289 1451  206
   86. phys. rev. 89, 80 (1953) m.e. battat, f.l. ribe.           1289 1451  207
   92. private communication (1954) p.h. stelson.                 1289 1451  208
  107. phys. rev. 94, 651 (1954) c.f. cook, t.w. bonner.          1289 1451  209
  121. phys. rev. 98, 669 (1955) j.d. seagrave, r.l. henkel.      1289 1451  210
  151. phys. rev. 104, 1319 (1956) j.r. beyster, m. walt,         1289 1451  211
       e.w. salmi.                                                1289 1451  212
  160. phys. rev. 106, 1252 (1957) p.h. stelson, e.c. campbell.   1289 1451  213
  231. anl-5567 (1956) a. langsdorf, jr., r.o. lane, j.e. monahan,1289 1451  214
       see also, anl-5554 p. 22 (1956), phys. rev. 107, 1077      1289 1451  215
       (1957), anl-5567 (rev.) (1961).                            1289 1451  216
  296. phys. rev. 98, 677 (1955) m. walt, j.r. beyster.           1289 1451  217
  336. proc. phys. soc. (london) 64, 388 (1951) g.h. st afford.   1289 1451  218
  356. phys. rev. 111, 1155 (1958) m.h. macgregor, w.p. ball,     1289 1451  219
       r. booth.                                                  1289 1451  220
  402. phys. rev. 110, 1439 (1959) m.p. nakada, j.d. anderson,    1289 1451  221
       c.c. gardner, c. wong.                                     1289 1451  222
  494. doklady akad. nauk s.s.s.r. 119, 914 (1958) s.s. vasilev,  1289 1451  223
       v.v. kumarov, a.m. popova, see also, j. exptl. theoret.    1289 1451  224
       phys. (ussr) 33, 527 (1957).                               1289 1451  225
  496. phys. rev. 112, 1264 (1958) m.e. wyman, e.m. fryer,        1289 1451  226
       m.m. thorpe.                                               1289 1451  227
  500. phys. rev. 114, 1584 (1959) j.b. marion, j.s. levin,       1289 1451  228
       l. cranberg.                                               1289 1451  229
  571. anl-6172 (1960) r.o. lane, a.s. langsdorf, jr.,            1289 1451  230
       j.e. monahan, a.j. elwyn, see also, ann. phys. (n.y.) 12,  1289 1451  231
       135 (1961).                                                1289 1451  232
  605. ucrl-5596)(1959) j. benveniste, a.c. mitchell,             1289 1451  233
       c.d. schrader, j.h. zenger, see also, nuclear phys. 19, 52 1289 1451  234
       (1960).                                                    1289 1451  235
  650. j. exptl. theoret. phys. (ussr) 40, 1244 (1961)            1289 1451  236
       s.a. myachkova, v.p. perelygin.                            1289 1451  237
  673.  phys. rev. 120, 521 (1960) j.m. peterson, a. bratenahl,   1289 1451  238
       j.p. stoering.                                             1289 1451  239
  682. phys. rev. 123, 209 (1961) d.b. fossan, r.l. walter,       1289 1451  240
       w.e. wilson, h.h. barschall.                               1289 1451  241
  720. private communication (1962) e.g. bilpuch, j.a. farrell,   1289 1451  242
       g.c. kyker, jr., p.b. parks, h. newson.                    1289 1451  243
  733. nuclear ph ys. 23, 122 (1961) r. bass, t.w. bonner,        1289 1451  244
       h.p.haenni.                                                1289 1451  245
  750. private communication (1967) d.g. foster, jr.,             1289 1451  246
       d.w. glasgow, see also, hw-73116 (1962), hw-77311 (1963),  1289 1451  247
       phys. rev. c, 3, 576 (1971), phys. rev. c, 3, 604 (1971).  1289 1451  248
  763. nuclear phys. 129, 305 (1969) m. holmberg, j. hansen, see  1289 1451  249
       also, iaea conference on nuclear data, paris, paper        1289 1451  250
       cn-23/18 (1966).                                           1289 1451  251
  772. compt. rend. 255, 277 (1962) a. perrin, g. surget,         1289 1451  252
       c. thibault, f. verriere.                                  1289 1451  253
  913. phys. rev. 132, 328 (1963) d.e. albuger.                   1289 1451  254
  945. ornl-2610 p. 14 (1958) h.o. cohn, j.l. fowler, see also,   1289 1451  255
       bull. am. phys. soc. 3, 305 (1958).                        1289 1451  256
 1002. private communication (1954) c.t. hibdon, a. langsdorf.    1289 1451  257
 1642. bull. am. phys. soc. 4, 385 (1959) j.l. fowler, h.o. cohn. 1289 1451  258
 1643. doklady akad. nauk s.s.s.r. 158, 574 (1964) g.v. gorlov,   1289 1451  259
       n.s. lebedeva, v.m. morozov, see also, yad. fiz. 5, 910    1289 1451  260
       (1967).                                                    1289 1451  261
 1645. private communication (1960) j.s. levin, l. cranberg, see  1289 1451  262
       also, wash-1028 p. 26 (1960), wash-1029 p. 44 (1960).      1289 1451  263
 1646. private communication (1961) d.d. phillips.                1289 1451  264
 1647. phys. rev. 133, 409 (1964) r.o. lane, a.j. elwyn,          1289 1451  265
       a. langsdorf, jr.                                          1289 1451  266
 2367. nuclear phys. 96, 476 (1967) g. paic, d. rendic, p. tomas. 1289 1451  267
 2415. ga-10248 (dasa-2570) (1970) n.c. rasmussen, v.j. orphan,   1289 1451  268
       t.l. harper, j. cunningham, s.a. ali.                      1289 1451  269
 2585. private communication (1966) r. bouchez, see also, iaea    1289 1451  270
       conference on nuclear data, paris, paper cn-23/75 (1966).  1289 1451  271
 2595. conference on neutron cross section technology,            1289 1451  272
       washington d. c., vol. 1, p. 169 (1968) j.r.p. eaton,      1289 1451  273
       j. walke .                                                 1289 1451  274
 3088. conference on neutron cross section technology,            1289 1451  275
       washington d. c., p. 851 (1968) c.h. johnson, f.x. haas,   1289 1451  276
       j.l. fowler, f.d. martin, r.l. kernell, h.o. cohn.         1289 1451  277
 3101. z. naturforsch. 24, 289 (1969) w. scobel.                  1289 1451  278
 3106. np-17794 (1968) j. roturier, see also, compt. rend. 260,   1289 1451  279
       4491 (1965), bnl-400, 3rd ed. (1970).                      1289 1451  280
 3320. atomkernenergie 20,309 (1972) m. bloser                    1289 1451  281
 3321. univ. of birmingham dept. of phys. rept. 73-02 (1973)      1289 1451  282
       d.r. weaver, j. walker                                     1289 1451  283
                                1        451        324           1289 1451  284
                                2        151          4           1289 1451  285
