/*===================================================================*/
 /* NRDF D1957 Data No.1                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D1957;
 TITLE=/ Measurement of the breakup cross sections in 6He+9Be
         reaction at 25 MeV/nucleon /;
 ATH=(J.WANG'1', Y.-LI.YE'1', D.-X.JIANG'1', G.-L.ZHANG'1',
      D.-Y.PANG'1', Z.-H.LI'1', T.ZHENG'1', X.-Q.LI'1', Q.-J.WANG'1',
      Q.-Y.HU'1', C.-E.WU'1', A.OZAWA'2', Y.YAMAGUCHI'2', R.KANUNGO'2',
      D.FANG'2', I.TANIHATA'2');
 INST-ATH=(3CPRBJG'1', 2JPNIPC'2');
      /* '1' School of Physics and DOE Key Laboratory of Heavy Ion
              Physics */
 REF=CPL;
 VLP=22(2005)1370;
 /* Secondary reference 
    - JP/G, 31(2005)S1647 (Y.L.Ye et al., Proc. of the 1st
      International Conference on NUclear, STructure, Astrophysics and
      Reactions (NUSTAR'05))
 RCTS=9BE(6HE,2*N,ALPHA)9BE;
 PHQS=ANGL-DSTRN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 2005-10-22 : Compiled+Checked, C.Kurokawa + N.Otuka */
 /* 2006-10-04 : Altered, N.Otuka. Reference (NUSTAR'05) added */
 /* 2009-08-23 : Altered, Nf. REFERENCE: JP/S -> JP/G */
 PHQ=ANGL-DSTRN;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'4';
 /* '4' 100 micro-meter */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'5',PRJFS'6');
 /* '5' To accelerate primary 13C beam to 70 MeV/nucleon */
 /* '6' To separate secondary 6He beam from 9Be target */
 INST-ACC=(2JPNIPC'5',2JPNIPC'6');
 /* '6' RIKEN projectile fragment separator (RIPS) */
 INC-ENGY-LAB-RANGE=25MEV/A;
 BEAM-INTNSTY=[200000PPS;
 POL-PRJ=0%;
 DET-PARTCL=(N,ALPHA);
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SI'7',SBD'7',CSI'7',SCT'8');
 /* '7' To measure energy of 4He */
 /* '8' To measure neutron in coincidence with 4He */
 ANL=X'9';
 /* '9' Serber model (a spectator-participant model) [A.G. Sitenko,
        Nucl. Phys. A422(1985)122] */
 /* Analysis:
    - Integration of energy distribution (Integration of inclusive
      alpha spectra assuming Gaussian shape, which width and peak
      position are determined by coincidence with neutron detection)
 RCT=9BE(6HE,2*N,ALPHA)9BE;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 INC-ENGY-LAB=25MEV/A;
 SYS-ERR=[20%'10';
 /* '10' Uncertainties in counts of direct breakup peaks in energy
         spectra */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTL DELTA-THTL DSIGMA/DOMEGA'11' DELTA-DSIGMA/DOMEGA'11,12'
 (DEG) (DEG) (MB/SR) (MB/SR)
 8.822E+00 +-1.480E+00 1.504E+03 +-8.511E+01
 1.276E+01 +-2.344E+00 4.468E+02 +-7.801E+01
 1.563E+01 +-1.151E+00 3.475E+02 +-7.092E+01
 1.633E+01 +-1.481E+00 2.624E+02 +-7.092E+01
 2.032E+01 +-2.139E+00 1.277E+02 +-6.383E+01
 \END;
 /*===================================================================*/