3-Li-  6   ENDF/B-VI, Processed by Red Cullen using PREPRO2004  6000 0  0    0
 3.00600E+3 5.96340E+0          0          0          0          2 325 1451    1
 0.0        0.0                 0          0          0          6 325 1451    2
 1.00000E+0 2.00000E+7          1          0         10          6 325 1451    3
 0.0        0.0                 1          0        330         79 325 1451    4
  3-LI - 6 LANL       EVAL-APR89 G.M.HALE, P.G.YOUNG               325 1451    5
                      DIST-SEP91 REV1-JUL91            19910806    325 1451    6
----ENDF/B-VI         MATERIAL  325         REVISION 1             325 1451    7
-----INCIDENT NEUTRON DATA                                         325 1451    8
------ENDF-6 FORMAT                                                325 1451    9
                                                                   325 1451   10
 ***************************************************************** 325 1451   11
 ***************************************************************** 325 1451   12
                                                                   325 1451   13
                  MOD1 OF ENDF/B-VI                                325 1451   14
                                                                   325 1451   15
     The following revisions were made for MOD1 of ENDF/B-VI:      325 1451   16
                                                                   325 1451   17
 1. MF=1,MT=451 - Comments were added regarding estimated          325 1451   18
    (expanded) covariance for the Standards Cross Sections.        325 1451   19
 2. MF=3,MT=53 - LF flag and Q-value corrected.                    325 1451   20
                                                                   325 1451   21
 ***************************************************************** 325 1451   22
****************************************************************** 325 1451   23
                                                                   325 1451   24
                        ENDF/VI EVALUATION                         325 1451   25
                     G. M. Hale and P. G. Young                    325 1451   26
                                                                   325 1451   27
 MAJOR CHANGES FROM VERSION V OF ENDF/B ARE:                       325 1451   28
                                                                   325 1451   29
   1. Inclusion of the ENDF/B-VI standard (n,t) cross section      325 1451   30
      from the simultaneous standards analysis (ca85) over the     325 1451   31
      energy range thermal to 1 MeV.                               325 1451   32
   2. Replacement of all major cross sections and elastic angular  325 1451   33
      distributions at energies between 10^-5 eV and 3 MeV with    325 1451   34
      results from the R-matrix analysis performed in conjunction  325 1451   35
      with the simultaneous standards analysis.                    325 1451   36
   3. Revision of the elastic cross sections and angular distri-   325 1451   37
      butions at energies between 3 and 20 MeV to match recent     325 1451   38
      experimental data, resulting in a general decrease of the    325 1451   39
      elastic cross section in this energy range.                  325 1451   40
   4. Revision of the (n,n')d cross sections to account for        325 1451   41
      recent measurements, resulting in a general increase in      325 1451   42
      the total (n,n')d cross section that tends to offset the     325 1451   43
      decrease in the elastic cross section and maintain about     325 1451   44
      the same total cross section as before.                      325 1451   45
                                                                   325 1451   46
                                                                   325 1451   47
****************************************************************** 325 1451   48
                                                                   325 1451   49
                        STANDARDS COVARIANCES                      325 1451   50
                                                                   325 1451   51
 Phase 1 reviewers of the ENDF/B-VI standards cross sections have  325 1451   52
 expressed the concern that the uncertainties resulting from the   325 1451   53
 combination of R-matrix and simultaneous evaluations might have   325 1451   54
 led to uncertainties that are too small.  As a result, the        325 1451   55
 Standards Subcommittee produced (at the May, 1990 CSEWG meeting)  325 1451   56
 a set of expanded covariance estimates for the standard cross     325 1451   57
 section reactions.  These uncertainties are estimates such that   325 1451   58
 if a modern day experiment were performed on a given standard     325 1451   59
 cross section using the best techniques, approximately 2/3 of     325 1451   60
 the results should fall within these expanded uncertainties. The  325 1451   61
 expanded uncertainties for the Li-6(n,t) cross section are given  325 1451   62
 in the following table and are compared to values from the        325 1451   63
 combined output of the standards covariance analysis:             325 1451   64
                                                                   325 1451   65
    Energy Range    Estimated Uncertainty    Combined Analysis     325 1451   66
      (keV)              (percent)               (percent)         325 1451   67
                                                                   325 1451   68
