1-H -  2   ENDF/B-VI, Processed by Red Cullen using PREPRO2004  6000 0  0    0
 1.00200E+3 1.99680E+0          0          0          0          4 128 1451    1
 0.0        0.0                 0          0          0          6 128 1451    2
 1.00000E+0 1.50000E+8          6          0         10          6 128 1451    3
 0.0        0.0                 1          0        218         13 128 1451    4
  1-H -  2 LANL       EVAL-FEB97 P.G.YOUNG,G.M.HALE,M.B.CHADWICK   128 1451    5
 Ch97,Ch99            DIST-AUG99 REV3-                 19990803    128 1451    6
----ENDF/B-VI         MATERIAL  128         REVISION 3             128 1451    7
-----INCIDENT NEUTRON DATA                                         128 1451    8
------ENDF-6 FORMAT                                                128 1451    9
                                                                   128 1451   10
 ****************************************************************  128 1451   11
                                                                   128 1451   12
 ENDF/B-VI MOD 4 Evaluation, February 1997, M.B. Chadwick,         128 1451   13
                 P.G. Young, and G. M. Hale  (LANL)                128 1451   14
                                                                   128 1451   15
 Produced with FKK/GNASH/GSCAN code in cooperation with ECN Petten 128 1451   16
                                                                   128 1451   17
SUMMARY                                                            128 1451   18
                                                                   128 1451   19
  This evaluation provides a complete representation of the        128 1451   20
nuclear data needed for transport, damage, heating,                128 1451   21
radioactivity, and shielding applications over the incident        128 1451   22
neutron energy range from 1.0E-11 to 150 MeV.  Below 50 MeV the    128 1451   23
evaluation is based mainly on the ENDF/B-VI.3 (Release 3)          128 1451   24
evaluation by Young (Yo94).                                        128 1451   25
                                                                   128 1451   26
 To summarize, the following ENDF sections are utilized at all     128 1451   27
energies:                                                          128 1451   28
                                                                   128 1451   29
  MF=3 MT=  1  Total Cross Section                                 128 1451   30
       MT=  2  Elastic Scattering Cross Section                    128 1451   31
       MT=  3  Nonelastic Cross Section                            128 1451   32
       MT= 16  2H(n,2n)1H Cross Section                            128 1451   33
       MT=102  Radiative Capture Cross Section (Estimate Only at   128 1451   34
               higher energies)                                    128 1451   35
                                                                   128 1451   36
  MF=4 MT=  2  Elastic Angular Distributions                       128 1451   37
                                                                   128 1451   38
  MF=6 MT= 16  Production Cross Sections and Energy-Angle          128 1451   39
               Distributions for Emission Neutrons, Protons,       128 1451   40
               Deuterons, and Alphas; and Angle-Integrated         128 1451   41
               Spectra for Gamma Rays and Residual Nuclei That     128 1451   42
               Are Stable Against Particle Emission                128 1451   43
                                                                   128 1451   44
                                                                   128 1451   45
The following modifications were made to the ENDF/B-VI.3           128 1451   46
evaluation:                                                        128 1451   47
                                                                   128 1451   48
1.  The (n,2n), elastic, and nonelastic cross sections were        128 1451   49
revised slightly above 10 MeV to better reflect experimental       128 1451   50
data;                                                              128 1451   51
                                                                   128 1451   52
2.  The tabulated elastic scattering angular distributions         128 1451   53
(MF=4, MT=2) below 3.2 MeV and above 20 MeV were revised           128 1451   54
slightly to better reflect measurements.  The results below 3.2    128 1451   55