                                3          1         84           1289 1451  286
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                                3        251         10           1289 1451  301
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                                3        740          5           1289 1451  304
                                3        741          6           1289 1451  305
                                4          2        176           1289 1451  306
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                                4         46        218           1289 1451  311
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                                5         46        383           1289 1451  315
                                5         47        396           1289 1451  316
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                               12        102          4           1289 1451  319
                               12        741          4           1289 1451  320
                               14        102          1           1289 1451  321
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                               15        102         22           1289 1451  323
                               15        741         12           1289 1451  324
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 3.78670+ 4 1.26520- 7 5.04890+ 4 1.46560- 7 6.38510+ 4 1.61230- 71289 5 49 2648
 8.73790+ 4 1.81600- 7 1.01310+ 5 1.91310- 7 1.30990+ 5 2.03590- 71289 5 49 2649
 2.67950+ 5 2.50130- 7 3.15550+ 5 2.61290- 7 3.49510+ 5 2.63840- 71289 5 49 2650
 4.01100+ 5 2.63240- 7 5.92460+ 5 2.65480- 7 8.17740+ 5 2.55390- 71289 5 49 2651
 9.77600+ 5 2.41750- 7 1.25950+ 6 2.10650- 7 1.74530+ 6 1.90540- 71289 5 49 2652
 2.05410+ 6 1.70290- 7 2.35330+ 6 1.60020- 7 2.77480+ 6 1.38910- 71289 5 49 2653
 3.05040+ 6 1.31370- 7 3.52520+ 6 1.14130- 7 4.30710+ 6 9.14860- 81289 5 49 2654
 4.74510+ 6 8.48100- 8 5.21730+ 6 7.24260- 8 6.27440+ 6 5.49860- 81289 5 49 2655
 6.57720+ 6 5.07970- 8 7.57930+ 6 3.34480- 8 8.31980+ 6 2.61960- 81289 5 49 2656
 9.28310+ 6 1.44470- 8 9.41830+ 6 1.33290- 8 1.01250+ 7 8.97650- 91289 5 49 2657
 1.11040+ 7 3.77850- 9 1.13680+ 7 2.41540- 9 1.15440+ 7 1.61280- 91289 5 49 2658
 1.16310+ 7 1.26750- 9 1.16920+ 7 1.05850- 9 1.17460+ 7 9.03500-101289 5 49 2659
 1.18050+ 7 7.68020-10 1.18850+ 7 6.29060-10 1.20370+ 7 4.52340-101289 5 49 2660
 1.25600+ 7 1.38900-10 1.27960+ 7 0.00000+ 0                      1289 5 49 2661
                                                                  1289 5  0 2662
                                                                  1289 0  0 2663
 4.00900+ 3 8.93480+ 0          1          0          1          0128912102 2664
 0.00000+ 0 0.00000+ 0          0          1          1          2128912102 2665
          2          2                                            128912102 2666
 1.00000- 5 1.60000+ 0 2.00000+ 7 5.82000+ 0                      128912102 2667
                                                                  128912  0 2668
 4.00900+ 3 8.93480+ 0          1          0          1          0128912741 2669
 0.00000+ 0 0.00000+ 0          0          1          1          2128912741 2670
          2          2                                            128912741 2671
 1.21300+ 7 1.00000+ 0 2.00000+ 7 1.00000+ 0                      128912741 2672
                                                                  128912  0 2673
                                                                  1289 0  0 2674
 4.00900+ 3 8.93480+ 0          1          0          1          0128914102 2675
                                                                  128914  0 2676
 4.00900+ 3 8.93480+ 0          1          0          1          0128914741 2677
                                                                  128914  0 2678
                                                                  1289 0  0 2679
 4.00900+ 3 8.93480+ 0          0          0          1          0128915102 2680
 0.00000+ 0 0.00000+ 0          0          1          1          2128915102 2681
          2          2                                            128915102 2682
 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      128915102 2683
 0.00000+ 0 0.00000+ 0          0          0          1          2128915102 2684
          2          2                                            128915102 2685
 0.00000+ 0 1.00000- 5          0          0          1         18128915102 2686
         18          2                                            128915102 2687
 8.52000+ 5 0.00000+ 0 8.53000+ 5 1.58480- 4 8.54000+ 5 0.00000+ 0128915102 2688
 2.58900+ 6 0.00000+ 0 2.59000+ 6 1.50400- 4 2.59100+ 6 0.00000+ 0128915102 2689
 3.36700+ 6 0.00000+ 0 3.36800+ 6 2.13800- 4 3.36900+ 6 0.00000+ 0128915102 2690
 3.44300+ 6 0.00000+ 0 3.44400+ 6 7.39590- 5 3.44500+ 6 0.00000+ 0128915102 2691
 5.95700+ 6 0.00000+ 0 5.95800+ 6 1.24300- 5 5.95900+ 6 0.00000+ 0128915102 2692
 6.80900+ 6 0.00000+ 0 6.81000+ 6 3.90930- 4 6.81100+ 6 0.00000+ 0128915102 2693
 0.00000+ 0 2.00000+ 7          0          0          1         18128915102 2694
         18          2                                            128915102 2695
 8.52000+ 5 0.00000+ 0 8.53000+ 5 1.58480- 4 8.54000+ 5 0.00000+ 0128915102 2696
 2.58900+ 6 0.00000+ 0 2.59000+ 6 1.50400- 4 2.59100+ 6 0.00000+ 0128915102 2697
 3.36700+ 6 0.00000+ 0 3.36800+ 6 2.13800- 4 3.36900+ 6 0.00000+ 0128915102 2698
 3.44300+ 6 0.00000+ 0 3.44400+ 6 7.39590- 5 3.44500+ 6 0.00000+ 0128915102 2699
 5.95700+ 6 0.00000+ 0 5.95800+ 6 1.24300- 5 5.95900+ 6 0.00000+ 0128915102 2700
 6.80900+ 6 0.00000+ 0 6.81000+ 6 3.90930- 4 6.81100+ 6 0.00000+ 0128915102 2701
                                                                  128915  0 2702
 4.00900+ 3 8.93480+ 0          0          0          1          0128915741 2703
 0.00000+ 0 0.00000+ 0          0          1          1          2128915741 2704
          2          2                                            128915741 2705
 1.21300+ 7 1.00000+ 0 2.00000+ 7 1.00000+ 0                      128915741 2706
 0.00000+ 0 0.00000+ 0          0          0          1          2128915741 2707
          2          2                                            128915741 2708
