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 /* NRDF D1844 Data No.147                                            */
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 /* Bibliography                                                      */
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 \\BIB,147;
 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,147;
 /* 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=98MO(P,P)X;
 PHQ=ENGY-SPEC'150';
 /* '150' Angular integrated energy spectrum */
 THK-TGT=0.45MG/CM**2;
 INC-ENGY-LAB=12MEV;
 ANL=(STATIST-MODEL'151',EXCITON-MODEL'152');
 /* '151' Hauser-Feshbach model */
 /* '152' 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,147;
 INC-ENGY-LAB=12MEV;
 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'153'
 (MEV) (MEV) (MB/MEV) (MB/MEV)
 4.0 4.2 4.726 +-0.241
 4.2 4.4 6.204 +-0.257
 4.4 4.6 7.288 +-0.272
 4.6 4.8 9.101 +-0.290
 4.8 5.0 9.674 +-0.300
 5.0 5.2 10.458 +-0.311
 5.2 5.4 11.406 +-0.322
 5.4 5.6 12.830 +-0.331
 5.6 5.8 13.434 +-0.337
 5.8 6.0 13.221 +-0.337
 6.0 6.2 12.666 +-0.335
 6.2 6.4 12.832 +-0.338
 6.4 6.6 12.058 +-0.333
 6.6 6.8 11.183 +-0.326
 6.8 7.0 10.303 +-0.320
 7.0 7.2 9.985 +-0.316
 7.2 7.4 9.151 +-0.309
 7.4 7.6 9.061 +-0.307
 7.6 7.8 8.169 +-0.302
 7.8 8.0 8.440 +-0.306
 \END;
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