MeV are based on a couple-channels R-matrix analysis.              128 1451   56
                                                                   128 1451   57
METHODOLOGY USED IN NEW EVALUATION                                 128 1451   58
                                                                   128 1451   59
  The neutron total cross section is based on ENDF/B-VI below      128 1451   60
100 MeV and on experimental data between 100 and 200 MeV.  The     128 1451   61
elastic scattering, nonelastic, and 2H(n,2n)1H cross sections      128 1451   62
were determined above 10 MeV in concert, using the fact that the   128 1451   63
nonelastic cross section essentially equals the (n,2n) cross       128 1451   64
section above En ~ 1 keV, and the elastic and nonelastic cross     128 1451   65
sections must sum to the total cross section.  Note that we        128 1451   66
revised the existing ENDF/B-VI (n,2n) cross section at most        128 1451   67
energies between 10 and 100 MeV to improve the agreement with      128 1451   68
experimental data.  We also included experimental data for the     128 1451   69
proton reaction cross section of 2H in our analysis, as we         128 1451   70
determined empirically that it is entirely consistent with the     128 1451   71
neutron nonelastic (or reaction) cross section above an incident   128 1451   72
nucleon energy of about 20 MeV.                                    128 1451   73
                                                                   128 1451   74
  The elastic cross section and angular distributions below an     128 1451   75
incident energy of 4 MeV were validated by comparing to results    128 1451   76
of a coupled-channels R-matrix analysis.  No changes were made     128 1451   77
to the existing ENDF/B-VI.2 cross section evaluation because the   128 1451   78
results were consistent with data and the R-matrix analysis;       128 1451   79
the elastic angular distributions below 3.2 MeV were replaced      128 1451   80
with tabulated distributions from the R-matrix analysis.           128 1451   81
                                                                   128 1451   82
  Several elastic scattering angular distribution measurements     128 1451   83
exist above 20 MeV which we fit with Legendre expansions to get    128 1451   84
integrated cross sections and to establish the evaluated angular   128 1451   85
distributions.  Especially important are the measurements of       128 1451   86
Romero, Wang, and Howard, as well as the partial distributions     128 1451   87
of Yountz and Palmieri.  We inferred nonelastic cross sections     128 1451   88
from the elastic scattering angular distribution measurements      128 1451   89
above 20 MeV, combined with our evaluated total cross section      128 1451   90
from experimental data.                                            128 1451   91
                                                                   128 1451   92
  We assume that the energy distributions of neutrons from         128 1451   93
2H(n,2n)1H follow a pure three-body phase space distribution at    128 1451   94
all incident neutron energies and utilize LAW=6 in MF=6 to         128 1451   95
represent these energy distributions.                              128 1451   96
                                                                   128 1451   97
----------------------------------------------------------------   128 1451   98
                                                                   128 1451   99
REFERENCES                                                         128 1451  100
                                                                   128 1451  101
[Ch97].  M.B. Chadwick, P G. Young, and G. M. Hale, "Evaluation    128 1451  102
  of n + 2H Cross Sections," Group T-2 Progress Report for the     128 1451  103
  Accelerator Production of Tritium Program, 1 January - 1         128 1451  104
  February 1997.                                                   128 1451  105
[Ch99]  M.B. Chadwick, P.G. Young, G.M. Hale, et al., Los Alamos   128 1451  106
  National Laboratory report, LA-UR-99-1222 (1999)                 128 1451  107
[Yo94].  P.G. Young, "n + D Evaluation to 100 MeV," Release 3,     128 1451  108
  ENDF/B-VI evaluation, distributed April, 1995.                   128 1451  109
                                                                   128 1451  110
