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 /* NRDF D1844 Data No.153                                            */
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 /* Bibliography                                                      */
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 \\BIB,153;
 D#=D1844;
 TITLE=/ Incident energy dependence of preequilibrium (p,p') spectra
 PURPOSE=/ To investigate the incident energy dependence of
           preequilibrium (p,p') process /;
 ATH=(Y.WATANABE'1', K.KODAKA'1', Y.KUBO'1', N.KOORI'1', M.ERIGUCHI'1',
      M.HANADA'1', I.KUMABE'1');
 INST-ATH=(2JPNKYU'1');
      /* '1' Department of Nuclear Engineering */
 REF=ZP/A;
 VLP=336(1990)63;
 RCTS=(98MO(P,P)X, 106PD(P,P)X, 60NI(P,P)X);
 PHQS=(ENGY-SPEC, ANGL-DSTRN, ENGY-SPEC'2');
 /* '2' Angular integrated energy spectrum */
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 /* Experimental Conditions                                           */
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 \\EXP,153;
 /* 2003-11-11 : Converted, Data converted from EXFOR E1323.
    Numerical data are exchanged with author's one and data which are
    obtained in the same work but not shown in the original reference
    are added. */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNKYU;
 POL-PRJ=0%;
 DET-PARTCL=P;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SBD'3',EDE);
 /* '3' Used as Delta E-E counter telescope, consisting of 75
        micro-meter and 2000 micro-meter */
 /* Experimental Method:
    - Particle identification by 'E/Delta E' measurement
 RCT=60NI(P,P)X;
 PHQ=ENGY-SPEC'174';
 /* '174' Angular integrated energy spectrum */
 THK-TGT=0.85MG/CM**2;
 INC-ENGY-LAB=18MEV;
 ANL=(STATIST-MODEL'175',EXCITON-MODEL'176');
 /* '175' Hauser-Feshbach model */
 /* '176' See [J.S. Bell and E.J. Squires, Phys. Lett. 3(1959)96]
          for detail. */
 /* Analysis:
    - Integration of angular distribution
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 /* Descriptive Parameters                                            */
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 \\DATA,153;
 INC-ENGY-LAB=18MEV;
 EMT=P;
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT-CM-MIN ENGY-EMT-CM-MAX DSIGMA/DE DELTA-DSIGMA/DE'177'
 (MEV) (MEV) (MB/MEV) (MB/MEV)
 3.0 3.2 135.753 +-0.509
 3.2 3.4 151.296 +-0.519
 3.4 3.6 157.428 +-0.526
 3.6 3.8 159.118 +-0.524
 3.8 4.0 159.780 +-0.522
 4.0 4.2 161.781 +-0.524
 4.2 4.4 158.475 +-0.517
 4.4 4.6 152.320 +-0.505
 4.6 4.8 148.324 +-0.500
 4.8 5.0 139.644 +-0.485
 5.0 5.2 132.160 +-0.471
 5.2 5.4 126.368 +-0.462
 5.4 5.6 119.370 +-0.450
 5.6 5.8 112.080 +-0.436
 5.8 6.0 103.890 +-0.423
 6.0 6.2 96.157 +-0.407
 6.2 6.4 91.736 +-0.400
 6.4 6.6 87.340 +-0.393
 6.6 6.8 82.716 +-0.385
 6.8 7.0 77.858 +-0.375
 7.0 7.2 72.831 +-0.365
 7.2 7.4 67.770 +-0.354
 7.4 7.6 65.051 +-0.354
 7.6 7.8 60.555 +-0.345
 7.8 8.0 54.856 +-0.329
 8.0 8.2 50.519 +-0.320
 8.2 8.4 48.203 +-0.318
 8.4 8.6 45.213 +-0.312
 8.6 8.8 41.964 +-0.302
 8.8 9.0 38.344 +-0.297
 9.0 9.2 36.660 +-0.292
 9.2 9.4 34.188 +-0.284
 9.4 9.6 31.689 +-0.277
 9.6 9.8 28.803 +-0.269
 9.8 10.0 27.449 +-0.268
 10.0 10.2 25.694 +-0.263
 10.2 10.4 24.392 +-0.258
 10.4 10.6 25.978 +-0.270
 10.6 10.8 21.863 +-0.256
 10.8 11.0 18.543 +-0.241
 11.0 11.2 18.704 +-0.246
 11.2 11.4 26.254 +-0.275
 11.4 11.6 19.714 +-0.324
 11.6 11.8 16.770 +-0.308
 11.8 12.0 14.118 +-0.230
 12.0 12.2 16.354 +-0.240
 12.2 12.4 23.089 +-0.269
 12.4 12.6 31.273 +-0.294
 12.6 12.8 12.780 +-0.228
 12.8 13.0 7.405 +-0.202
 13.0 13.2 8.630 +-0.227
 13.2 13.4 14.677 +-0.231
 13.4 13.6 46.149 +-0.333
 13.6 13.8 10.497 +-0.219
 13.8 14.0 9.240 +-0.217
 \END;
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