 1.0E-08 - 0.1               0.3                     0.14          325 1451   69
     0.1 - 1.0               0.5                                   325 1451   70
     1.0 - 10.               0.7                     0.14          325 1451   71
     10. - 50.               0.9                                   325 1451   72
     50. - 90.               1.1                     0.25          325 1451   73
     90. - 150               1.5                                   325 1451   74
     150 - 450               2.0                     0.29          325 1451   75
     450 - 650               5.0                                   325 1451   76
     650 - 800               2.0                     0.36          325 1451   77
     800 - 1000              5.0                                   325 1451   78
                                                                   325 1451   79
 ****************************************************************  325 1451   80
                                                                   325 1451   81
                                                                   325 1451   82
 mf=2 --------- resonance parameters ----------------------------  325 1451   83
                                                                   325 1451   84
   mt=151  effective scattering radius = 2.31175e-13 cm.           325 1451   85
                                                                   325 1451   86
 mf=3 --------- smooth cross sections ---------------------------  325 1451   87
                                                                   325 1451   88
      the 2200 m/s cross sections are as follows:                  325 1451   89
          mt=1     sigma = 941.6928  barns                         325 1451   90
          mt=2     sigma = 0.67157   barns                         325 1451   91
          mt=102   sigma = 0.03850   barns                         325 1451   92
          mt=105   sigma = 940.9827  barns                         325 1451   93
                                                                   325 1451   94
   mt=1        total cross section                                 325 1451   95
       below 3 mev, the values are taken from an r-matrix          325 1451   96
          analysis by hale, dodder, and witte (ha84) which takes   325 1451   97
          into account data from all reactions possible in 7li     325 1451   98
          up to 4 mev neutron energy. total cross section data     325 1451   99
          considered in this analysis were those of ha75 and sm77. 325 1451  100
          between 3 and 20 mev, the total was taken to be the      325 1451  101
          sum of mt=2,4,24,102,103, and 105, which generally       325 1451  102
          follows the measurements of sm82, ke79, kn77, go72,      325 1451  103
          and fo71.                                                325 1451  104
   mt=2        elastic cross section                               325 1451  105
       below 3 mev, the values are taken from the r-matrix         325 1451  106
          analysis cited for mt=1, which includes the elastic      325 1451  107
          measurements of sm82 and la61. above 3 mev, the curve    325 1451  108
          is a smooth representation of the data of kn79 and ba63  325 1451  109
          up to 7.5 mev, and of that of ho79 between 7.5 and 13    325 1451  110
          mev.  the curve passes through the average of several    325 1451  111
          measurements at 14 mev, and is extrapolated to 20 mev    325 1451  112
          using the shape of an optical model calculation.         325 1451  113
   mt=4        total inelastic cross section                       325 1451  114
       sum of mt=51 through mt=81.                                 325 1451  115
   mt=24       (n,2n)alpha cross section                           325 1451  116
       passes through the point of mather and paine (ma69) at      325 1451  117
       14 mev, taking into account the measurements of as63.       325 1451  118
   mt=51,52,54-56,58-81  (n,n')d continuum                         325 1451  119
       represented by continuum-level contributions in 6li,        325 1451  120
          binned in .5-mev intervals.  The energy-angle spectra    325 1451  121
          are determined by a 3-body phase-space calculation,      325 1451  122
          assuming isotropic center-of mass distributions.  at     325 1451  123
          each energy, the sum of the continuum-level              325 1451  124
          contributions is normalized to an assumed energy-angle   325 1451  125
          integrated continuum cross section which approximates    325 1451  126
          the difference of the nonelastic sigma and the           325 1451  127
          contribution from the first and second levels in 6li.    325 1451  128
          the steep rise of the pseudo-level cross sections from   325 1451  129
          their thresholds and the use of fixed bin widths over    325 1451  130
          finite angles produces anomolous structure in the        325 1451  131
          individual cross sections which is especially apparent   325 1451  132
          near the thresholds.  some effort has been made to       325 1451  133
          smooth out these effects, but they remain to some        325 1451  134
          extent.                                                  325 1451  135
   mt=53        (n,n1)d discrete level cross section               325 1451  136
       has p-wave penetrability energy dependence from threshold   325 1451  137