****************************************************************** 128 1451  111
                                                                   128 1451  112
 ENDF/B-VI MOD 3 Revision, November 1996, P.G.Young (LANL)         128 1451  113
                                                                   128 1451  114
   File 6, MT=16: Second subsection added.                         128 1451  115
                                                                   128 1451  116
****************************************************************   128 1451  117
                                                                   128 1451  118
 ENDF/B-VI MOD 2 Evaluation, March 1994, M.B. Chadwick,            128 1451  119
                 P.G. Young, and G.M. Hale  (LANL)                 128 1451  120
                                                                   128 1451  121
   This evaluation is a revision of the ENDF/B-VI evaluation       128 1451  122
 by Stewart and Horsley (LA-3271, 1968).  The evaluation was       128 1451  123
 extended to 100 MeV based on experimental total, elastic, and     128 1451  124
 (n,2n) cross section measurements and elastic scattering          128 1451  125
 angular distribution measurements.  Additionally, the total       128 1451  126
 cross section (and elastic cross section) were revised between    128 1451  127
 3 and 8 MeV on the basis of newer data, and similarly the (n,2n)  128 1451  128
 cross section was revised above 10 MeV.                           128 1451  129
                                                                   128 1451  130
****************************************************************** 128 1451  131
                                                                   128 1451  132
 ENDF/B-VI MOD 1 Evaluation, December 1989, R.E. MacFarlane (LANL) 128 1451  133
                                                                   128 1451  134
       CONVERTED FOR ENDF/B-VI AT LOS ALAMOS NATIONAL LABORATORY.  128 1451  135
       THE CROSS SECTIONS, ELASTIC MF4, AND PHOTON PRODUCTION      128 1451  136
       DATA WERE LEFT UNCHANGED.  MF4 AND MF5 FOR THE (N,2N)       128 1451  137
       REACTION WERE REMOVED AND REPLACED BY AN MF6 USING AN       128 1451  138
       ANALYTIC PHASE-SPACE REPRESENTATION.  THIS IS CONSISTANT    128 1451  139
       WITH THE ORIGINAL EVALUATION, BUT PROVIDES A MORE           128 1451  140
       ACCURATE REPRESENTATION OF THE ENERGY-ANGLE CORRELATION     128 1451  141
       OF (N,2N) NEUTRONS.                                         128 1451  142
                                                                   128 1451  143
------------------------------------------------------------------ 128 1451  144
                                                                   128 1451  145
MF=2   NO RESONANCE PARAMETERS GIVEN                               128 1451  146
                                                                   128 1451  147
MF=3                                                               128 1451  148
                                                                   128 1451  149
  MT=1                                                             128 1451  150
      TOTAL CROSS SECTIONS.  ALL DATA PLOTTED AND COMPARED UP TO   128 1451  151
      1967 IN LA-3271.  CHANGES INCORPORATED BELOW 1.5 MEV BUT     128 1451  152
      EVALUATION DOES NOT AGREE WITH LOW-ENERGY EXPERIMENTS AT     128 1451  153
      NBS (WHICH ARE PRELIMINARY) BUT AGREES AT HIGHER ENERGIES.   128 1451  154
      THE DAVIS DATA SHOW A PECULIAR DROP OF A FEW PERCENT FROM    128 1451  155
      3.5 TO 9 MEV BUT AGREE ABOVE AND BELOW THESE ENERGIES.       128 1451  156
                                                                   128 1451  157
  MT=2                                                             128 1451  158
      ELASTIC CROSS SECTIONS.  DATA OBTAINED FROM INTEGRATING N-D  128 1451  159
      AND P-D ANGULAR DISTRIBUTIONS.  SINCE THE RADIATIVE          128 1451  160
      CAPTURE IS IN MICROBARNS, THE ELASTIC IS ESSENTIALLY         128 1451  161
      EQUAL TO THE TOTAL CROSS SECTION BELOW THE N,2N              128 1451  162
      THRESHOLD AND THE TOTAL MINUS THE N,2N ABOVE THE             128 1451  163
      THRESHOLD.  CHECKS AND BALANCES WERE ALWAYS MADE.  SEE       128 1451  164
      LA-3271 FOR THE GRAPHICAL COMPARISONS.                       128 1451  165
                                                                   128 1451  166
