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 /* NRDF D1790 Data No.5                                              */
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 /* Bibliography                                                      */
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 \\BIB,5;
 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,5;
 /* 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,13C)60NI;
 RTY=ELA-SCATT;
 PHQ=ANGL-DSTRN;
 DET-PARTCL=13C;
 ANL=DWBA'23';
 /* '23' 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,5;
 INC-ENGY-LAB=100MEV/A;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (MB/SR) (MB/SR)
 0.93 0.3320E+07 +-0.2096E+05
 1.05 0.2015E+07 +-0.1309E+05
 1.17 0.1079E+07 +-0.8357E+04
 1.30 0.5789E+06 +-0.5526E+04
 1.42 0.3533E+06 +-0.4081E+04
 1.54 0.2416E+06 +-0.3268E+04
 1.67 0.1609E+06 +-0.2584E+04
 1.79 0.1050E+06 +-0.2025E+04
 1.92 0.6284E+05 +-0.1522E+04
 2.04 0.3306E+05 +-0.1074E+04
 2.16 0.2180E+05 +-0.8494E+03
 2.29 0.1320E+05 +-0.9885E+02
 2.41 0.1101E+05 +-0.8690E+02
 2.53 0.1047E+05 +-0.8191E+02
 2.66 0.9056E+04 +-0.7382E+02
 2.78 0.6682E+04 +-0.6159E+02
 2.90 0.4118E+04 +-0.4705E+02
 3.03 0.2235E+04 +-0.3427E+02
 3.15 0.1187E+04 +-0.2513E+02
 3.27 0.8291E+03 +-0.2110E+02
 3.40 0.8198E+03 +-0.2107E+02
 3.52 0.8839E+03 +-0.2195E+02
 3.65 0.9140E+03 +-0.2239E+02
 3.77 0.7644E+03 +-0.2053E+02
 3.89 0.5735E+03 +-0.1783E+02
 4.02 0.3439E+03 +-0.1383E+02
 4.14 0.1809E+03 +-0.1005E+02
 4.26 0.1020E+03 +-0.7558E+01
 4.39 0.1035E+03 +-0.2356E+01
 4.51 0.1444E+03 +-0.2583E+01
 4.63 0.1514E+03 +-0.2501E+01
 4.76 0.1340E+03 +-0.2248E+01
 4.88 0.1034E+03 +-0.1921E+01
 5.00 0.7251E+02 +-0.1610E+01
 5.13 0.3918E+02 +-0.1185E+01
 5.25 0.2547E+02 +-0.9558E+00
 5.38 0.1933E+02 +-0.8332E+00
 5.50 0.2090E+02 +-0.8676E+00
 5.62 0.2370E+02 +-0.9246E+00
 5.75 0.2311E+02 +-0.9136E+00
 5.87 0.2050E+02 +-0.8608E+00
 5.99 0.1447E+02 +-0.7237E+00
 6.12 0.1148E+02 +-0.6449E+00
 6.24 0.6489E+01 +-0.4850E+00
 6.36 0.4354E+01 +-0.3974E+00
 6.49 0.4103E+01 +-0.3860E+00
 6.61 0.4033E+01 +-0.3828E+00
 6.73 0.2909E+01 +-0.3252E+00
 6.86 0.3311E+01 +-0.3471E+00
 6.98 0.3386E+01 +-0.3511E+00
 7.10 0.2185E+01 +-0.2821E+00
 7.23 0.1786E+01 +-0.2551E+00
 7.35 0.1422E+01 +-0.2277E+00
 7.47 0.8391E+00 +-0.1750E+00
 7.60 0.6935E+00 +-0.1591E+00
 7.72 0.4017E+00 +-0.1211E+00
 7.84 0.4749E+00 +-0.1317E+00
 7.97 0.7309E+00 +-0.1634E+00
 8.09 0.4394E+00 +-0.1268E+00
 8.22 0.3296E+00 +-0.1099E+00
 8.34 0.2198E+00 +-0.8970E-01
 8.46 0.1100E+00 +-0.6350E-01
 8.59 0.7330E-01 +-0.5180E-01
 \END;
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