JENDL-3.3   Cm-248                                                0 0  0    0
 9.624800+4 2.459410+2          1          1          0          29649 1451    1
 0.000000+0 0.000000+0          0          0          0          69649 1451    2
 1.000000+0 2.000000+7          3          0         10          39649 1451    3
 0.000000+0 0.000000+0          0          0        211         549649 1451    4
 96-CM-248 JAERI      EVAL-OCT95 T.NAKAGAWA AND T.LIU             9649 1451    5
                      DIST-MAR02 REV2-OCT00            20001003   9649 1451    6
----JENDL-3.3         MATERIAL 9649                               9649 1451    7
-----INCIDENT NEUTRON DATA                                        9649 1451    8
------ENDF-6 FORMAT                                               9649 1451    9
                                                                  9649 1451   10
HISTORY                                                           9649 1451   11
84-03 EVALUATION FOR JENDL-3 WAS MADE BY Y.KIKUCHI AND            9649 1451   12
      T.NAKAGAWA (JAERI).  DETAILS ARE GIVEN IN REF. /1/.         9649 1451   13
95-10 NEW EVALUATION FOR JENDL ACTINIDE FILE WAS MADE BY          9649 1451   14
      T.NAKAGAWA AND T.LIU.                                       9649 1451   15
00-04 MODIFICATION WAS MADE BY T.NAKAGAWA.                        9649 1451   16
                                                                  9649 1451   17
     ***** Modified parts from JENDL-3.2 *******************      9649 1451   18
     MF=2                                                         9649 1451   19
     MF=3  All data                                               9649 1451   20
     MF=4  All data                                               9649 1451   21
     MF=5  All data                                               9649 1451   22
     *******************************************************      9649 1451   23
                                                                  9649 1451   24
                                                                  9649 1451   25
MF=1  GENERAL INFORMATION                                         9649 1451   26
  MT=451   COMMENTS AND DICTIONARY                                9649 1451   27
  MT=452   NUMBER OF NEUTRONS PER FISSION                         9649 1451   28
             SUM OF MT'S =455 AND 456.                            9649 1451   29
  MT=455   DELAYED NEUTRON DATA                                   9649 1451   30
             SEMI-EMPIRICAL FORMULA BY TUTTLE /2/.                9649 1451   31
  MT=456   PROMPT NEUTRON DATA                                    9649 1451   32
             SEMI-EMPIRICAL FORMULA BY HOWERTON /3/.              9649 1451   33
                                                                  9649 1451   34
MF=2,MT=151  RESONANCE PARAMETERS                                 9649 1451   35
        (TAKEN FROM JENDL-3.2)                                    9649 1451   36
     RESOLVED RESONANCE REGION (MLBW) : 1.0E-5 TO 1.5 KEV         9649 1451   37
        RESONANCE ENERGIES, NEUTRON AND RADIATIVE WIDTHS WERE     9649 1451   38
        TAKEN FROM THE EXPERIMENTAL DATA OF BENJAMIN ET AL./4/.   9649 1451   39
        FOR RESONANCES WHOSE RADIATIVE WIDTH WAS UNKNOWN, THE     9649 1451   40
        AVERAGE VALUE OF 0.026 EV /4/ WAS ADOPTED. THE FISSION    9649 1451   41
        WIDTHS were adopted from Moore and Keyworth /5/ and       9649 1451   42
        Maguire et al. /6/ THE AVERAGE FISSION WIDTH OF 0.0013    9649 1451   43
        EV /5/ WAS USED FOR ALL RESONANCES OF WHICH FISSION       9649 1451   44
        WIDTH HAD NOT BEEN MEASURED.  Then the fission widths were9649 1451   45
        roughly adjusted to the fission cross section measured by 9649 1451   46
        Maguire et al.  R=9.1 FM WAS ASSUMED TO REPRODUCE THE     9649 1451   47
        POTENTIAL SCATTERING CROSS SECTION OF 10.4 BARNS ASSUMED  9649 1451   48
        BY BENJAMIN ET AL./4/.  THE NEUTRON WIDTH OF THE FIRST    9649 1451   49
        RESONANCE WAS SLIGHTLY ADJUSTED TO REPRODUCE THE CAPTURE  9649 1451   50
        CROSS SECTION OF 2.57 BARNS AT 0.0253 EV.  BACKGROUND     9649 1451   51
        CROSS SECTIONS WERE GIVEN ONLY FOR THE FISSION AND TOTAL  9649 1451   52
        CROSS SECTIONS BY ASSUMING THE FORM OF 1/V.  THE THERMAL  9649 1451   53
        CROSS SECTIONS TO BE REPRODUCED WERE ESTIMATED FROM       9649 1451   54