 0.00000+ 0 1.21300+ 7          0          0          1          3128915741 2709
          3          2                                            128915741 2710
 4.76000+ 5 0.00000+ 0 4.77000+ 5 1.00000- 3 4.78000+ 5 0.00000+ 0128915741 2711
 0.00000+ 0 2.00000+ 7          0          0          1          3128915741 2712
          3          2                                            128915741 2713
 4.76000+ 5 0.00000+ 0 4.77000+ 5 1.00000- 3 4.78000+ 5 0.00000+ 0128915741 2714
                                                                  128915  0 2715
                                                                  1289 0  0 2716
                                                                     0 0  0 2717
 5.41350+ 4 1.33748+ 2          0          0          0         161294 1451    1
 0.00000+ 0 0.00000+ 0          0          0         52          01294 1451    2
 54-xe-135 bnw        eval-jun67 b.r.leonard,jr. and k.b.stewart  1294 1451    3
 pri.com.june,1967    dist-may74 rev-may75                        1294 1451    4
 *         *          *          *         *          *         * 1294 1451    5
 endf/b version-iv modifications=                  (apr74)        1294 1451    6
 file extended from 1.0 kev to 20.0 mev by f.schmittroth and      1294 1451    7
 r.e. schenter (hedl)                                             1294 1451    8
 radioactive decay data evaluated by c.w.reich (anc) added.       1294 1451    9
 added same angular distribution (mf=4,mt=2) as for               1294 1451   10
 cs-133 (mat=1141).                                               1294 1451   11
 *          *         *          *         *          *         * 1294 1451   12
 data modified june,1970 to conform to endf/b-ii formats          1294 1451   13
 *         *          *          *         *          *         * 1294 1451   14
 xenon-135 entry by b.r.leonard,jr. and k.b.stewart ref.1         1294 1451   15
           june 1967                                              1294 1451   16
*          *          *          *          *          *          1294 1451   17
     xe 135  evaluation updated for energies from  1  kev to      1294 1451   18
     20  mev.                                                     1294 1451   19
     f. schmittroth and r.e. schenter                             1294 1451   20
     westinghouse hanford company  (february 1974)                1294 1451   21
         mt=1  total cross section was obtained from moldauers    1294 1451   22
               optical potential,ref.6.                           1294 1451   23
         mt=2  elastic cross section was obtained by subtracting  1294 1451   24
               the inelastic and capture cross sections from      1294 1451   25
               total.                                             1294 1451   26
         mt=4,51,91   inelastic cross sections were obtained      1294 1451   27
               from the compound nucleus code comnuc,ref.7.       1294 1451   28
         mt=102   neutron capture obtained from the code ncap,    1294 1451   29
               ref.8.                                             1294 1451   30
*          *          *          *          *          *          1294 1451   31
 mf=1                     general information                     1294 1451   32
   mt=451 atomic mass = 134.907 ref.2                             1294 1451   33
   mt=457    q- 1973 revision of wapstra-gove mass tables         1294 1451   34
             half-life  n.e.holden, chart of the nuclides (1973)  1294 1451   35
                        and private communication (sept.,1973)    1294 1451   36
             other- m.j.martin,!radioactive atoms-supplement 1!,  1294 1451   37
                    ornl-4923  (1973).                            1294 1451   38
 mf=3                     smooth cross sections                   1294 1451   39
   mt=1   the resonance parameters of sumner(ref.4) have been     1294 1451   40
   mt=2    accepted as the best estimate of the cross section.    1294 1451   41
   mt=102  these parameters have been used in the program         1294 1451   42
           unicorn(ref.5) to calculate point values at 0 deg.k    1294 1451   43
           from 0.0001 ev to 1 kev .the calculations give         1294 1451   44
           sigma capture = 2.636e+06 barns at 0.0253 ev.          1294 1451   45
q-value ref.j.mattauch et al.nuc.phys 67(1965)no.1                1294 1451   46
                          references                              1294 1451   47
  1. leonard,b.r.,stewart,k.b.,pnl june 1967                      1294 1451   48
  2. everling,f.,et.al.,nucl.phys.18,529(1960).                   1294 1451   49
  4. sumner,h.m.,aeew-r-116(june 1962).                           1294 1451   50
  5. otter,j.m.,naa-sr.11980,vol.6(june 1966).                    1294 1451   51
  6. p.a.moldauer,phys.rev.,vol.135(1964)b642.                    1294 1451   52
  7. c.dunford, comnuc-3,private comm. to a.prince.               1294 1451   53
  8. f.schmittroth,hedl-tme-71-106,august 1971.                   1294 1451   54
                                1        451         70           1294 1451   55
                                1        457         24           1294 1451   56
                                2        151          4           1294 1451   57
                                3          1        130           1294 1451   58
                                3          2        130           1294 1451   59
                                3          4          8           1294 1451   60
                                3         51          8           1294 1451   61
                                3         91          8           1294 1451   62
                                3        102        130           1294 1451   63
                                3        251         14           1294 1451   64
                                3        252         14           1294 1451   65
                                3        253         14           1294 1451   66
                                4          2        206           1294 1451   67
                                4         51         10           1294 1451   68
                                4         91         10           1294 1451   69
                                5         91          7           1294 1451   70
