/*===================================================================*/
 /* NRDF D1915 Data No.7                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,7;
 D#=D1915;
 TITLE=/ Coulomb and nuclear breakup of a halo nucleus 11Be /;
 ATH=(N.FUKUDA'1', T.NAKAMURA'2', N.AOI'1', N.IMAI'1', M.ISHIHARA'1',
      T.KOBAYASHI'3', H.IWASAKI'4', T.KUBO'1', A.MENGONI'1,5',
      M.NOTANI'6', H.OTSU'3', H.SAKURAI'4', S.SHIMOURA'6',
      T.TERANISHI'6', Y.X.WATANABE'1', K.YONEDA'1');
 INST-ATH=(2JPNIPC'1', 2JPNTIT'2', 2JPNTOH'3', 2JPNTOK'4', 2ITYBOL'5',
           2JPNTOK'6');
      /* '2' Department of Physics */
      /* '3' Department of Physics */
      /* '4' Department of Physics */
      /* '5' Applied Physics Division */
      /* '6' Center for Nuclear Study (CNS) */
 REF=PR/C;
 VLP=70(2004)054606;
 /* Secondary references 
    - EPJ/A, 25(2005)325 (T.Nakamura et al., Proc. of the 4th
      International Conference on Exotic Nuclei and Atomic Masses
      (ENAM'04))
    - NP/A, 722(2003)301C (T.Nakamura et al., Proc. of the
      International Symposium on Physics of Unstable Nuclei (ISPUN 02))
 RCTS=(PB(11BE,11BE)PB, C(11BE,11BE)C);
 PHQS=(ENGY-SPEC'8', ANGL-DSTRN, DBL-DIFF-XSECTN, XSECTN);
 /* '8' Relative energy spectrum */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,7;
 /* 2005-04-21 : Compiled+Checked, Sr + On */
 /* 2006-10-04 : Altered, On. Reference (ENAM'04) added */
 /* 2009-04-09 : Altered, On. REFERENCE: ISPUN02 Conf. Proc. added
 /* 2010-08-20 : Altered, TM. 002 corrected */
 /* 2023-04-06 : Altered, MA. REFERENCE, FACILITY and INC-SOURCE in
    001 were modified. (EPJ/AS -> EPJ/S, PRJFS in FACILITY -> FRAGM in
    INC-SOURCE) */
 RTY=INEL-SCATT;
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNIPC'9';
 /* '9' RIKEN Accelerator Research Facility */
 POL-PRJ=0%;
 ION-SOURCE=/ Fragmentation (Secondary radioactive 11Be beam is
              produced by fragmentation of 18O primary beam (100 MeV/A)
              in Be target.) /;
 DET-PARTCL=(10BE,N);
 COINC=(N,10BE);
 ANT-COINC=NO;
 DET-SYS=(MAG'10',MWDC'10',SCT'10',SCT'11',EDE,TOF'12');
 /* '10' To detect 10Be */
 /* '11' Two layers of neutron hodoscope array which consists of
         30 plastic scintillator rods and thin layer of plastic
         scintillator to reject charged particle background. */
 /* '12' To deduce momentum vector of 10Be and neutron */
 /* Analysis:
    - Invariant mass method to extract relative energy between 10Be
      and neutron
 /* In some data tables, excitation energy of 11Be is measured from
    10Be-n threshold. Authors mention that the one-neutron separation
    energy is precisely known to be 504+-4 keV. */
 RCT=C(11BE,11BE)C;
 PHQ=DBL-DIFF-XSECTN;
 THK-TGT=376MG/CM**2;
 INC-ENGY-LAB-RANGE=67.0MEV/A;
 ERS-DET=XMEV'38';
 /* '38' Relatvie energy resolution (FWHM) was estimated to be
         0.45 times square root of relative energy [MeV] */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,7;
 INC-ENGY-LAB=67.0MEV/A;
 INTRM=11BE;
 THTC-INTRM=6.0DEG;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 EXC-ENGY-INTRM DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (MEV) (MB/SR/MEV) (MB/SR/MEV)
 6.106E-01 5.787E+01 +-9.313E+00
 8.197E-01 1.024E+02 +-1.131E+01
 1.013E+00 1.098E+02 +-1.330E+01
 1.221E+00 1.044E+02 +-1.264E+01
 1.414E+00 1.377E+02 +-1.397E+01
 1.617E+00 2.169E+02 +-1.729E+01
 1.817E+00 2.302E+02 +-2.129E+01
 2.017E+00 1.922E+02 +-1.996E+01
 2.217E+00 1.543E+02 +-1.729E+01
 2.409E+00 9.180E+01 +-1.596E+01
 2.617E+00 6.186E+01 +-1.863E+01
 2.817E+00 6.186E+01 +-1.596E+01
 3.011E+00 8.581E+01 +-1.663E+01
 3.219E+00 8.381E+01 +-1.663E+01
 3.412E+00 1.098E+02 +-1.863E+01
 3.613E+00 9.978E+01 +-2.129E+01
 3.806E+00 9.446E+01 +-1.530E+01
 4.014E+00 8.647E+01 +-1.929E+01
 4.206E+00 5.455E+01 +-1.796E+01
 4.415E+00 5.854E+01 +-1.796E+01
 4.615E+00 2.661E+01 +-1.064E+01
 5.016E+00 2.528E+01 +-1.197E+01
 5.208E+00 4.656E+00 +-1.463E+01
 5.409E+00 2.993E+01 +-1.197E+01
 \END;
 /*===================================================================*/