        AVAILABLE EXPERIMENTAL DATA.                              9649 1451   55
                                                                  9649 1451   56
     UNRESOLVED RESONANCE REGION : 1.5 KEV TO 30 KEV              9649 1451   57
        PARAMETERS WERE DETERMINED WITH A FITTING CODE ASREP/7/   9649 1451   58
        OBTAINED FROM OPTICAL MODEL CALCULATION:                  9649 1451   59
          S1=3.32E-4, S2=0.844E-4.                                9649 1451   60
        ESTIMATED FROM RESOLVED RESONANCES:                       9649 1451   61
          D-OBS=40.0 EV, GAM-G=26 MILLI-EV, S0=1.2E-4             9649 1451   62
        GAM-F OBTAINED BY FITTING THE DATA OF STOPA ET AL./6/     9649 1451   63
        Scattring radius R was adjusted so as to reproduce the    9649 1451   64
        ealstic scattering cross section calculated with CASTHY   9649 1451   65
        at 30 keV.                                                9649 1451   66
                                                                  9649 1451   67
  CALCULATED 2200 M/S CROSS SECTIONS AND RESONANCE INTEGRALS      9649 1451   68
                   2200 M/S VALUE           RES. INT.             9649 1451   69
      TOTAL           9.456  B                 -                  9649 1451   70
      ELASTIC         6.514  B                 -                  9649 1451   71
      FISSION         0.372  B               10.0  B              9649 1451   72
      CAPTURE         2.570  B              267.   B              9649 1451   73
                                                                  9649 1451   74
MF=3  NEUTRON CROSS SECTIONS                                      9649 1451   75
     BELOW 30 KEV, CROSS SECTIONS WERE REPRESENTED WITH RESONANCE 9649 1451   76
     PARAMETERS. BACKGROUND CROSS SECTION WAS GIVEN TO FISSION.   9649 1451   77
                                                                  9649 1451   78
  MT=1 TOTAL CROSS SECTION                                        9649 1451   79
      CALCULATED WITH CASTHY CODE /8/ BASED ON THE SHERICAL       9649 1451   80
      OPTICAL MODEL. THE OPTICAL POTENTIAL OF REF./9/ WERE        9649 1451   81
      USED.                                                       9649 1451   82
                                                                  9649 1451   83
           V = 45.036-0.3*EN                        (MEV)         9649 1451   84
           WS= 4.115+0.4*EN                         (MEV)         9649 1451   85
           WV= 0             , VSO = 7.5            (MEV)         9649 1451   86
           R = RSO = 1.256   , RS  = 1.260           (FM)         9649 1451   87
           A = ASO = 0.626   , B   = 0.555+0.0045*EN (FM)         9649 1451   88
                                                                  9649 1451   89
      COMPETING PROCESSES OF THE FISSION, (N,2N) AND (N,3N) WERE  9649 1451   90
      TAKEN INTO ACCOUNT.  THE FOLLOWING LEVEL DENSITY PARAMETERS 9649 1451   91
      OF GILBERT-CAMERON'S FORMULA /10/ WERE USED.                9649 1451   92
                                                                  9649 1451   93
                 ISOTOPE        CM-248         CM-249             9649 1451   94
                A(1/MEV)         27.8           34.2              9649 1451   95
        SPIN-CUTOFF PARA.        30.39          33.79             9649 1451   96
          PAIRING E(MEV)          0.0            0.903            9649 1451   97
             TEMP. (MEV)          0.326          0.366            9649 1451   98
                C(1/MEV)         10.8           12.2              9649 1451   99
                 EX(MEV)          1.85           4.30             9649 1451  100
                                                                  9649 1451  101
      THE LEVEL SCHEME TAKEN FROM REF. /11/.                      9649 1451  102
                   NO.        ENERGY(KEV)   SPIN-PARITY           9649 1451  103
                  G.S.            0.0           0 +               9649 1451  104
                   1.            43.4           2 +               9649 1451  105
                   2.           143.8           4 +               9649 1451  106
                   3.           298.8           6 +               9649 1451  107
                   4.           506.0           8 +               9649 1451  108
                   5.           761.9          10 +               9649 1451  109
                   6.          1049.0           2 +               9649 1451  110
