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 /* NRDF D1901 Data No.1                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D1901;
 TITLE=/ Study of the density distribution of 17C from reaction cross
         section measurement /;
 ATH=(C.WU'1,2', Y.YAMAGUCHI'1,3', A.OZAWA'1', R.KANUNGO'1',
      I.TANIHATA'1', T.SUZUKI'4', D.Q.FANG'1,5', T.SUDA'1',
      T.OHNISHI'1', M.FUKUDA'6', N.IWASA'7', T.OHTSUBO'3',
      T.IZUMIKAWA'3', R.KOYAMA'3', W.SHINOZAKI'3', M.TAKAHASHI'3');
 INST-ATH=(2JPNIPC'1', 3CPRBJG'2', 2JPNNII'3', 2JPNSUU'4', 3CPRNRS'5',
           2JPNOSA'6', 2JPNTOH'7');
      /* '2' School of Physics */
      /* '3' Department of Physics */
      /* '4' Department of Physics */
      /* '6' Department of Physics */
      /* '7' Department of Physics */
 REF=(NP/A'8');
 VLP=(739(2004)3'8');
 /* 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(17C,X)X, C(17C,17C)C);
 PHQS=(RCT-XSECTN, XSECTN'9');
 /* '9' Inelastic cross section */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 2005-09-14 : Compiled, Kc + Am + On */
 /* 2006-10-04 : Altered, On. Reference (CLUSTER'03) added */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=377MG/CM**2;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'10',PRJFS'11');
 /* '10' Secondary beam 17C was produced by the projectile
        fragmentation of the primary beam 22Ne at 110 A MeV. */
 /* '11' RIKEN projectile fragment separator (RIPS) */
 INST-ACC=(2JPNIPC'10',2JPNIPC'11');
 INC-ENGY-LAB=79MEV/A;
 POL-PRJ=0%;
 DET-PARTCL=17C;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'12',NAI'13',IC'14',PPAC'15',TOF,EDE);
 /* '12' To give TOF signal */
 /* '13' To measure the total energy */
 /* '14' To measure the energy loss (Delta E) */
 /* '15' To monitor the beam position */
 ANL=(GLAUBER'16',X'17');
 /* '16' Finite-range Glauber model */
 /* '17' Kox formula [S.Kox et al., Phys. Rev. C 35(1987)1678] */
 /* Experimental Method:
    - Time-of-flight
    - Particle identification by 'E/Delta E' measurement
 /* Analysis:
    - Transmission method
 RCT=C(17C,X)X;
 RTY=NON-ELA-SCATT;
 PHQ=RCT-XSECTN;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 DELTA-RCT-XSECTN=+-11MB;
 DELTA-RCT-XSECTN=+-9MB'18';
 /* '18' Uncertainty in the incident contaminations */
 DELTA-RCT-XSECTN=+-4MB'19';
 /* '19' Uncertainty in the estimation of fragments */
 DELTA-RCT-XSECTN=+-0.5MB'20';
 /* '20' Uncertainty in the target thickness */
 DELTA-RCT-XSECTN=+-15MB'21';
 /* '21' Uncertainty in the estimation of inelastic particles */
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB RCT-XSECTN DELTA-RCT-XSECTN
 (MEV/A) (MB) (MB)
 79 1350 +-21
 \END;
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