  MT=16                                                            128 1451  167
      N,2N CROSS SECTION.  DATA TAKEN FROM HOLMBERG AND FROM       128 1451  168
      CATRON.  SEE LA-3271.  NOTHING IS KNOWN ABOUT THE CROSS      128 1451  169
      SECTION ABOVE 14 MEV.                                        128 1451  170
                                                                   128 1451  171
  MT=102                                                           128 1451  172
      RADIATIVE CAPTURE CROSS SECTION.  THE THERMAL CROSS SECTION  128 1451  173
      IS 506 MICROBARNS WHICH WAS EXTRAPOLATED AS 1/V UP TO        128 1451  174
      1 KEV.  CURVE WAS DRAWN ABOVE THIS ENERGY TO INCLUDE         128 1451  175
      MEASUREMENTS ON THE INVERSE REACTION BY BOSCH.  THE          128 1451  176
      14 MEV VALUE IS A FACTOR OF 3 LOWER THAN CERINEO.            128 1451  177
      SEE LA-3271 FOR GRAPHICAL RESULTS.                           128 1451  178
                                                                   128 1451  179
MF=4                                                               128 1451  180
                                                                   128 1451  181
  MT=2                                                             128 1451  182
      ELASTIC ANGULAR DISTRIBUTIONS TAKEN FROM N-D AND P-D SCAT.   128 1451  183
      AGREEMENT IS GOOD WITH VAN OERS ANALYSIS.  SEE LA-3271.      128 1451  184
                                                                   128 1451  185
                                 MF=6                              128 1451  186
  MT=16                                                            128 1451  187
     ENERGY-ANGLE DISTRIBUTIONS REPRESENTED AS A                   128 1451  188
     3-BODY PHASE SPACE DISTRIBUTION.                              128 1451  189
                                                                   128 1451  190
                             MF= 8 AND 9                           128 1451  191
                                                                   128 1451  192
  MT=102 DECAY INFORMATION ADDED FOR TRITIUM PRODUCTION            128 1451  193
                                                                   128 1451  194
                           MF=12 AND   MF=14                       128 1451  195
                                                                   128 1451  196
  MT=102                                                           128 1451  197
      ASSUMED A SINGLE GAMMA EMITTED AT ALL ENERGIES.              128 1451  198
      EMPLOYED THE LP = 2 FLAG TO CONSERVE ENERGY                  128 1451  199
                                                                   128 1451  200
  FOR REFERENCES, SEE LA-3271.                                     128 1451  201
                                                                   128 1451  202
 ************************ C O N T E N T S ************************ 128 1451  203
 ***************** Program LINEAR (VERSION 2004-1) *************** 128 1451  204
 For All Data Greater than 1.0000E-10 barns in Absolute Value      128 1451  205
 Data Linearized to Within an Accuracy of .100000000 per-cent      128 1451  206
 ***************** Program FIXUP (Version 2004-1) **************** 128 1451  207
 Corrected ZA/AWR in All Sections-----------------------------Yes  128 1451  208
 Corrected Thresholds-----------------------------------------No   128 1451  209
 Extended Cross Sections to 20 MeV----------------------------No   128 1451  210
 Allow Cross Section Deletion---------------------------------No   128 1451  211
 Allow Cross Section Reconstruction---------------------------Yes  128 1451  212
 Make All Cross Sections Non-Negative-------------------------Yes  128 1451  213
 Delete Energies Not in Ascending Order-----------------------Yes  128 1451  214
 Deleted Duplicate Points-------------------------------------Yes  128 1451  215
 Check for Ascending MAT/MF/MT Order--------------------------Yes  128 1451  216
 Check for Legal MF/MT Numbers--------------------------------Yes  128 1451  217
 Allow Creation of Missing Sections---------------------------No   128 1451  218
 Allow Insertion of Energy Points-----------------------------No   128 1451  219
 Create Uniform Energy Grid-----------------------------------No   128 1451  220
 Delete Section if Cross Section =0 at All Energies-----------Yes  128 1451  221
