/*===================================================================*/
 /* NRDF D1924 Data No.1                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D1924;
 TITLE=/ Density distribution of 17B from a reaction cross-section
         measurement /;
 ATH=(Y.YAMAGUCHI'1,2', C.WU'1,3', T.SUZUKI'2', A.OZAWA'1', D.Q.FANG'1,
     4', M.FUKUDA'5', N.IWASA'6', T.IZUMIKAWA'2', H.JEPPESEN'1,7',
      R.KANUNGO'1', R.KOYAMA'2', T.OHNISHI'1', T.OHTSUBO'2',
      W.SHINOZAKI'2', T.SUDA'1', M.TAKAHASHI'2', I.TANIHATA'1');
 INST-ATH=(2JPNIPC'1', 2JPNNII'2', 3CPRBJG'3', 3CPRNRS'4', 2JPNOSA'5',
           2JPNTOH'6', 2DENAAU'7');
      /* '2' Department of Physics */
      /* '3' School of Physics */
      /* '5' Department of Physics */
      /* '6' Department of Physics */
      /* '7' Department of Physics and Astronomy */
 REF=PR/C;
 VLP=70(2004)054320;
 RCTS=12C(17B,X)X;
 PHQS=XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 2005-01-30 : Compiled, Kc + Am + On. */
 RTY=NON-ELA-SCATT;
 PHQ=XSECTN;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=377MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'8',PRJFS'9');
 /* '8' Incident primary beam of 22Ne with 110 A MeV accelerated
        by the RIKEN ring cyclotron, was directed onto the Be or Ta
        production target to produce 17B as a sectondary beam. */
 /* '9' RIKEN projectile fragment separator (RIPS) */
 INST-ACC=(2JPNIPC'8',2JPNIPC'9');
 INC-ENGY-LAB=77MEV/A;
 BEAM-INTNSTY=[200PPS;
 POL-PRJ=0%;
 DET-PARTCL=17B;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'10',NAI'11',IC'12',PPAC,EDE,TOF);
 /* '10' To obtain the TOF information */
 /* '11' To measure energy (E) */
 /* '12' Tilted-Electrode Gas Ionization Chamber (TEG-IC) used to
         measure Delta E */
 ANL=(GLAUBER,X'13');
 /* '13' Phenomenological formula [S.Kox et al. Phys. Rev. C
         35(1987)1678] */
 /* Experimental Method:
    - Particle identification by 'E/Delta E' measurement
    - Time-of-flight
    - Transmission method
 RCT=12C(17B,X)X;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 DELTA-RCT-XSECTN=+-19MB'14';
 /* '14' Depending on the uncertainty of the number of outgoing
         unreacted 17B */
 DELTA-RCT-XSECTN=+-9MB'15';
 /* '15' Uncertainty from contamination of the incident particle
         from reacted events in silicon detector */
 DELTA-RCT-XSECTN=+-1MB'16';
 /* '16' Uncertainty from measurement of reacion-target thickness
 DELTA-RCT-XSECTN=+-7MB'17';
 /* '17' Uncertainty from estimation of the number of fragments
         (13,14,15B) and the ambiguity of its method */
 DELTA-RCT-XSECTN=+-18MB'18';
 /* '18' Uncertainty from estimation of inelastic events */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB RCT-XSECTN'19' DELTA-RCT-XSECTN'19'
 (MEV/A) (MB) (MB)
 77 1400 +-29
 \END;
 /*===================================================================*/