                                                                  1294 1  0   71
 5.41350+ 4 1.33748+ 2          0          0          0          21294 1457   72
 3.30120+ 4 3.60000+ 1          0          0          4          21294 1457   73
 3.09890+ 5 0.00000+ 0 2.61430+ 5 0.00000+ 0                      1294 1457   74
 5.41350+ 4 1.33748+ 2          0          0          6          11294 1457   75
 1.00000+ 0 0.00000+ 0 1.15800+ 6 9.00000+ 3 1.00000+ 0 0.00000+ 01294 1457   76
 1.00000+ 0 0.00000+ 0          0          0         36          51294 1457   77
 1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01294 1457   78
 9.50000+ 4 9.00000+ 3 8.20000- 2 7.00000- 3 0.00000+ 0 0.00000+ 01294 1457   79
 1.76000+ 5 9.00000+ 3 5.60000- 2 1.00000- 2 0.00000+ 0 0.00000+ 01294 1457   80
 5.49000+ 5 9.00000+ 3 2.80000+ 0 2.00000- 1 0.00000+ 0 0.00000+ 01294 1457   81
 7.50000+ 5 9.00000+ 3 5.00000- 1 1.00000- 2 0.00000+ 0 0.00000+ 01294 1457   82
 9.08000+ 5 9.00000+ 3 9.66000+ 1 2.00000- 1 0.00000+ 0 0.00000+ 01294 1457   83
 0.00000+ 0 0.00000+ 0          0          0         66         101294 1457   84
 1.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 0 0.00000+ 01294 1457   85
 1.58200+ 5 2.00000+ 2 2.30000- 1 2.00000- 2 0.00000+ 0 0.00000+ 01294 1457   86
 1.99900+ 5 7.00000+ 2 2.00000- 2 0.00000+ 0 0.00000+ 0 0.00000+ 01294 1457   87
 2.49741+ 5 1.00000+ 1 9.06000+ 1 5.00000- 1 7.10000- 2 5.00000- 31294 1457   88
 3.58300+ 5 3.00000+ 2 2.00000- 1 2.00000- 2 0.00000+ 0 0.00000+ 01294 1457   89
 3.73100+ 5 1.00000+ 3 1.10000- 2 0.00000+ 0 0.00000+ 0 0.00000+ 01294 1457   90
 4.07900+ 5 3.00000+ 2 3.20000- 1 2.00000- 2 0.00000+ 0 0.00000+ 01294 1457   91
 6.08070+ 5 4.00000+ 1 2.58000+ 0 1.40000- 1 0.00000+ 0 0.00000+ 01294 1457   92
 6.54600+ 5 4.00000+ 2 3.20000- 2 4.00000- 3 0.00000+ 0 0.00000+ 01294 1457   93
 7.31900+ 5 4.00000+ 2 4.50000- 2 5.00000- 3 0.00000+ 0 0.00000+ 01294 1457   94
 8.21600+ 5 4.00000+ 2 5.00000- 2 6.00000- 3 0.00000+ 0 0.00000+ 01294 1457   95
                                                                  1294 1  0   96
                                                                  1294 0  0   97
 5.41350+ 4 1.33748+ 2          0          0          1          01294 2151   98
 5.41350+ 4 1.00000+ 0          0          0          1          01294 2151   99
 1.00000- 5 1.00000+ 5          0          0          0          01294 2151  100
 1.50000+ 0 7.46000- 1          0          0          0          01294 2151  101
                                                                  1294 2  0  102
                                                                  1294 0  0  103
 5.41350+ 4 1.33748+ 2          0          0          0          01294 3  1  104
 0.00000+ 0 0.00000+ 0          0          0          2        3811294 3  1  105
        346          5        381          3                      1294 3  1  106
 1.00000- 5 8.69987+ 7 2.00000- 5 6.21985+ 7 5.00000- 5 3.94983+ 71294 3  1  107
 1.00000- 4 2.83388+ 7 1.20000- 4 2.58877+ 7 1.40000- 4 2.39833+ 71294 3  1  108
 1.60000- 4 2.24487+ 7 1.80000- 4 2.11781+ 7 2.00000- 4 2.01034+ 71294 3  1  109
 2.20000- 4 1.91793+ 7 2.40000- 4 1.83736+ 7 2.60000- 4 1.76630+ 71294 3  1  110
 2.80000- 4 1.70301+ 7 3.00000- 4 1.64619+ 7 3.20000- 4 1.59480+ 71294 3  1  111
 3.40000- 4 1.54803+ 7 3.60000- 4 1.50523+ 7 3.80000- 4 1.46587+ 71294 3  1  112
 4.00000- 4 1.42951+ 7 4.20000- 4 1.39580+ 7 4.40000- 4 1.36441+ 71294 3  1  113
 4.60000- 4 1.33511+ 7 4.80000- 4 1.30768+ 7 5.00000- 4 1.28191+ 71294 3  1  114
 5.20000- 4 1.25766+ 7 5.40000- 4 1.23477+ 7 5.60000- 4 1.21313+ 71294 3  1  115
 5.80000- 4 1.19263+ 7 6.00000- 4 1.17316+ 7 6.20000- 4 1.15466+ 71294 3  1  116
 6.40000- 4 1.13703+ 7 6.60000- 4 1.12022+ 7 6.80000- 4 1.10416+ 71294 3  1  117
 7.00000- 4 1.08880+ 7 7.20000- 4 1.07409+ 7 7.40000- 4 1.05998+ 71294 3  1  118
 7.60000- 4 1.04645+ 7 7.80000- 4 1.03344+ 7 8.00000- 4 1.02093+ 71294 3  1  119
 8.20000- 4 1.00888+ 7 8.40000- 4 9.97265+ 6 8.60000- 4 9.86066+ 61294 3  1  120
 8.80000- 4 9.75256+ 6 9.00000- 4 9.64811+ 6 9.20000- 4 9.54712+ 61294 3  1  121
 9.40000- 4 9.44942+ 6 9.60000- 4 9.35482+ 6 9.80000- 4 9.26317+ 61294 3  1  122
 1.00000- 3 9.17432+ 6 1.20000- 3 8.41331+ 6 1.40000- 3 7.82420+ 61294 3  1  123
 1.60000- 3 7.35123+ 6 1.80000- 3 6.96105+ 6 2.00000- 3 6.63235+ 61294 3  1  124
 2.20000- 3 6.35074+ 6 2.40000- 3 6.10615+ 6 2.60000- 3 5.89132+ 61294 3  1  125
 2.80000- 3 5.70077+ 6 3.00000- 3 5.53038+ 6 3.20000- 3 5.37694+ 61294 3  1  126
 3.40000- 3 5.23788+ 6 3.60000- 3 5.11118+ 6 3.80000- 3 4.99519+ 61294 3  1  127
 4.00000- 3 4.88853+ 6 4.20000- 3 4.79008+ 6 4.40000- 3 4.69889+ 61294 3  1  128
 4.60000- 3 4.61414+ 6 4.80000- 3 4.53517+ 6 4.97152- 3 4.47159+ 61294 3  1  129
 5.00000- 3 4.46137+ 6 5.20000- 3 4.39227+ 6 5.40000- 3 4.32738+ 61294 3  1  130
 5.60000- 3 4.26635+ 6 5.80000- 3 4.20884+ 6 6.00000- 3 4.15454+ 61294 3  1  131
 6.20000- 3 4.10320+ 6 6.40000- 3 4.05457+ 6 6.60000- 3 4.00845+ 61294 3  1  132
 6.80000- 3 3.96465+ 6 7.00000- 3 3.92301+ 6 7.20000- 3 3.88338+ 61294 3  1  133
 7.40000- 3 3.84562+ 6 7.60000- 3 3.80958+ 6 7.80000- 3 3.77520+ 61294 3  1  134
 8.00000- 3 3.74232+ 6 8.20000- 3 3.71088+ 6 8.40000- 3 3.68079+ 61294 3  1  135
 8.60000- 3 3.65196+ 6 8.80000- 3 3.62433+ 6 8.84437- 3 3.61836+ 61294 3  1  136
 9.00000- 3 3.59782+ 6 9.20000- 3 3.57238+ 6 9.40000- 3 3.54795+ 61294 3  1  137
 9.60000- 3 3.52447+ 6 9.80000- 3 3.50190+ 6 1.00000- 2 3.48019+ 61294 3  1  138
 1.19269- 2 3.30777+ 6 1.20000- 2 3.30233+ 6 1.40000- 2 3.17746+ 61294 3  1  139
 1.44454- 2 3.15499+ 6 1.60000- 2 3.08859+ 6 1.65719- 2 3.06828+ 61294 3  1  140
 1.80000- 2 3.02562+ 6 1.84699- 2 3.01383+ 6 2.00000- 2 2.98206+ 61294 3  1  141
 2.13627- 2 2.96125+ 6 2.20000- 2 2.95362+ 6 2.24695- 2 2.94879+ 61294 3  1  142
 2.33065- 2 2.94171+ 6 2.40000- 2 2.93724+ 6 2.40214- 2 2.93712+ 61294 3  1  143
 2.46745- 2 2.93403+ 6 2.53000- 2 2.93198+ 6 2.59255- 2 2.93078+ 61294 3  1  144
 2.60000- 2 2.93069+ 6 2.65786- 2 2.93038+ 6 2.72935- 2 2.93089+ 61294 3  1  145
 2.80000- 2 2.93229+ 6 2.81305- 2 2.93265+ 6 2.92373- 2 2.93680+ 61294 3  1  146
 2.99948- 2 2.94072+ 6 3.00000- 2 2.94076+ 6 3.20000- 2 2.95502+ 61294 3  1  147
 3.40000- 2 2.97420+ 6 3.60000- 2 2.99755+ 6 3.80000- 2 3.02441+ 61294 3  1  148
 3.87383- 2 3.03508+ 6 4.00000- 2 3.05415+ 6 4.20000- 2 3.08620+ 61294 3  1  149