 **************** Program DICTIN (VERSION 2004-1) **************** 128 1451  222
                                1        451        235          4 128 1451  223
                                2        151          4          0 128 1451  224
                                3          1        128          4 128 1451  225
                                3          2         41          4 128 1451  226
                                3          3        114          4 128 1451  227
                                3         16         22          4 128 1451  228
                                3        102        105          4 128 1451  229
                                4          2        440          4 128 1451  230
                                6         16          9          4 128 1451  231
                                8        102          3          2 128 1451  232
                                9        102          4          2 128 1451  233
                               12        102          4          2 128 1451  234
                               14        102          1          2 128 1451  235
                                                                   128 1  0  236
                                                                   128 0  0  237
 1.00200E+3 1.99680E+0          0          0          1          0 128 2151  238
 1.002000+3 1.000000+0          0          0          1          0 128 2151  239
 1.000000-5 1.000000+8          0          0          0          0 128 2151  240
 1.000000+0 5.197700-1          0          0          0          0 128 2151  241
                                                                   128 2  0  242
                                                                   128 0  0  243
 1.00200E+3 1.99680E+0          0          0          0          0 128 3  1  244
 0.0        0.0                 0          0          1        375 128 3  1  245
        375          2                                             128 3  1  246
 1.00000E-5 3.42030000 1.09051E-5 3.41922727 1.21607E-5 3.41794239 128 3  1  247
 1.33221E-5 3.41691949 1.47465E-5 3.41583392 1.63750E-5 3.41477076 128 3  1  248
 1.75872E-5 3.41407720 1.91611E-5 3.41327686 2.08855E-5 3.41250606 128 3  1  249
 2.26528E-5 3.41180927 2.51417E-5 3.41095552 2.66442E-5 3.41049909 128 3  1  250
 2.94929E-5 3.40973152 3.27499E-5 3.40897976 3.51745E-5 3.40848931 128 3  1  251
 3.83221E-5 3.40792344 4.17709E-5 3.40737840 4.53055E-5 3.40688571 128 3  1  252
 5.02833E-5 3.40628203 5.32883E-5 3.40595929 5.89856E-5 3.40541655 128 3  1  253
 6.54997E-5 3.40488498 7.03489E-5 3.40453819 7.66442E-5 3.40413806 128 3  1  254
 8.45897E-5 3.40369828 9.19727E-5 3.40334184 .000100000 3.40300000 128 3  1  255
 .000109051 3.40266154 .000121607 3.40225611 .000133221 3.40193330 128 3  1  256
 .000147465 3.40159068 .000163750 3.40125509 .000175872 3.40103615 128 3  1  257
 .000191611 3.40078347 .000208855 3.40054010 .000226528 3.40032008 128 3  1  258
 .000251417 3.40005047 .000266442 3.39990631 .000294929 3.39966387 128 3  1  259
 .000327499 3.39942640 .000351745 3.39927145 .000383221 3.39909267 128 3  1  260
 .000417709 3.39892045 .000453055 3.39876475 .000502833 3.39857397 128 3  1  261
 .000532883 3.39847196 .000589856 3.39830041 .000654997 3.39813237 128 3  1  262
 .000703489 3.39802273 .000766442 3.39789621 .000835419 3.39777435 128 3  1  263
 .000906111 3.39766418 .001005665 3.39752919 .001065766 3.39745701 128 3  1  264
 .001179713 3.39733562 .001309994 3.39721672 .001406978 3.39713915 128 3  1  265
 .001532883 3.39704964 .001670838 3.39696341 .001812222 3.39688547 128 3  1  266
 .002011331 3.39678996 .002131532 3.39673890 .002359426 3.39665302 128 3  1  267
 .002619990 3.39656891 .002813958 3.39651403 .003065767 3.39645072 128 3  1  268
 .003341676 3.39638973 .003624443 3.39633460 .004022660 3.39626706 128 3  1  269
 .004263062 3.39623095 .004718851 3.39617023 .005239977 3.39611076 128 3  1  270
 .005627914 3.39607197 .006131534 3.39602721 .006683352 3.39598411 128 3  1  271
 .007248887 3.39594516 .008045322 3.39589744 .008526126 3.39587194 128 3  1  272
 .009437703 3.39582906 .010479956 3.39578709 .011255829 3.39575972 128 3  1  273
 .012263068 3.39572815 .013356860 3.39569802 .014467097 3.39567102 128 3  1  274
 .016028156 3.39563794 .016969271 3.39562025 .018751133 3.39559052 128 3  1  275
 .020784855 3.39556142 .022296544 3.39554245 .024256391 3.39552058 128 3  1  276
 .025300000 3.39551000 .027589846 3.39548852 .029762844 3.39547047 128 3  1  277