          to 3.2 mev.  matched at higher energies to a curve       325 1451  138
          through fitted legendre coefficients from experimental   325 1451  139
          data of sa82, ho79, sm80, ho68, ba63.                    325 1451  140
   mt=57        (n,n2)gamma cross section                          325 1451  141
       is based on the available experimental data, especially     325 1451  142
          that of ho79, li80, sm82, ho68.                          325 1451  143
          gradually to 20 mev.  smooth curve drawn through data    325 1451  144
          of pr69 and be75.                                        325 1451  145
   mt=102       (n,gamma) cross section                            325 1451  146
       unchanged from version v, which was based on the thermal    325 1451  147
          measurement of jurney (ju73) and the pendlebury          325 1451  148
          evaluation (pe64) at higher energies.                    325 1451  149
   mt=103        (n,p) cross section                               325 1451  150
       threshold to 9 mev, based on the data of ba65.extended to   325 1451  151
          20 mev through the 14 mev data of fr54 and ba53.         325 1451  152
   mt=105        (n,t) cross section                               325 1451  153
       below 3 mev, values are taken from the r-matrix analysis,   325 1451  154
          which includes (n,t) measurements from re78, la78, br77, 325 1451  155
          ov74, and ba75.  between 3 and 5 mev, the values are     325 1451  156
          based on ba75, and at higher energies are taken from the 325 1451  157
          evaluation of pe64, extended to 20 mev considering the   325 1451  158
          data of ke58.                                            325 1451  159
                                                                   325 1451  160
                                                                   325 1451  161
 mf = 4-------------------angular distributions------------------- 325 1451  162
                                                                   325 1451  163
   mt=2          elastic cross section                             325 1451  164
       legendre coefficients determined as follows:                325 1451  165
          below 4 mev, coefficients up to l=6 were taken from      325 1451  166
          the r-matrix analysis , which included the measurements  325 1451  167
          la61 and sm 82.  above 4 mev, the coefficients represent 325 1451  168
          fits to the measurements of ho68, ho79, kn79, sm82,      325 1451  169
          de73, ba63, ab70, and hy68.  most emphasis was placed    325 1451  170
          on the data of ho79, kn79, sm82.  extrapolation of the   325 1451  171
          coefficients to 20 mev was aided by optical model        325 1451  172
          calculations.                                            325 1451  173
   mt=24        (n,2n) cross section                               325 1451  174
       lab distributions obtained by integrating over energy the   325 1451  175
          4-body phase-space spectra that result from transforming 325 1451  176
          isotropic center-of-mass distributions to the laboratory 325 1451  177
          system.                                                  325 1451  178
   mt=51-81     (n,n')d cross sections                             325 1451  179
       excitation energy binned data is assumed isotropic in the   325 1451  180
          center of mass reference system.  mt = 53 and 57         325 1451  181
          are real levels.  mt = 57 is assumed to be isotropic     325 1451  182
          in the two-body reference system.  mt = 53 is given as   325 1451  183
          anisotropic, based on fits of legendre expansions to     325 1451  184
          the experimental data of ab70, ba63, ho68, ho79, me65,   325 1451  185
          hy68, wo62, sa82.                                        325 1451  186
   mt=105       (n,t).cross section        (to be added)           325 1451  187
       legendre coefficients obtained from the r-matrix analysis   325 1451  188
          are supplied at energies below 4 mev.  the analysis      325 1451  189
          takes into account (n,t) angular distribution            325 1451  190
          measurements from kn83, co82, dr82, br77, ba75, and      325 1451  191
          ov74.                                                    325 1451  192
                                                                   325 1451  193
                                                                   325 1451  194
 mf = 5---------secondary energy distributions-------------------- 325 1451  195
                                                                   325 1451  196
   mt=24        (n,2n)                                             325 1451  197
       lab distributions obtained by integrating over angle the 4- 325 1451  198
          body phase-space spectra that result from transforming   325 1451  199
          isotropic center-of-mass distributions to the laboratory 325 1451  200
          system.                                                  325 1451  201
                                                                   325 1451  202
                                                                   325 1451  203
 mf = 12--------gamma-ray multiplicities-------------------------- 325 1451  204
                                                                   325 1451  205
