/*===================================================================*/
 /* NRDF D1790 Data No.2                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1790;
 TITLE=/ Isovector quadrupole resonance observed in the
         60Ni(13C,13N)60Co reaction at E/A=100 MeV /;
 PURPOSE=/ To identify isovector giant quadrupole resonance (IVGQR)
           in the 60Ni(13C,13N)60Co /;
 ATH=(T.ICHIHARA'1', M.ISHIHARA'1', H.OHNUMA'2', T.NIIZEKI'3',
      Y.SATOU'4', H.OKAMURA'5', S.KUBONO'4', M.H.TANAKA'6',
      Y.FUCHI'6');
 INST-ATH=(2JPNIPC'1', 2JPNJPN'2', 2JPNJPN'3', 2JPNTOK'4', 2JPNSUU'5',
           2JPNKEK'6');
      /* '2' Department of Physics, Chiba Institute of Technology, Chiba
      /* '3' Faculty of Home Economics, Tokyo Kasei University, Tokyo */
      /* '4' Center for Nuclear Study (CNS) */
      /* '5' Department of Physics */
 REF=PRL;
 VLP=89(2002)142501;
 RCTS=(60NI(13C,13N)60CO, 60NI(13C,13C)60NI);
 PHQS=(GIA-RESN'7', ANGL-DSTRN, OPT-POTL-PARA);
 /* '7' The authors also did 60Ni(12C,12N)60Co at 135MeV/A. One
    resonance was found at excitation energy of 10MeV. */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2003-03-13 : Compiled */
 ENR=X%'8';
 /* '8' enriched target */
 THK-TGT=3.0MG/CM**2;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'9';
 /* '9' K540 RIKEN Ring Cyclotron */
 INST-ACC=2JPNIPC;
 INC-ENGY-LAB=100MEV/A;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'10',MWDC'11',SCT'12',TOF'13',EDE'14');
 /* '10' Spectrograph SMART [T.Ichihara et al., Nucl. Phys. A569
         (1994) 287c] */
 /* '11' To obtain momentum and scattering angle. Cathode readout
         drift chambers (CRDC) [M.H.Tanaka et al., Nucl. Instrum.
         Methods Phys. Res., A362 (1995) 521] The overall angular
         resolution obtained by reconstructing the trajectory through
         the two CRDC's was estimated to be approximately 0.1 deg. */
 /* '12' To provide Delta-E and time of flight signals for
         particle identification */
 /* '13' for paticle identification */
 /* '14' for paticle identification */
 SOLID-ANGL=XMSR'15';
 /* '15' Angular acceptance is 200 mrad for vertical and 50 mrad
         for horizontal planes. */
 ERS-DET=1MEV'16';
 /* '16' Including contribution of incident beam energy
         resolution, energy loss due to finite target thickness,
         optical momentum resolution of spectrograph, and position
         resolution of position detector */
 /* Experimental Method:
    - Time-of-flight (for paticle identification)
    - Particle identification by 'E/Delta E' measurement (for paticle
      identification)
 RCT=60NI(13C,13N)60CO;
 PHQ=ANGL-DSTRN;
 DET-PARTCL=13N;
 ANL=DWBA'18';
 /* '18' using code developed by Lenske [H.Lenske, Nucl. Phys.
         A482 (1988) 343c]. Optical potential determined by fitting the
         present data on the 60Ni(13C,13C)60Ni elastic scattering with
         code ECIS79 [J.Raynal, code ECIS79 (unpublisehd)]. */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=100MEV/A;
 EXC-ENGY=8.7MEV;
 DELTA-EXC-ENGY=0.5MEV;
 TRNSF-L=1'19';
 /* '19' Transferred orbital angular momentum L */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (MB/SR) (MB/SR)
 0.12 0.4830E+01 +-0.2100E+00
 0.37 0.5030E+01 +-0.1200E+00
 0.62 0.4230E+01 +-0.8640E-01
 0.87 0.2840E+01 +-0.6300E-01
 1.11 0.1640E+01 +-0.4600E-01
 1.36 0.1280E+01 +-0.3550E-01
 1.61 0.1330E+01 +-0.3300E-01
 1.86 0.9440E+00 +-0.2790E-01
 2.10 0.4540E+00 +-0.2280E-01
 2.35 0.3220E+00 +-0.2210E-01
 2.60 0.3720E+00 +-0.2170E-01
 2.85 0.2470E+00 +-0.1700E-01
 3.09 0.1970E+00 +-0.1520E-01
 3.34 0.1180E+00 +-0.1270E-01
 3.59 0.1170E+00 +-0.1140E-01
 3.84 0.8980E-01 +-0.1020E-01
 4.08 0.7090E-01 +-0.8890E-02
 4.33 0.3030E-01 +-0.1090E-01
 4.58 0.1780E-01 +-0.8910E-02
 4.83 0.1480E-01 +-0.6820E-02
 \END;
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