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 /* NRDF D1770 Data No.18                                             */
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 /* Bibliography                                                      */
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 \\BIB,18;
 D#=D1770;
 TITLE=/ 12,13C(p,pi-)13,14Og.s. reactions in the Delta1232 resonance
         region /;
 ATH=(K.HATANAKA'1', J.KAMIYA'1', D.HIROOKA'1', Y.MAEDA'1', Y.MAEDA'2',
      T.NORO'1', E.OBAYASHI'1', H.OKAMURA'3', H.SAKAI'2', A.TAMII'2',
      K.TAMURA'4', T.WAKASA'1', K.YAKO'2', H.P.YOSHIDA'1');
 INST-ATH=(2JPNRCN'1', 2JPNTOK'2', 2JPNSUU'3', 2JPNJPN'4');
      /* '2' Department of Physics */
      /* '3' Department of Physics */
      /* '4' Department of Physics, Fukui Medical University, Fukui */
 REF=PR/C;
 VLP=65(2002)014609;
 RCTS=(12C(P,PIP)13C, 13C(P,PIP)14C, 13C(P,PIN)14O, 12C(P,PIN)13O);
 PHQS=(ANGL-DSTRN, VCTR-ANALPW);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,18;
 /* 2003-03-12 : Compiled, Am + Kc */
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'5';
 /* '5' AVF and ring cyclotrons */
 INST-ACC=2JPNRCN;
 ERS-PRJ=400KEV'6';
 /* '6' Full Width at Half Maximum */
 BEAM-INTNSTY=10[500NA;
 POL-PRJ=[70%'7';
 /* '7' Beam polarization was continuously monitored by an in-line
        polarimeter downstream of the ring cyclotron */
 ION-SOURCE=/ Polarized ion source (Atmoic beam-type polarized ion
              source [K.Hatanaka et al., Nucl. Instrum. Methods Phys.
              Res. A384(1997)575]) /;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'8',SCT,X'9',TOF);
 /* '8' Large Acceptance Spectrometer (LAS) */
 /* '9' Focal plane counter system consists of two Vertical Drift
        Chambers (VDCs). The efficiency of each plane of VDCs was
        estimated to be better than 90%, and the overall systematic
        uncertainties in the normalization were estimated to be less
        than 5%. */
 /* Experimental Method:
    - Time-of-flight
 RCT=92MO(P,P)X;
 PHQ=ENGY-SPEC;
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 /* Descriptive Parameters                                            */
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 \\DATA,18;
 INC-ENGY-LAB=18MEV;
 SYS-ERR=X%'40';
 /* '40' 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=60DEG;
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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'41'
 (MEV) (MEV) (MB/SR/MEV) (MB/SR/MEV)
 \END;
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