/*===================================================================*/
 /* NRDF D1889 Data No.8                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,8;
 D#=D1889;
 TITLE=/ One-neutron halo structure in 15C /;
 ATH=(D.Q.FANG'1,2', T.YAMAGUCHI'1', T.ZHENG'1,3', A.OZAWA'1',
      M.CHIBA'1,4', R.KANUNGO'1', T.KATO'1', K.MORIMOTO'1',
      T.OHNISHI'1', T.SUDA'1', Y.YAMAGUCHI'1,5', A.YOSHIDA'1',
      K.YOSHIDA'1', I.TANIHATA'1');
 INST-ATH=(2JPNIPC'1', 3CPRNRS'2', 3CPRBJG'3', 2JPNTOH'4',
           2JPNNII'5');
      /* '3' Department of Technical Physics */
      /* '4' Department of Physics */
      /* '5' Department of Physics */
 REF=(PR/C'6');
 VLP=(69(2004)034613'6');
 /* 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(15C,14C)X, C(15C,13C)X, C(14C,13C)X, C(14C,X)X, C(15C,X)X);
 PHQS=(MOM-DSTRN, XSECTN);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,8;
 /* 2004-04-15 : Compiled, Kc + On */
 /* 2006-10-04 : Altered, On. Reference (CLUSTER'03) added */
 /* Related references 
    - T.Zheng et al., NP/A, 709(2002)103.
    (Reaction cross sectons for 12C and 16C beams obtained in this work
    are compared with those for 14C and 15C beams obtained in present
    work. Detailed description of the method to obtain reaction cross
    section is also found in this reference.). See also NRDF D1791.
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=X;
 POL-TGT=0%;
 ACC=(CYC'7',PRJFS'8');
 /* '7' Primary beam of 110 MeV/A 22Ne was used to bombard on a
        Be target to produce the secondary beams of 14,15C. */
 /* '8' RIKEN Projectile fragment Separator (RIPS) */
 INST-ACC=(2JPNIPC'7',2JPNIPC'8');
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(PPAC'9',SCT'10',SI'11',NAI'12',TOF'13',EDE'14');
 /* '9' To monitor beam size and emittance angle */
 /* '10' To give ToF signal */
 /* '11' To measure energy loss (Delta E) */
 /* '12' To measure total energy (E) with energy resolution of
         0.7% in FWHM for 110 MeV/A 22Ne */
 /* '13' To identify particle and to determine longitudinal
         momentum distributions */
 /* '14' To identify particle with ToF */
 /* Experimental Method:
    - Time-of-flight (To identify particle and to determine
      longitudinal momentum distributions)
    - Particle identification by 'E/Delta E' measurement (To identify
      particle with ToF)
 RCT=C(15C,X)X;
 RTY=NON-ELA-SCATT;
 PHQ=XSECTN;
 THK-TGT=375MG/CM**2'28';
 /* '28' The uncertainty in thickness was less than 1%. */
 INC-ENGY-LAB=51[83MEV/A;
 DET-PARTCL=15C;
 ANL=GLAUBER;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,8;
 TOT-ERR=X%'29';
 /* '29' Statistical error and error from background and target
         thickness */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB'30' XSECTN'31' DELTA-XSECTN'31'
 (MEV/A) (MB) (MB)
 51 1560 +-44
 83 1319 +-40
 \END;
 /*===================================================================*/