                   7.          1049.0           1 -               9649 1451  111
                   8.          1062.8          12 +               9649 1451  112
                   9.          1084.0           0 +               9649 1451  113
                  10.          1094.0           3 -               9649 1451  114
                  11.          1126.0           2 +               9649 1451  115
                  12.          1143.0           4 +               9649 1451  116
                  13.          1172.0           5 -               9649 1451  117
                  14.          1222.0           4 +               9649 1451  118
                  15.          1235.0           3 -               9649 1451  119
                  16.          1302.0           3 -               9649 1451  120
                CONTINUUM LEVELS ASSUMED ABOVE 1314 KEV.          9649 1451  121
                                                                  9649 1451  122
  MT= 2         ELASTIC SCATTERING                                9649 1451  123
      CALCULATED AS TOTAL - PARTIAL CROSS SECTIONS.               9649 1451  124
                                                                  9649 1451  125
  MT= 4         TOTAL INELASTIC SCATTERING                        9649 1451  126
      SUM OF MT=51, 52, 53, 54 AND 91.                            9649 1451  127
                                                                  9649 1451  128
  MT=16,17      (N,2N),(N,3N)  CROSS SECTION                      9649 1451  129
      STAPRE RESULTS CALCULATED BY KONSHIN /12/ WERE ADOPTED.     9649 1451  130
                                                                  9649 1451  131
  MT=18            FISSION CROSS SECTION                          9649 1451  132
      BELOW 6 MEV TAKEN FROM JENDL-3.2 WHICH WAS EVALUATED ON     9649 1451  133
      THE BASIS OF THE MEASURED DATA BY STOPA ET AL./6/ AND       9649 1451  134
      FOMUSHKIN ET AL./13/. FROM 6 MEV TO 8 MEV, THE STAPRE       9649 1451  135
      RESULT CALCULATED BY KONSHIN /12/ WERE USED.  FROM 8 MEV    9649 1451  136
      TO 20 MEV BY EYE GUIDE, BASED ON THE MEASURED DATA OF       9649 1451  137
      FOMUSHKIN ET AL./14/                                        9649 1451  138
                                                                  9649 1451  139
  MT=51, 52, 53, 54   Inelastic scattering                        9649 1451  140
      CALCULATED BY ECIS /15/ AND CASTHY /8/ CODES.               9649 1451  141
      LAGRANGE'S DEFORMED OPTICAL POTENTIAL PARAMETERS /16/ WERE  9649 1451  142
      USED.                                                       9649 1451  143
           V  = 49.82 - 17*((N-Z)/A) - 0.3*EN (MEV)               9649 1451  144
           WS =  5.52 - 9*((N-Z)/A)+ 0.4*EN (MEV)     <EN=<10 MEV 9649 1451  145
              =  9.52 - 9*((N-Z)/A) (MEV)          10=<EN=<20 MEV 9649 1451  146
           VSO = 6.2                                              9649 1451  147
           R = RS = 1.26, RSO = 1.12           (FM)               9649 1451  148
           A = 0.63, AS = 0.52, ASO = 0.47     (FM)               9649 1451  149
           BETA-2 = 0.204, BETA-4 = 0.051                         9649 1451  150
  MT=55-66, 91        Inelastic scattering                        9649 1451  151
      CALCULATED WITH CASTHY CODE /8/.                            9649 1451  152
                                                                  9649 1451  153
  MT=102 RADIATIVE CAPTURE                                        9649 1451  154
      CALCULATED WITH CASTHY CODE/8/.  AVERAGE RADIATIVE WIDTH    9649 1451  155
      = 0.026 EV /17/ AND D-obs = 40 EV OBTAINED FROM THE LEVEL   9649 1451  156
      DENSITY PARAMETERS WERE USED.  They were consistent with    9649 1451  157
      the unresolved resonance parameters.  DIRECT AND            9649 1451  158
      SEMI-DIRECT CAPTURE CROSS SECTIONS WERE ESTIMATED WITH DSD  9649 1451  159
      CODE /18/.                                                  9649 1451  160
                                                                  9649 1451  161
                                                                  9649 1451  162
MF=4  ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS                 9649 1451  163
  MT=2                                                            9649 1451  164
      BELOW 300 KEV: CALCULATED WITH CASTHY CODE /8/              9649 1451  165