   mt=57        (n,n2) gamma                                       325 1451  206
       energy taken from aj74.  multiplicity assumed to be one.    325 1451  207
   mt=102       (n,gamma)                                          325 1451  208
       energies and transition arrays for radiative capture taken  325 1451  209
          from ju73, as reported in aj74.  the lp flag was used to 325 1451  210
          describe the mt=102 photons.                             325 1451  211
                                                                   325 1451  212
                                                                   325 1451  213
 mf = 14--------gamma-ray angular distributions------------------- 325 1451  214
                                                                   325 1451  215
   mt=57        (n,n2)gamma                                        325 1451  216
       the gamma is assumed isotropic.                             325 1451  217
   mt=102       (n,gamma)                                          325 1451  218
      .the two high-energy gammas are assumed isotropic. data on   325 1451  219
          the 477 kev gamma indicate isotropy.                     325 1451  220
                                                                   325 1451  221
                                                                   325 1451  222
 mf=33----------cross section covariances------------------------- 325 1451  223
                   (to be added later)                             325 1451  224
                                                                   325 1451  225
  the relative covariances for mt=1,2, and 105 below 4 mev are     325 1451  226
  given in file 33. they are based on calculations using the co-   325 1451  227
  variances of the r-matrix parameters in first-order error        325 1451  228
  propogation.                                                     325 1451  229
   mt=1         total                                              325 1451  230
       relative covariances entered as nc-type sub-subsection,     325 1451  231
          implying that they are to be constructed from those for  325 1451  232
          mt=2 and 105.  they are not intended for use at energies 325 1451  233
          above 4 mev.                                             325 1451  234
   mt=2,105     elastic and (n,t)                                  325 1451  235
       relative covariances among these two cross sections are     325 1451  236
          entered explicitly as ni-type sub-subsections in the     325 1451  237
          lb=5 (direct) representation at energies below 4 mev.    325 1451  238
          although values for the 3.95-4.05 mev bin are repeated   325 1451  239
          in a 4-20 mev bin, the covariances are not intended for  325 1451  240
          use at energies above 4 mev.                             325 1451  241
                                                                   325 1451  242
                                                                   325 1451  243
--------------------- references --------------------------------  325 1451  244
                                                                   325 1451  245
ab70  U.Abbondanno, Nuo.Cim. A166,139(1970).                       325 1451  246
aj74  f.ajzenberg-selove and t.lauritsen, nucl. phys. a227,55      325 1451  247
      (1974).                                                      325 1451  248
ar64  a.h.armstrong, j.gammel, l.rosen, and g.m.frye, nucl. phys.  325 1451  249
      52,505 (1964).                                               325 1451  250
as63  v.j.ashby et al, phys. rev. 129,1771 (1963).                 325 1451  251
ba53  m.e.battat and f.l.ribe, phys.rev. 89,80 (1953).             325 1451  252
ba63  r.batchelor and j.h.towle, nucl. phys. 47,385 (1963).        325 1451  253
ba65  r.bass, c.bindhardt, and k.kruger, eandc(e)-57u (1965).      325 1451  254
ba75  c.m.bartle, proc. conf. on nuclear cross sections and        325 1451  255
      technology, vol.2,688 (1975),  and private communication     325 1451  256
      (1976).  see also nucl. phys. a330, 1 (1979).                325 1451  257
be75  besotosnyj et al., yk-19, 77 (1975).                         325 1451  258
br77  r.e.brown,g.g.ohlsen,r.f.haglund, and n.jarmie, phys. rev.   325 1451  259
      16c, 513 (1977).                                             325 1451  260
ca85  a.d.carlson,w.p.poenitz,g.m.hale, and r.w.peele, nuclear     325 1451  261
      data for basic and applied science (santa fe, n.m.), 1429    325 1451  262
      (1985).                                                      325 1451  263
co67  j.a.cookson and d.dandy, nucl. phys. a91,273 (1967).         325 1451  264
co82  h.conde,t.andersson,l.nilsson, and c.nordborg, nuclear data  325 1451  265
      for science and technology (antwerp, belgium), 447 (1982).   325 1451  266
de73  F.Demanins et al., infn/be-73 (1973).                        325 1451  267
dr82  m.drosg,d.m.drake,r.a.hardekopf, and g.m.hale, la-9129-ms    325 1451  268
      (1982).                                                      325 1451  269
dr85  m.drosg et al., santa fe conf.1, 145(1985).                  325 1451  270
fo71  d.g.foster and d.w.glasgow, phys. rev. c3,576 (1971).        325 1451  271
fr54  g.m.frye, phys. rev. 93,1086 (1954).                         325 1451  272
go72  c.a.goulding and p.stoler, eandc(us)-176u,161 (1972).        325 1451  273
ha75  j.a.harvey and n.w.hill, nuclear cross sections and          325 1451  274