 4.40000- 2 3.12000+ 6 4.60000- 2 3.15499+ 6 4.80000- 2 3.19061+ 61294 3  1  150
 5.00000- 2 3.22629+ 6 5.15119- 2 3.25297+ 6 5.20000- 2 3.26147+ 61294 3  1  151
 5.40000- 2 3.29554+ 6 5.60000- 2 3.32791+ 6 5.80000- 2 3.35796+ 61294 3  1  152
 6.00000- 2 3.38508+ 6 6.11720- 2 3.39937+ 6 6.20000- 2 3.40868+ 61294 3  1  153
 6.40000- 2 3.42816+ 6 6.60000- 2 3.44295+ 6 6.80000- 2 3.45255+ 61294 3  1  154
 6.94231- 2 3.45596+ 6 7.00000- 2 3.45649+ 6 7.20000- 2 3.45436+ 61294 3  1  155
 7.40000- 2 3.44582+ 6 7.60000- 2 3.43067+ 6 7.69610- 2 3.42099+ 61294 3  1  156
 7.80000- 2 3.40876+ 6 8.00000- 2 3.38004+ 6 8.20000- 2 3.34459+ 61294 3  1  157
 8.40000- 2 3.30259+ 6 8.41800- 2 3.29849+ 6 8.60000- 2 3.25431+ 61294 3  1  158
 8.80000- 2 3.20010+ 6 9.00000- 2 3.14040+ 6 9.13989- 2 3.09566+ 61294 3  1  159
 9.20000- 2 3.07574+ 6 9.40000- 2 3.00665+ 6 9.60000- 2 2.93373+ 61294 3  1  160
 9.80000- 2 2.85761+ 6 9.89369- 2 2.82101+ 6 1.00000- 1 2.77888+ 61294 3  1  161
 1.07188- 1 2.48360+ 6 1.16848- 1 2.08840+ 6 1.20000- 1 1.96621+ 61294 3  1  162
 1.29622- 1 1.62555+ 6 1.40000- 1 1.31923+ 6 1.60000- 1 8.92161+ 51294 3  1  163
 1.63009- 1 8.43201+ 5 1.80000- 1 6.21996+ 5 1.84915- 1 5.72275+ 51294 3  1  164
 2.00000- 1 4.48918+ 5 2.09458- 1 3.89208+ 5 2.20000- 1 3.34643+ 51294 3  1  165
 2.38525- 1 2.61475+ 5 2.40000- 1 2.56632+ 5 2.60000- 1 2.01660+ 51294 3  1  166
 2.74102- 1 1.72317+ 5 2.80000- 1 1.61803+ 5 3.00000- 1 1.32167+ 51294 3  1  167
 3.18800- 1 1.10831+ 5 3.20000- 1 1.09639+ 5 3.40000- 1 9.21786+ 41294 3  1  168
 3.60000- 1 7.84132+ 4 3.76327- 1 6.92467+ 4 3.80000- 1 6.73959+ 41294 3  1  169
 4.00000- 1 5.84592+ 4 4.20000- 1 5.11227+ 4 4.40000- 1 4.50349+ 41294 3  1  170
 4.52174- 1 4.18265+ 4 4.60000- 1 3.99343+ 4 4.80000- 1 3.56233+ 41294 3  1  171
 5.00000- 1 3.19502+ 4 5.20000- 1 2.87982+ 4 5.40000- 1 2.60749+ 41294 3  1  172
 5.54770- 1 2.42960+ 4 5.60000- 1 2.37079+ 4 5.80000- 1 2.16387+ 41294 3  1  173
 6.00000- 1 1.98206+ 4 6.20000- 1 1.82152+ 4 6.40000- 1 1.67914+ 41294 3  1  174
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 7.00000- 1 1.33714+ 4 7.20000- 1 1.24549+ 4 7.40000- 1 1.16269+ 41294 3  1  176
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          2          2                                            1294 5 91  802
 5.30940+ 5 1.00000+ 0 2.00000+ 7 1.00000+ 0                      1294 5 91  803
 0.00000+ 0 0.00000+ 0          0          0          1          21294 5 91  804
          2          2                                            1294 5 91  805
 5.30940+ 5 6.00000+ 5 2.00000+ 7 6.00000+ 5                      1294 5 91  806
 0.00000+ 0 0.00000+ 0          0          0          0          01294 5  0  807
 0.00000+ 0 0.00000+ 0          0          0          0          01294 0  0  808
                                                                     0 0  0  809
 9.02320+ 4 2.30040+ 2          1          1          0         441296 1451    1
 0.00000+ 0 0.00000+ 0          0          1        103          01296 1451    2
 90-th-232 b+w        eval-nov66 wittkopf, roy, and livolsi       1296 1451    3
 baw-317 (1970)       dist-may74  rev-nov74                       1296 1451    4
          *          *          *          *          *          *1296 1451    5
 file modified for endf/b version-iv   o.ozer (bnl)  apr74       *1296 1451    6
         1)included yield data from fiss. prod. task force(jan74) 1296 1451    7
            revised nov-74                                        1296 1451    8
         2)included rad. decay data from c.w.reich-anc    (feb74) 1296 1451    9
         3)included delayed neut. yields from s.a.cox-anl (dec73) 1296 1451   10
         4)added prompt neut. yields by calculating mt=452-455    1296 1451   11
         5)extended cross section data to 20 mev by using lll     1296 1451   12
           ratios (15mev/20 mev)                                  1296 1451   13
         6)extended mf=4,mt=2 data by repeating the 15 mev dist.  1296 1451   14
           at 20 mev.                                             1296 1451   15
         7)extended mf=5 and remaining mf=4 data by extrapolation 1296 1451   16
           (csewg recommendation dec73)                           1296 1451   17
          *          *          *          *          *          *1296 1451   18
          mf=1,mt=454                                             1296 1451   19
  fission product yield data for endf/b-iv 1/74.      recommended 1296 1451   20
  values are given from the yields subcommittees of the decay heat1296 1451   21
  task force. members of the subcommittees include w.walker(ch),  1296 1451   22
  p.aline,n.dudey,r.larsen,w.maeck,w.mcelroy,b.rider,t.england(ch)1296 1451   23
  a.wahl and k.wolfsberg. final direct yields were generated by b.1296 1451   24
  rider as described in nedo-12154 rev.1 jan.74. endf/b file prep.1296 1451   25
  was made by r.schenter 1/74. peak chain yields are given as     1296 1451   26
     elab=5.00e+05 ev     a-ychain(percent)=                      1296 1451   27
   832.04, 843.72, 853.82, 866.09, 876.48, 886.85, 897.83, 907.96,1296 1451   28
   917.10, 927.18, 937.75, 946.08, 955.53, 964.89, 974.12, 984.00,1296 1451   29
   993.02,1322.66,1333.66,1344.87,1354.85,1365.12,1377.02,1386.91,1296 1451   30
  1396.73,1407.91,1417.65,1426.64,1436.99,1448.22,1455.67,1464.85,1296 1451   31
  1473.27,1482.11                                                 1296 1451   32
          *          *          *          *          *          *1296 1451   33
          mf=1,mt=455                                             1296 1451   34
 delayed neutron data evaluation by s.a.cox (anl) (to be publ.)   1296 1451   35
          *          *          *          *          *          *1296 1451   36
          mf=1,mt=456                                             1296 1451   37
 prompt neutron data generated by subtracting delayed yields from 1296 1451   38
 total.                                                           1296 1451   39
          *          *          *          *          *          *1296 1451   40
          mf=1,mt=457                                             1296 1451   41
 radioactive decay data prepared by c.w.reich (anc)  jan74        1296 1451   42
 references  q(alpha)- 1973 revision of wapstra-gove mass table   1296 1451   43