      ABOVE 500 KEV: CALCULATED WITH ECIS CODE /15/               9649 1451  166
                                                                  9649 1451  167
  MT=16,17,18                                                     9649 1451  168
      ASSUMED TO BE ISOTROPIC IN THE LABORATORY SYSTEM.           9649 1451  169
                                                                  9649 1451  170
  MT=51,52,53,54                                                  9649 1451  171
      SUM OF ECIS AND CASTHY CALCULATIONS.                        9649 1451  172
                                                                  9649 1451  173
  MT=55-66,91                                                     9649 1451  174
      CALCULATED WITH CASTHY CODE.                                9649 1451  175
                                                                  9649 1451  176
MF=5  ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS                  9649 1451  177
  MT=16,17,91                                                     9649 1451  178
      CALCULATED WITH EGNASH /19/.                                9649 1451  179
                                                                  9649 1451  180
  MT=18                                                           9649 1451  181
      MAXWELLIAN FISSION SPECTRUM.  TEMPERATURE ESTIMATED FROM    9649 1451  182
      SYSTEMATICS OF HOWERTON AND DOYAS /20/.  THE RATIOS OF      9649 1451  183
      MULTI-CHANCE FISSION TO TOTAL WERE ESTIMATED FROM STAPRE    9649 1451  184
      CALCULATION/12/.                                            9649 1451  185
                                                                  9649 1451  186
                                                                  9649 1451  187
References                                                        9649 1451  188
 1) KIKUCHI Y. AND NAKAGAWA T.: JAERI-M 84-116 (1984).            9649 1451  189
 2) TUTTLE R.J.: INDC(NDS)-107/G+SPECIAL, P.29 (1979).            9649 1451  190
 3) HOWERTON R.J.: NUCL. SCI. ENG., 62, 438 (1977).               9649 1451  191
 4) BENJAMIN R.W. ET AL.: NUCL. SCI. ENG., 55, 440(1974).         9649 1451  192
 5) MOORE M.S. AND KEYWORTH G.A.: PHYS. REV., C3, 1656(1971)      9649 1451  193
 6) STOPA C.R.S. ET AL.: 1982 KIAMESHA, 1090 (1982), AND          9649 1451  194
    MAGUIRE JR. H.T. ET AL.: NUCL. SCI. ENG., 89, 293 (1985).     9649 1451  195
 7) KIKUCHI Y. et al.: JAERI-Data/Code 99-025 (1999).             9649 1451  196
 8) IGARASI S. AND FUKAHORI T.: JAERI 1321 (1991).                9649 1451  197
 9) IGNATYUK A.V. ET AL.: SOV. J. NUCL. PHYS., 42, 360 (1985).    9649 1451  198
10) GILBERT A. AND CAMERON A.G.W.: CAN. J. PHYS., 43, 1446 (1965).9649 1451  199
11) SCHMORAK M.R.: NUCL. DATA SHEETS, 57, 515 (1989).             9649 1451  200
12) KONSHIN V.A.: JAERI-RESEARCH 95-010 (1995).                   9649 1451  201
13) FOMUSHKIN E.F. ET AL.: SOV. J. NUCL. PHYS., 31, 19(1980).     9649 1451  202
14) FOMUSHKIN E.F. ET AL.: Proc. Int. Conf. Nuclear Data for      9649 1451  203
    Science and Technology, Juelich, Germany, 13-17 May 1991, p.  9649 1451  204
    439 (1992).                                                   9649 1451  205
15) RAYNAL J.: IAEA SMR-9/8 (1970).                               9649 1451  206
16) LAGRANGE Ch. and JARY J.: NEANDC(E) 198 "L" (1978)            9649 1451  207
17) Mughabghab S.F.: "Neutron Cross Sections," Vol.1, Part B,     9649 1451  208
    Academic Press (1984).                                        9649 1451  209
18) KAWANO T.: PRIVATE COMMUNICATION (1999).                      9649 1451  210
19) YAMAMURO. N.: JAERI-M 90-006 (1990).                          9649 1451  211
    Young P.G. and Arthur E.D.: LA-6947 (1977).                   9649 1451  212
20) HOWERTON R.J. AND DOYAS R.J.: NUCL. SCI. ENG., 46, 414        9649 1451  213
     (1971).                                                      9649 1451  214
                                                                  9649 1451  215
                                1        451        269          29649 1451  216
                                1        452          5          19649 1451  217
                                1        455          7          19649 1451  218
                                1        456          4          19649 1451  219
                                2        151        122          29649 1451  220