      technology (washington, d.c.), 244 (1975).                   325 1451  275
ha84  g.m.hale, nuclear standard reference data (geel,belgium)     325 1451  276
      iaea tecdoc-335, 103 (1984). describes preliminary analysis. 325 1451  277
ho68  j.c.hopkins,d.m.drake, and h.conde, nucl. phys. a107,139     325 1451  278
      (1968), and j.c.hopkins, d.m.drake, and h.conde, la-3765     325 1451  279
      (1967).                                                      325 1451  280
ho79  h.h.hogue et al., n.s.&e. 69, 22 (1979).                     325 1451  281
ju73  e.t.jurney, lasl, private communication (1973).              325 1451  282
ke58  r.d.kern and w.e.kreger, phys. rev. 112, 926 (1958).         325 1451  283
ke79  j.d.kellie,g.p.lamaze, and r.b.schwartz, nuclear cross       325 1451  284
      sections for technology (knoxville, tn.), 48 (1979).         325 1451  285
kn77  h.h.knitter,c.budtz-jorgensen,m.mailly, and r.vogt, eur-     325 1451  286
      5726e (1977).                                                325 1451  287
kn79  h.d.knox,r.m.white, and r.o.lane, n.s.&e. 69, 223 (1979).    325 1451  288
kn83  h.h.knitter,c.budtz-jorgensen,d.l.smith, and d.marletta,     325 1451  289
      n.s.&e. 83, 229(1983).                                       325 1451  290
la61  r.o.lane,a.s.langsdorf,j.e.monahan, and a.j.elwyn, ann.      325 1451  291
      phys.12, 135 (1961).                                         325 1451  292
la78  g.p.lamaze,o.a.wasson,r.a.schrack, and a.d.carlson, n.s.&e.  325 1451  293
      68, (1978).                                                  325 1451  294
li80  p.w.lisowski et al., la-8342 (1980).                         325 1451  295
ma69  d.s.mather and l.f.paine, awre-o-47/69 (1969).               325 1451  296
me65  f.merchez,n.v.sen,v.regis, and r.bouchez, compt. rend. 260,  325 1451  297
      3922 (1965).                                                 325 1451  298
ov74  j.c.overley,r.m.sealock, and d.h.ehlers, nucl. phys. a221,   325 1451  299
      573 (1974).                                                  325 1451  300
pe64  e.d.pendlebury, awre-o-60/64 (1964).                         325 1451  301
pr69  g.presser et al., nuc.phys. a131, 679(1969).                 325 1451  302
re78  c.renner,j.a.harvey,n.w.hill,g.l.morgan, and k.pusk, bull.   325 1451  303
      am. phys. soc. 23, 526 (1978).                               325 1451  304
sa82  e.t.sadowski,h.knox,d.a.resler, and r.o.lane, bap 27,624(c5) 325 1451  305
      (1982).                                                      325 1451  306
sm77  a.b.smith,p.guenther,d.havel, and j.f.whalen, anl/ndm-29     325 1451  307
      (1977).                                                      325 1451  308
sm82  a.b.smith,p.t.guenther, and j.f.whalen, nucl. phys. a373,    325 1451  309
      305 (1982).                                                  325 1451  310
wo62  c.wong,j.d.anderson, and j.w.mcclure, nucl. phys. 33,680     325 1451  311
      (1962).                                                      325 1451  312
                                                                   325 1451  313
****************************************************************** 325 1451  314
                                                                   325 1451  315
 ***************** Program LINEAR (VERSION 2004-1) *************** 325 1451  316
 For All Data Greater than 1.0000E-10 barns in Absolute Value      325 1451  317
 Data Linearized to Within an Accuracy of .100000000 per-cent      325 1451  318
 ***************** Program FIXUP (Version 2004-1) **************** 325 1451  319
 Corrected ZA/AWR in All Sections-----------------------------Yes  325 1451  320
 Corrected Thresholds-----------------------------------------No   325 1451  321
 Extended Cross Sections to 20 MeV----------------------------No   325 1451  322
 Allow Cross Section Deletion---------------------------------No   325 1451  323
 Allow Cross Section Reconstruction---------------------------Yes  325 1451  324
 Make All Cross Sections Non-Negative-------------------------Yes  325 1451  325
 Delete Energies Not in Ascending Order-----------------------Yes  325 1451  326
 Deleted Duplicate Points-------------------------------------Yes  325 1451  327
 Check for Ascending MAT/MF/MT Order--------------------------Yes  325 1451  328
 Check for Legal MF/MT Numbers--------------------------------Yes  325 1451  329
 Allow Creation of Missing Sections---------------------------No   325 1451  330
 Allow Insertion of Energy Points-----------------------------No   325 1451  331
 Create Uniform Energy Grid-----------------------------------No   325 1451  332
 Delete Section if Cross Section =0 at All Energies-----------Yes  325 1451  333
 **************** Program DICTIN (VERSION 2004-1) **************** 325 1451  334
                                1        451        413          2 325 1451  335
                                2        151          4          1 325 1451  336
                                3          1        233          1 325 1451  337
                                3          2         46          1 325 1451  338
                                3          4         45          1 325 1451  339
                                3         24         17          0 325 1451  340
                                3         51         38          1 325 1451  341
                                3         52         36          1 325 1451  342
                                3         53         19          2 325 1451  343