             half-life-n.e. holden, chart of the nuclides (1973)  1296 1451   44
                        and private communication (jan.,1974)     1296 1451   45
             other- m.r. schmorak, nuclear data b 4,no.6,561(1966)1296 1451   46
  note  1. )e-alpha  = 4068. kev.                                 1296 1451   47
            this value includes, in addition to the kinetic energy1296 1451   48
            of the alpha particle, the recoil energy of the       1296 1451   49
            daughter nucleus.                                     1296 1451   50
        2. the internal-conversion coefficients are theoretical   1296 1451   51
           values.the gamma-ray intensities are derived from these1296 1451   52
           values, with the requirement that the total transition 1296 1451   53
           intensity agree with that given by the alpha-particle  1296 1451   54
           branching data.                                        1296 1451   55
 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *1296 1451   56
                                                                  1296 1451   57
  thorium-232       (b and w)    wittcopf, roy, and livolsi       1296 1451   58
          *          *          *          *          *           1296 1451   59
           data compiled nov., 1966 and modified may, 1969        1296 1451   60
           evaluation described in babcock and wilcox report,     1296 1451   61
           baw-317                                                1296 1451   62
          *          *          *          *          *           1296 1451   63
 energy range (0.00001 to 10 ev.                                  1296 1451   64
    total x/s according to memo from b.r. leonard to csewg on aug.1296 1451   65
    8, 1969.  a value of 10.15 b for the potential x/s was provid 1296 1451   66
    ed as the best fit to the experimentally measured data.       1296 1451   67
    the 2200 m/sec capture cross section was  7.40 b, of which    1296 1451   68
    6.96 b is due to a neg. energy level, 0.245 is due to the     1296 1451   69
    positive energy levels, and 0.195 is 1/v contributions.       1296 1451   70
    elastic scattering x/s derived as the difference between      1296 1451   71
    the total and the capture x/s.                                1296 1451   72
 energy range (0.01 to 50.0 kev)                                  1296 1451   73
    bnl-325, 2nd ed. proveded the recommended values for all      1296 1451   74
    resolved resonances up to 3.006 kev. the last group of        1296 1451   75
    resonances up to 3.931 kev were obtained from the measurement 1296 1451   76
    made by grag, et al., phys. rev.134,895(1964). all resolved   1296 1451   77
    resonances were taken as s-wave.                              1296 1451   78
    the range from 3.931 to 50 kev is covered by the unresolved   1296 1451   79
    resonance region and the parameters are desribed in baw-317.  1296 1451   80
    a background cross section is given in file 3 for the         1296 1451   81
    capture x/s to account for missed p-wave resonances  in the   1296 1451   82
    resolved resonance region.                                    1296 1451   83
 energy range (0.05 to 15 mev)                                    1296 1451   84
    the total x/s was taken from the data given in bnl-325,       1296 1451   85
    2nd ed. the elastic x/s was obtained as the difference        1296 1451   86
    between the total and all non-elastic cross sections.         1296 1451   87
    the radiative capture x/s was taken from the data given in    1296 1451   88
    bnl-325, 2nd ed.  the fission x/s was taken from an evaluation1296 1451   89
    made by davey, n.s.e., 26,149(1966) up to 10 mev and from     1296 1451   90
    bnl-325, 2nd ed. up to 15 mev.                                1296 1451   91
    the number of neutrons per fission is in agreement with h.    1296 1451   92
    conde and m. holmberg, iaea conf.(1965) vol.2. p61.           1296 1451   93
    for secondary energy distribution  of fission neutrons, the   1296 1451   94
    temperature is in agreement with the work by e.barnard et al. 1296 1451   95
    nuc. phys. 71,228(1965).                                      1296 1451   96
    inelastic           threshold set at 50 kev as from a.b.smith 1296 1451   97
    phys.rev. 126,718(1962). all other discrete levels were       1296 1451   98
    obtained from work of n.p.glaskov, at. energy. 14,400(1963),  1296 1451   99
    r. batchelor et al. nuc. phys. 65,236(1965), and s.o. moore,  1296 1451  100
    bnl-818 (1963).                                               1296 1451  101
    the (n,2n) x/s was obtained as an unweighted average through  1296 1451  102
    several experimental data sets published between 1964 and 19561296 1451  103
    the (n,3n) x/s was obtined from the work of m.h.taggart and   1296 1451  104
    h. goodfellow, jne 17,437(1963).                              1296 1451  105
                                1        451        149           1296 1451  106
                                1        452          3           1296 1451  107
                                1        454        551           1296 1451  108
                                1        455          7           1296 1451  109
                                1        456          5           1296 1451  110
                                1        457         14           1296 1451  111
                                2        151        241           1296 1451  112
                                3          1        132           1296 1451  113
                                3          2        114           1296 1451  114
                                3          4         24           1296 1451  115
                                3         16          8           1296 1451  116
                                3         17          5           1296 1451  117
                                3         18         14           1296 1451  118
                                3         51         18           1296 1451  119
                                3         52         16           1296 1451  120
                                3         53         14           1296 1451  121
                                3         54         12           1296 1451  122
