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 /* NRDF D1790 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 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. */
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 /* Experimental Conditions                                           */
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 \\EXP,1;
 /* 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=GIA-RESN'17';
 /* '17' The authors also did 60Ni(12C,12N)60Co at 135MeV/A. One
         resonance was found at excitation energy of 10MeV. */
 DET-PARTCL=13N;
 /* Analysis:
    - Resonance parameters are obtained by fit two gaussians to
      excitation spectram (contributions of quasi-free charge-exchange
      are subtracted before the fit)
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 INC-ENGY-LAB=100MEV/A;
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY DELTA-EXC-ENGY WDTH DELTA-WDTH
 (MEV) (MEV) (MEV) (MEV)
 8.7 +-0.5 2.8 +-0.8
 20 +-2 9 +-2
 \END;
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