                                3         54         34          1 325 1451  344
                                3         55         32          1 325 1451  345
                                3         56         30          1 325 1451  346
                                3         57         21          1 325 1451  347
                                3         58         26          1 325 1451  348
                                3         59         22          1 325 1451  349
                                3         60         22          1 325 1451  350
                                3         61         20          1 325 1451  351
                                3         62         19          1 325 1451  352
                                3         63         19          1 325 1451  353
                                3         64         18          1 325 1451  354
                                3         65         16          1 325 1451  355
                                3         66         15          1 325 1451  356
                                3         67         14          1 325 1451  357
                                3         68         13          1 325 1451  358
                                3         69         12          1 325 1451  359
                                3         70         12          1 325 1451  360
                                3         71         11          1 325 1451  361
                                3         72         11          1 325 1451  362
                                3         73         11          1 325 1451  363
                                3         74         10          1 325 1451  364
                                3         75          9          1 325 1451  365
                                3         76          7          1 325 1451  366
                                3         77          7          1 325 1451  367
                                3         78          7          1 325 1451  368
                                3         79          7          1 325 1451  369
                                3         80          6          1 325 1451  370
                                3         81          5          1 325 1451  371
                                3        102        100          0 325 1451  372
                                3        103         25          0 325 1451  373
                                3        105        132          1 325 1451  374
                                4          2        284          1 325 1451  375
                                4         24        184          0 325 1451  376
                                4         51          8          0 325 1451  377
                                4         52          8          0 325 1451  378
                                4         53         38          1 325 1451  379
                                4         54          8          0 325 1451  380
                                4         55          8          0 325 1451  381
                                4         56          8          0 325 1451  382
                                4         57          8          0 325 1451  383
                                4         58          8          0 325 1451  384
                                4         59          8          0 325 1451  385
                                4         60          8          0 325 1451  386
                                4         61          8          0 325 1451  387
                                4         62          8          0 325 1451  388
                                4         63          8          0 325 1451  389
                                4         64          8          0 325 1451  390
                                4         65          8          0 325 1451  391
                                4         66          8          0 325 1451  392
                                4         67          8          0 325 1451  393
                                4         68          8          0 325 1451  394
                                4         69          8          0 325 1451  395
                                4         70          8          0 325 1451  396
                                4         71          8          0 325 1451  397
                                4         72          8          0 325 1451  398
                                4         73          8          0 325 1451  399
                                4         74          8          0 325 1451  400
                                4         75          8          0 325 1451  401
                                4         76          8          0 325 1451  402
                                4         77          8          0 325 1451  403
                                4         78          8          0 325 1451  404
                                4         79          8          0 325 1451  405
                                4         80          8          0 325 1451  406
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                                                                   325 3  0  961
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                                                                   325 3  0 1077
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                                                                   325 3  0 1117
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