                                3         55         10           1296 1451  123
                                3         56         10           1296 1451  124
                                3         57          8           1296 1451  125
                                3         58          9           1296 1451  126
                                3         91         14           1296 1451  127
                                3        102        115           1296 1451  128
                                3        251          8           1296 1451  129
                                3        252          8           1296 1451  130
                                3        253          8           1296 1451  131
                                4          2        193           1296 1451  132
                                4         16         10           1296 1451  133
                                4         17         10           1296 1451  134
                                4         18         10           1296 1451  135
                                4         51         10           1296 1451  136
                                4         52         10           1296 1451  137
                                4         53         10           1296 1451  138
                                4         54         10           1296 1451  139
                                4         55         10           1296 1451  140
                                4         56         10           1296 1451  141
                                4         57         10           1296 1451  142
                                4         58         10           1296 1451  143
                                4         91         10           1296 1451  144
                                5         16          8           1296 1451  145
                                5         17          8           1296 1451  146
                                5         18          7           1296 1451  147
                                5         91         13           1296 1451  148
                                5        455        107           1296 1451  149
                                                                  1296 1  0  150
 9.02320+ 4 2.30040+ 2          0          1          0          01296 1452  151
 0.00000+ 0 0.00000+ 0          0          0          2          01296 1452  152
 1.85400+ 0 1.56000- 7                                            1296 1452  153
                                                                  1296 1  0  154
 9.02320+04 2.30040+ 2          1          0          0          01296 1454  155
 5.00000+05 0.                  0          0       3291       10971296 1454  156
 2.40660+04 0.         9.99888-11 2.40670+04 0.         3.36962-111296 1454  157
 2.40680+04 0.         3.90956-12 2.40700+04 0.         1.73981-141296 1454  158
 2.50660+04 0.         3.27963-09 2.50670+04 0.         3.36962-091296 1454  159
 2.50680+04 0.         1.22986-09 2.50690+04 0.         3.44961-101296 1454  160
 2.50700+04 0.         5.80935-11 2.50710+04 0.         7.47916-121296 1454  161
 2.60660+04 0.         1.55983-08 2.60670+04 0.         4.35951-081296 1454  162
 2.60680+04 0.         4.53949-08 2.60690+04 0.         3.79957-081296 1454  163
 2.60700+04 0.         1.97978-08 2.60710+04 0.         8.12909-091296 1454  164
 2.60720+04 0.         2.74969-09 2.60730+04 0.         2.90967-101296 1454  165
 2.60740+04 0.         2.16976-11 2.60760+04 0.         5.92934-141296 1454  166
 2.70660+04 0.         3.00966-09 2.70670+04 0.         2.21975-081296 1454  167
 2.70680+04 0.         6.01933-08 2.70690+04 0.         1.33985-071296 1454  168
 2.70700+04 0.         1.93978-07 2.70710+04 0.         2.30974-071296 1454  169
 2.70720+04 0.         2.36973-07 2.70730+04 0.         7.88912-081296 1454  170
 2.70740+04 0.         1.89979-08 2.70750+04 0.         4.20953-091296 1454  171
 2.70760+04 0.         5.64937-10 2.80660+04 0.         8.35906-111296 1454  172
 2.80670+04 0.         1.80980-09 2.80680+04 0.         1.37985-081296 1454  173
 2.80690+04 0.         8.19908-08 2.80700+04 0.         3.07966-071296 1454  174
 2.80710+04 0.         9.70891-07 2.80720+04 0.         2.68970-061296 1454  175
 2.80730+04 0.         2.53972-06 2.80740+04 0.         1.80980-061296 1454  176
 2.80750+04 0.         1.23986-06 2.80760+04 0.         5.27941-071296 1454  177
 2.80770+04 0.         1.01989-07 2.80780+04 0.         2.03977-081296 1454  178
 2.80800+04 0.         8.73902-11 2.80820+04 0.         5.96933-141296 1454  179
 2.90660+04 0.         5.96933-14 2.90670+04 0.         4.13954-121296 1454  180
 2.90680+04 0.         4.91945-11 2.90680+04 1.00000+00 4.54949-111296 1454  181
 2.90690+04 0.         1.76980-09 2.90700+04 0.         9.60892-091296 1454  182
 2.90700+04 1.00000+00 9.60892-09 2.90710+04 0.         1.64982-071296 1454  183
 2.90720+04 0.         1.19987-06 2.90730+04 0.         2.96967-061296 1454  184
 2.90740+04 0.         5.60937-06 2.90750+04 0.         1.06188-051296 1454  185
 2.90760+04 0.         1.30785-05 2.90770+04 0.         7.81912-061296 1454  186
 2.90780+04 0.         5.21942-06 2.90790+04 0.         1.32985-061296 1454  187
 2.90800+04 0.         2.66970-07 2.90810+04 0.         2.56971-081296 1454  188
 2.90820+04 0.         2.21975-09 3.00660+04 0.         0.        1296 1454  189
 3.00670+04 0.         0.         3.00680+04 0.         7.48916-141296 1454  190
 3.00690+04 0.         2.17976-12 3.00690+04 1.00000+00 2.04977-121296 1454  191
 3.00700+04 0.         1.49983-10 3.00710+04 0.         1.98978-091296 1454  192
 3.00710+04 1.00000+00 1.80980-09 3.00720+04 0.         8.62903-081296 1454  193
 3.00730+04 0.         6.03932-07 3.00740+04 0.         3.01966-061296 1454  194
 3.00750+04 0.         1.49483-05 3.00760+04 0.         4.81146-051296 1454  195
 3.00770+04 0.         8.00110-05 3.00780+04 0.         1.58962-041296 1454  196
 3.00790+04 0.         1.34495-04 3.00800+04 0.         8.31407-051296 1454  197
 3.00810+04 0.         2.71470-05 3.00820+04 0.         7.86912-061296 1454  198
 3.00830+04 0.         8.62903-07 3.00840+04 0.         5.64937-081296 1454  199
 3.00860+04 0.         1.97978-11 3.10660+04 0.         0.        1296 1454  200
 3.10670+04 0.         0.         3.10680+04 0.         0.        1296 1454  201