 .032740711 3.39544872 .035460884 3.39543129 .038756968 3.39541269 128 3  1  278
 .042629201 3.39539366 .046443919 3.39537729 .050600000 3.39536161 128 3  1  279
 .055179691 3.39534643 .059525687 3.39533367 .065481421 3.39531830 128 3  1  280
 .070921765 3.39530598 .077513934 3.39529284 .085258401 3.39527938 128 3  1  281
 .092887837 3.39526781 .101200000 3.39525673 .110359383 3.39524600 128 3  1  282
 .119051376 3.39523698 .130962842 3.39522611 .141843531 3.39521741 128 3  1  283
 .155027869 3.39520812 .170516803 3.39519861 .185775674 3.39519043 128 3  1  284
 .202400000 3.39518259 .220718765 3.39517500 .238102751 3.39516863 128 3  1  285
 .261925683 3.39516095 .283687061 3.39515479 .310055738 3.39514822 128 3  1  286
 .341033606 3.39514150 .371551347 3.39513571 .404800000 3.39513017 128 3  1  287
 .441437530 3.39512480 .476205502 3.39512029 .523851366 3.39511485 128 3  1  288
 .567374123 3.39511050 .620111475 3.39510585 .682067211 3.39510109 128 3  1  289
 .743102694 3.39509699 .809600000 3.39509307 .882875060 3.39508926 128 3  1  290
 .952411007 3.39508607 1.04770274 3.39508221 1.13474825 3.39507912 128 3  1  291
 1.24022295 3.39507582 1.36413442 3.39507244 1.48620539 3.39506953 128 3  1  292
 1.61920000 3.39506674 1.76575012 3.39506403 1.90482201 3.39506175 128 3  1  293
 2.09540547 3.39505900 2.26949649 3.39505680 2.48044590 3.39505444 128 3  1  294
 2.72826884 3.39505202 2.97241077 3.39504993 3.23840000 3.39504792 128 3  1  295
 3.53150024 3.39504597 3.80964402 3.39504432 4.19081094 3.39504233 128 3  1  296
 4.53899300 3.39504072 4.96089182 3.39503900 5.45653770 3.39503723 128 3  1  297
 5.94482156 3.39503568 6.47680000 3.39503420 7.06300048 3.39503274 128 3  1  298
 7.61928803 3.39503151 8.38162186 3.39503000 9.07798596 3.39502877 128 3  1  299
 9.92178357 3.39502744 10.9130753 3.39502606 11.8896431 3.39502484 128 3  1  300
 12.9536000 3.39502365 14.1260010 3.39502247 15.2385761 3.39502145 128 3  1  301
 16.7632437 3.39502019 18.1559720 3.39501914 19.8435672 3.39501798 128 3  1  302
 21.8261507 3.39501675 23.7792862 3.39501563 25.9072000 3.39501451 128 3  1  303
 28.2520019 3.39501337 30.4771521 3.39501236 33.5264875 3.39501107 128 3  1  304
 36.3119439 3.39500997 39.6871345 3.39500871 43.6523015 3.39500732 128 3  1  305
 47.5585724 3.39500602 51.8144000 3.39500467 56.2528026 3.39500333 128 3  1  306
 62.3792480 3.39500156 68.0167866 3.39499999 74.8965965 3.39499815 128 3  1  307
 82.7209935 3.39499612 88.5194468 3.39499466 96.0165795 3.39499281 128 3  1  308
 104.427378 3.39499077 113.263852 3.39498868 125.708144 3.39498578 128 3  1  309
 133.220708 3.39498406 147.464099 3.39498084 163.749298 3.39497722 128 3  1  310
 175.872323 3.39497455 191.610438 3.39497112 208.854757 3.39496740 128 3  1  311
 226.527704 3.39496361 251.416290 3.39495832 266.441418 3.39495515 128 3  1  312
 294.928200 3.39494916 327.498598 3.39494235 351.744647 3.39493731 128 3  1  313
 383.220877 3.39493078 417.709513 3.39492365 453.055408 3.39491637 128 3  1  314
 502.832579 3.39490614 532.882834 3.39489998 589.856398 3.39488831 128 3  1  315
 654.997193 3.39487501 703.489293 3.39486512 766.441753 3.39485230 128 3  1  316
 845.897011 3.39483613 919.726596 3.39482113 1000.00000 3.39480484 128 3  1  317
 1090.50773 3.39478648 1176.39699 3.39476907 1294.09922 3.39474522 128 3  1  318
 1401.61591 3.39472345 1531.89593 3.39469708 1684.94864 3.39466612 128 3  1  319
 1835.72800 3.39463563 2000.00000 3.39460243 2213.36384 3.39455932 128 3  1  320
 2457.26128 3.39451006 2754.08287 3.39445012 3000.00000 3.39440047 128 3  1  321
 3223.70980 3.39352476 3590.93848 3.39208726 4000.00000 3.39048601 128 3  1  322
 4472.13596 3.38863788 5000.00000 3.38657162 5452.53866 3.38480023 128 3  1  323
 6345.25478 3.38130584 7419.20205 3.37710206 8253.88092 3.37383486 128 3  1  324
 9380.35770 3.36942547 10000.0000 3.36700000 20000.0000 3.34533336 128 3  1  325
 40000.0000 3.30200027 50000.0000 3.28725014 80000.0000 3.24299972 128 3  1  326
 90000.0000 3.23245445 100000.000 3.22190919 120000.000 3.20081863 128 3  1  327
 140000.000 3.17972805 160000.000 3.15863746 180000.000 3.14160694 128 3  1  328
 200000.000 3.12457641 225000.000 3.10328823 250000.000 3.08200005 128 3  1  329
 300000.000 3.05000033 350000.000 3.02760459 400000.000 3.01500508 128 3  1  330
 450000.000 3.00240555 500000.000 2.98980601 550000.000 2.97720645 128 3  1  331
 650000.000 2.95426757 750000.000 2.93132865 850000.000 2.90838970 128 3  1  332
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