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 /* NRDF D1791 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D1791;
 TITLE=/ Study of halo structure of 16C from reaction cross section
         measurement /;
 PURPOSE=/ To study the density distribution and the neutron
           configuration of 16C /;
 ATH=(T.ZHENG'1,2,3', T.YAMAGUCHI'1', A.OZAWA'1', M.CHIBA'1',
      R.KANUNGO'1', T.KATO'1', K.KATORI'1', K.MORIMOTO'1', T.OHNISHI'1',
      T.SUDA'1', I.TANIHATA'1', Y.YAMAGUCHI'1', A.YOSHIDA'1',
      K.YOSHIDA'1', H.TOKI'1,4', N.NAKAJIMA'4');
 INST-ATH=(2JPNIPC'1', 2JPNSUT'2', 3CPRBJG'3', 2JPNRCN'4');
      /* '2' Department of Physics */
      /* '3' Department of Technical Physics */
 REF=(NP/A'5');
 VLP=(709(2002)103'5');
 /* Secondary reference 
    - NP/A, 738(2004)38 (A.Ozawa et al., Proc. of the 8th
      International Conference on Clustering Aspects of Nuclear
      Structure and Dynamics (CLUSTER'03))
 RCTS=(C(16C,X)X, C(12C,X)X);
 PHQS=RCT-XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
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 \\EXP,2;
 /* 2003-04-04 : Compiled, Sr + Kc */
 /* 2006-10-04 : Altered, On. Reference (CLUSTER'03) added */
 RTY=NON-ELA-SCATT;
 PHQ=RCT-XSECTN;
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD'6';
 /* '6' Carbon plate */
 THK-TGT=370MG/CM**2;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'7',PRJFS'8');
 /* '7' 22Ne primary beam that was accelerated to about 110 AMeV
        by the RIKEN Ring Cyclotron (RRC). */
 /* '8' Secondary 12,16C beams were produced via the projectile
        fragmentation. */
 INST-ACC=(2JPNIPC'7',2JPNIPC'8');
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'9',SI'10',NAI'11',PPAC'12',EDE'13',TOF'14');
 /* '9' Two plastic scintillators are used for a TOF measurement */
 /* '10' Three silicon detectors (150 micro-meter * 3) were used
         to measure the energy loss (Delta E) */
 /* '11' The total energy (E) was measured by a NAI(Tl) detector
         (energy resolution of 0.7% in FWHM for 110 AMeV 22Ne) [T.Suda,
         et al., RIKEN Accel. Prog. Rep. 35(2002)42.] */
 /* '12' Used to monitor beam size and transmission */
 /* '13' to particle identification */
 /* '14' to particle identification */
 /* Experimental Method:
    - Particle identification by 'E/Delta E' measurement (to particle
      identification)
    - Time-of-flight (to particle identification)
 /* Analysis:
    - In order to obtain the reaction cross section of 16C, the
      number of the inelastically scattered 16C were subtracted from
      the total number of 16C.
 RCT=C(12C,X)X;
 INC-ENGY-LAB=83MEV/A;
 DET-PARTCL=12C;
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=83MEV/A;
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 /* Data Table                                                        */
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 \DATA;
 RCT-XSECTN DELTA-RCT-XSECTN
 (MB) (MB)
 957 +-39
 \END;
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