 3.10690+04 0.         0.         3.10700+04 0.         2.81968-141296 1454  202
 3.10710+04 0.         2.43973-12 3.10720+04 0.         1.69981-101296 1454  203
 3.10730+04 0.         3.69959-09 3.10740+04 0.         5.67936-081296 1454  204
 3.10750+04 0.         8.14909-07 3.10760+04 0.         7.24919-061296 1454  205
 3.10770+04 0.         3.32463-05 3.10780+04 0.         1.76760-041296 1454  206
 3.10790+04 0.         4.39721-04 3.10800+04 0.         7.51026-041296 1454  207
 3.10810+04 0.         7.51486-04 3.10820+04 0.         6.80564-041296 1454  208
 3.10830+04 0.         2.48902-04 3.10840+04 0.         5.58038-051296 1454  209
 3.10860+04 0.         2.48972-07 3.20660+04 0.         0.        1296 1454  210
 3.20670+04 0.         0.         3.20680+04 0.         0.        1296 1454  211
 3.20690+04 0.         0.         3.20700+04 0.         0.        1296 1454  212
 3.20710+04 0.         0.         3.20720+04 0.         3.35962-141296 1454  213
 3.20730+04 0.         1.46984-12 3.20730+04 1.00000+00 1.39984-121296 1454  214
 3.20740+04 0.         1.20986-10 3.20750+04 0.         2.75969-091296 1454  215
 3.20750+04 1.00000+00 2.75969-09 3.20760+04 0.         1.51983-071296 1454  216
 3.20770+04 0.         6.25930-06 3.20770+04 1.00000+00 1.03988-061296 1454  217
 3.20780+04 0.         3.37462-05 3.20790+04 0.         2.49812-041296 1454  218
 3.20800+04 0.         1.10776-03 3.20810+04 0.         3.06556-031296 1454  219
 3.20820+04 0.         7.71056-03 3.20830+04 0.         8.44921-031296 1454  220
 3.20840+04 0.         5.96277-03 3.20850+04 0.         1.42733-031296 1454  221
 3.20860+04 0.         3.04956-04 3.20870+04 0.         2.84168-051296 1454  222
 3.20880+04 0.         1.45984-06 3.30690+04 0.         0.        1296 1454  223
 3.30710+04 0.         0.         3.30720+04 0.         0.        1296 1454  224
 3.30730+04 0.         0.         3.30740+04 0.         0.        1296 1454  225
 3.30740+04 1.00000+00 0.         3.30750+04 0.         8.87901-131296 1454  226
 3.30760+04 0.         8.01910-11 3.30770+04 0.         3.64959-091296 1454  227
 3.30780+04 0.         1.96978-07 3.30790+04 0.         4.94945-061296 1454  228
 3.30800+04 0.         6.38729-05 3.30810+04 0.         5.09273-041296 1454  229
 3.30820+04 0.         1.73615-03 3.30820+04 1.00000+00 1.73603-031296 1454  230
 3.30830+04 0.         1.03266-02 3.30840+04 0.         2.05148-021296 1454  231
 3.30850+04 0.         1.43089-02 3.30860+04 0.         9.71051-031296 1454  232
 3.30870+04 0.         3.01035-03 3.30880+04 0.         5.50758-041296 1454  233
 3.30890+04 0.         6.86623-05 3.40720+04 0.         0.        1296 1454  234
 3.40730+04 0.         0.         3.40730+04 1.00000+00 0.        1296 1454  235
 3.40740+04 0.         0.         3.40750+04 0.         0.        1296 1454  236
 3.40760+04 0.         0.         3.40770+04 0.         9.01899-131296 1454  237
 3.40770+04 1.00000+00 3.36962-13 3.40780+04 0.         1.20986-101296 1454  238
 3.40790+04 0.         5.57938-09 3.40790+04 1.00000+00 5.57938-091296 1454  239
 3.40800+04 0.         4.57949-07 3.40810+04 0.         5.96933-061296 1454  240
 3.40810+04 1.00000+00 5.21942-06 3.40820+04 0.         2.46912-041296 1454  241
 3.40830+04 0.         1.10251-03 3.40830+04 1.00000+00 1.09543-031296 1454  242
 3.40840+04 0.         1.22479-02 3.40850+04 0.         1.16121-021296 1454  243
 3.40850+04 1.00000+00 1.17334-02 3.40860+04 0.         4.50358-021296 1454  244
 3.40870+04 0.         4.10375-02 3.40880+04 0.         2.39430-021296 1454  245
 3.40890+04 0.         9.49188-03 3.40900+04 0.         2.01241-031296 1454  246
 3.40910+04 0.         2.55201-04 3.40920+04 0.         2.17376-051296 1454  247
 3.40940+04 0.         3.28963-08 3.40950+04 0.         2.54297-101296 1454  248
 3.40960+04 0.         5.99933-12 3.50750+04 0.         0.        1296 1454  249
 3.50770+04 0.         0.         3.50770+04 1.00000+00 0.        1296 1454  250
 3.50780+04 0.         0.         3.50790+04 0.         2.87968-131296 1454  251
 3.50790+04 1.00000+00 2.73969-13 3.50800+04 0.         4.05955-111296 1454  252
 3.50800+04 1.00000+00 3.91956-11 3.50810+04 0.         7.11920-091296 1454  253
 3.50820+04 0.         4.90945-07 3.50820+04 1.00000+00 2.44973-071296 1454  254
 3.50830+04 0.         1.44184-05 3.50840+04 0.         1.28246-041296 1454  255
 3.50840+04 1.00000+00 1.28246-04 3.50850+04 0.         1.47241-031296 1454  256
 3.50860+04 0.         4.23746-03 3.50860+04 1.00000+00 4.23821-031296 1454  257
 3.50870+04 0.         2.19494-02 3.50880+04 0.         3.68425-021296 1454  258
 3.50890+04 0.         4.11372-02 3.50900+04 0.         2.50882-021296 1454  259
 3.50910+04 0.         9.62189-03 3.50920+04 0.         2.58795-031296 1454  260
 3.50930+04 0.         5.17522-04 3.50940+04 0.         4.40751-051296 1454  261
 3.50950+04 0.         1.92187-06 3.50960+04 0.         9.37895-081296 1454  262
 3.60770+04 0.         0.         3.60780+04 0.         0.        1296 1454  263
 3.60790+04 0.         0.         3.60790+04 1.00000+00 0.        1296 1454  264
 3.60800+04 0.         0.         3.60810+04 0.         2.17976-131296 1454  265
 3.60810+04 1.00000+00 2.04977-13 3.60820+04 0.         9.67892-111296 1454  266
 3.60830+04 0.         4.72947-09 3.60830+04 1.00000+00 4.72947-091296 1454  267
 3.60840+04 0.         6.14931-07 3.60850+04 0.         6.01933-061296 1454  268
 3.60850+04 1.00000+00 6.02933-06 3.60860+04 0.         2.28644-041296 1454  269
 3.60870+04 0.         1.88202-03 3.60880+04 0.         9.81612-031296 1454  270
 3.60890+04 0.         3.27619-02 3.60900+04 0.         5.13208-021296 1454  271
 3.60910+04 0.         5.20417-02 3.60920+04 0.         3.92033-021296 1454  272
 3.60930+04 0.         2.37809-02 3.60940+04 0.         6.27189-031296 1454  273
 3.60950+04 0.         1.20007-03 3.60960+04 0.         1.42014-041296 1454  274
 3.60970+04 0.         1.31285-05 3.60980+04 0.         6.97922-071296 1454  275
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                                                                  1296 5  0 2021
                                                                  1296 0  0 2022
                                                                     0 0  0 2023
                                                                    -1 0  0    1