                                3          1         40          29649 1451  221
                                3          2         39          29649 1451  222
                                3          4         22          29649 1451  223
                                3         16         12          29649 1451  224
                                3         17          9          29649 1451  225
                                3         18         25          29649 1451  226
                                3         51         22          29649 1451  227
                                3         52         21          29649 1451  228
                                3         53         19          29649 1451  229
                                3         54         18          29649 1451  230
                                3         55          9          29649 1451  231
                                3         56         13          29649 1451  232
                                3         57         13          29649 1451  233
                                3         58          8          29649 1451  234
                                3         59         12          29649 1451  235
                                3         60         12          29649 1451  236
                                3         61         12          29649 1451  237
                                3         62         11          29649 1451  238
                                3         63         11          29649 1451  239
                                3         64         11          29649 1451  240
                                3         65         10          29649 1451  241
                                3         66         10          29649 1451  242
                                3         91          8          29649 1451  243
                                3        102         24          29649 1451  244
                                4          2        159          29649 1451  245
                                4         16          2          29649 1451  246
                                4         17          2          29649 1451  247
                                4         18          2          29649 1451  248
                                4         51        136          29649 1451  249
                                4         52        136          29649 1451  250
                                4         53        133          29649 1451  251
                                4         54        133          29649 1451  252
                                4         55         29          29649 1451  253
                                4         56         27          29649 1451  254
                                4         57         27          29649 1451  255
                                4         58         28          29649 1451  256
                                4         59         27          29649 1451  257
                                4         60         27          29649 1451  258
                                4         61         27          29649 1451  259
                                4         62         27          29649 1451  260
                                4         63         27          29649 1451  261
                                4         64         27          29649 1451  262
                                4         65         27          29649 1451  263
                                4         66         27          29649 1451  264
                                4         91         27          29649 1451  265
                                5         16        170          29649 1451  266
                                5         17         80          29649 1451  267
                                5         18          8          29649 1451  268
                                5         91        311          29649 1451  269
                                                                  9649 1  099999
 9.624800+4 2.459410+2          0          2          0          09649 1452    1
 0.000000+0 0.000000+0          0          0          1          49649 1452    2
          4          2          0          0          0          09649 1452    3
 1.000000-5 3.129600+0 6.000000+6 4.377600+0 8.000000+6 4.787400+09649 1452    4
 2.000000+7 7.283400+0                                            9649 1452    5
