/*===================================================================*/
 /* NRDF D1915 Data No.11                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,11;
 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,11;
 /* 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'45';
 /* '45' Relatvie energy resolution (FWHM) was estimated to be
         0.45 times square root of relative energy [MeV] */
 ANL=DWBA'46';
 /* '46' ECIS code [ J. Raynal, coupled channel code ECIS97, also
         notes on ECIS94 (unpublished) ] */
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,11;
 INC-ENGY-LAB=67.0MEV/A;
 INTRM=11BE;
 EXC-ENGY-INTRM=1.7[1.9MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC-INTRM DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
 (DEG) (MB/SR/MEV) (MB/SR/MEV)
 1.426E-01 7.765E+03 +-1.428E+03
 4.635E-01 5.863E+03 +-9.812E+02
 7.665E-01 4.127E+03 +-6.233E+02
 1.052E+00 2.595E+03 +-4.772E+02
 1.373E+00 1.751E+03 +-3.514E+02
 1.676E+00 1.880E+03 +-2.537E+02
 1.979E+00 2.165E+03 +-NEGLIGIBLE
 2.264E+00 1.589E+03 +-NEGLIGIBLE
 2.585E+00 1.381E+03 +-NEGLIGIBLE
 2.870E+00 1.235E+03 +-1.471E+02
 3.173E+00 1.029E+03 +-NEGLIGIBLE
 3.512E+00 8.455E+02 +-NEGLIGIBLE
 3.779E+00 5.704E+02 +-NEGLIGIBLE
 4.100E+00 3.638E+02 +-4.911E+01
 4.385E+00 2.671E+02 +-4.470E+01
 4.688E+00 1.961E+02 +-3.936E+01
 4.973E+00 2.323E+02 +-3.888E+01
 5.312E+00 2.166E+02 +-3.625E+01
 5.615E+00 2.995E+02 +-NEGLIGIBLE
 5.900E+00 2.199E+02 +-4.043E+01
 6.203E+00 2.679E+02 +-NEGLIGIBLE
 6.488E+00 1.885E+02 +-3.468E+01
 6.809E+00 1.709E+02 +-2.861E+01
 7.112E+00 1.328E+02 +-2.890E+01
 7.415E+00 5.323E+01 +-2.138E+01
 7.718E+00 9.890E+01 +-2.497E+01
 8.004E+00 1.239E+02 +-2.698E+01
 8.307E+00 7.163E+01 +-2.328E+01
 8.610E+00 5.969E+01 +-2.280E+01
 8.930E+00 4.571E+01 +-1.746E+01
 9.234E+00 2.394E+01 +-1.309E+01
 9.537E+00 6.784E+01 +-2.461E+01
 9.840E+00 5.269E+01 +-2.543E+01
 \END;
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