/*===================================================================*/
 /* NRDF D1770 Data No.9                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,9;
 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,9;
 /* 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
 /* 2006-09-08 : Altered, Mh. Re-digitized */
 RCT=13C(P,PIN)14O;
 PHQ=VCTR-ANALPW;
 ENR=99%;
 THK-TGT=136MG/CM**2;
 INC-ENGY-LAB=300MEV;
 DET-PARTCL=PIN;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,9;
 INC-ENGY-LAB=300MEV;
 EXC-ENGY=0.0MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 SQ-MOM AY DELTA-AY
 ((GEV/C)**2) (NODIM) (NODIM)
 3.390E-01 3.735E-02 +-1.538E-01
 4.258E-01 7.450E-01 +-1.143E-01
 4.901E-01 7.494E-01 +-1.319E-01
 5.275E-01 1.165E-01 +-1.494E-01
 5.511E-01 -4.154E-01 +-1.363E-01
 \END;
 /*===================================================================*/