                                                                  9649 1  099999
 9.624800+4 2.459410+2          0          2          0          09649 1455    1
 0.000000+0 0.000000+0          0          0          6          09649 1455    2
 1.280000-2 3.140000-2 1.280000-1 3.250000-1 1.350000+0 3.700000+09649 1455    3
 0.000000+0 0.000000+0          0          0          1          49649 1455    4
          4          2          0          0          0          09649 1455    5
 1.000000-5 1.960000-2 6.000000+6 1.960000-2 8.000000+6 1.340000-29649 1455    6
 2.000000+7 1.340000-2                                            9649 1455    7
                                                                  9649 1  099999
 9.624800+4 2.459410+2          0          2          0          09649 1456    1
 0.000000+0 0.000000+0          0          0          1          29649 1456    2
          2          2          0          0          0          09649 1456    3
 1.000000-5 3.110000+0 2.000000+7 7.270000+0                      9649 1456    4
                                                                  9649 1  099999
                                                                  9649 0  0    0
 9.624800+4 2.459410+2          0          0          1          09649 2151    1
 9.624800+4 1.000000+0          0          1          2          09649 2151    2
 1.000000-5 1.500000+3          1          2          0          09649 2151    3
 0.000000+0 9.100000-1          0          0          1          09649 2151    4
 2.459410+2 0.000000+0          0          0        282         479649 2151    5
 7.247000+0 5.000000-1 2.525650-2 1.886500-3 2.330000-2 7.000000-59649 2151    6
 2.690000+1 5.000000-1 5.132000-2 1.920000-2 3.200000-2 1.200000-49649 2151    7
 3.501000+1 5.000000-1 4.178000-2 1.150000-2 3.020000-2 8.000000-59649 2151    8
 7.610000+1 5.000000-1 1.253000-1 9.509990-2 2.600000-2 4.200000-39649 2151    9
 9.895000+1 5.000000-1 1.734700-1 1.470000-1 2.600000-2 4.700000-49649 2151   10
 1.403000+2 5.000000-1 3.005000-2 1.500000-3 2.600000-2 2.550000-39649 2151   11
 1.864000+2 5.000000-1 3.318000-2 4.179990-3 2.600000-2 3.000000-39649 2151   12
 2.379000+2 5.000000-1 4.480000-2 1.620000-2 2.600000-2 2.600000-39649 2151   13
 2.587000+2 5.000000-1 8.980000-2 6.180000-2 2.600000-2 2.000000-39649 2151   14
 3.218000+2 5.000000-1 5.330000-2 2.600000-2 2.600000-2 1.300000-39649 2151   15
 3.806000+2 5.000000-1 1.193000-1 9.199990-2 2.600000-2 1.300000-39649 2151   16
 4.157000+2 5.000000-1 7.640000-2 4.910000-2 2.600000-2 1.300000-39649 2151   17
 4.577000+2 5.000000-1 1.015000-1 7.450000-2 2.600000-2 1.000000-39649 2151   18
 4.849000+2 5.000000-1 3.650000-2 9.500000-3 2.600000-2 1.000000-39649 2151   19
 5.418000+2 5.000000-1 4.060000-1 3.790000-1 2.600000-2 1.000000-39649 2151   20
 6.053000+2 5.000000-1 1.010000-1 7.399990-2 2.600000-2 1.000000-39649 2151   21
 6.470000+2 5.000000-1 1.340000-1 1.070000-1 2.600000-2 1.000000-39649 2151   22
 6.886000+2 5.000000-1 6.430000-2 3.700000-2 2.600000-2 1.300000-39649 2151   23
 6.943000+2 5.000000-1 2.273000-1 2.000000-1 2.600000-2 1.300000-39649 2151   24
 7.215000+2 5.000000-1 1.163000-1 8.899990-2 2.600000-2 1.300000-39649 2151   25
 7.694000+2 5.000000-1 8.830000-2 6.100000-2 2.600000-2 1.300000-39649 2151   26
 8.659000+2 5.000000-1 5.103000-1 4.830000-1 2.600000-2 1.300000-39649 2151   27
 8.871000+2 5.000000-1 1.253000-1 9.799990-2 2.600000-2 1.300000-39649 2151   28
 9.586000+2 5.000000-1 1.323000-1 1.050000-1 2.600000-2 1.300000-39649 2151   29
 9.942000+2 5.000000-1 1.473000-1 1.200000-1 2.600000-2 1.300000-39649 2151   30
 1.042000+3 5.000000-1 2.143000-1 1.870000-1 2.600000-2 1.300000-39649 2151   31
 1.103300+3 5.000000-1 2.433000-1 2.160000-1 2.600000-2 1.300000-39649 2151   32
 1.193600+3 5.000000-1 3.523000-1 3.250000-1 2.600000-2 1.300000-39649 2151   33
 1.209700+3 5.000000-1 6.230000-2 3.500000-2 2.600000-2 1.300000-39649 2151   34
 1.262000+3 5.000000-1 2.933000-1 2.660000-1 2.600000-2 1.300000-39649 2151   35
 1.276600+3 5.000000-1 2.023000-1 1.750000-1 2.600000-2 1.300000-39649 2151   36
 1.288100+3 5.000000-1 8.130000-2 5.400000-2 2.600000-2 1.300000-39649 2151   37
 1.389000+3 5.000000-1 4.263000-1 3.990000-1 2.600000-2 1.300000-39649 2151   38
 1.505000+3 5.000000-1 6.983000-1 6.710000-1 2.600000-2 1.300000-39649 2151   39
 1.646000+3 5.000000-1 1.573000-1 1.300000-1 2.600000-2 1.300000-39649 2151   40
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