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 /* NRDF D1313 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 D#=D1842;
 TITLE=/Preequilibrium (p,p') spectra for nuclei around neutron number
        50/;
 PURPOSE=/To see how the shell and odd-even effects will appear in the
          continuum proton spectra, and to interpret the experimental
          results in terms of realistic partial state density within the
          framework of the preequilibrium model/;
 ATH=(Y.WATANABE'1', I.KUMABE'1', M.HYAKUTAKE'1', N.KOORI'1',
      K.OGAWA'1', K.ORITO'1', K.AKAGI'1', N.ODA'1');
 INST-ATH=(2JPNKYU'1');
      /* '1' Department of Nuclear Engineering */
 REF=PR/C;
 VLP=36(1987)1325;
 RCTS=(90ZR(P,P)X, 92MO(P,P)X, 94MO(P,P)X, 96MO(P,P)X, 98MO(P,P)X,
       100MO(P,P)X, 93NB(P,P)X, 106PD(P,P)X, AG(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,1;
 /* 2003-07-16 : Converted, Data converted to EXFOR E1320 and EXFOR
    O0504. 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=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.5[1MG/CM**2'3';
 /* '3' Detailed information on the target is listed in Table I of
        [I.Kumabe et al., Phys. Rev. C35 (1987) 467]. */
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNKYU;
 INC-ENGY-LAB=18MEV;
 POL-PRJ=0%;
 DET-PARTCL=P;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SBD'4',SI(LI)'5');
 /* '4' Used as Delta E counter, 75 micro-meter */
 /* '5' Used as E counter, 2500 micro-meter */
 /* Experimental Method:
    - Beam current integrated (Beam intensity was determined with a
      current integrator connected to a Faraday cup and was also
      monitored by a detector located at a fixed backward angle to the
      beam.)
    - Particle identification by 'E/Delta E' measurement (Signals of
      protons were separated from those of other charged particles with
      a particle identification circuit.)
 RCT=90ZR(P,P)X;
 PHQ=ENGY-SPEC;
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 INC-ENGY-LAB=18MEV;
 SYS-ERR=X%'6';
 /* '6' Uncertainties associated with the normalization was
        estimated to be within 10% for each target. However, the
        relative uncertainties of the cross sections for different
        targets is believed to be less than 4%. */
 NORM=/ Absolute cross sections were determined by normalizing the
        experimental elastic cross sections to the optical model
        predictions at forward angles. The normalization factors for
        two sets of global optical model parameters were compared in
        order to estimate the uncertainties involved in this method.
        Optical model parameter [F.D. Becchetti, Jr. and G.W.
        Greenlees, Phys. Rev. 182(1969)1190] were adopted. /;
 EMT=P;
 THTL=30DEG;
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT-CM-MIN ENGY-EMT-CM-MAX DSIGMA/DOMEGA/DE
 DELTA-DSIGMA/DOMEGA/DE'7'
 (MEV) (MEV) (MB/SR/MEV) (MB/SR/MEV)
 \END;
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