/*===================================================================*/
 /* NRDF D1915 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 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,2;
 /* 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=PB(11BE,11BE)PB;
 PHQ=ENGY-SPEC'18';
 /* '18' Relative energy spectrum */
 THK-TGT=224MG/CM**2;
 INC-ENGY-LAB-RANGE=68.7MEV/A;
 ERS-DET=XMEV'19';
 /* '19' Relatvie energy resolution (FWHM) was estimated to be
         0.44 times square root of relative energy [MeV] */
 ANL=(DWBA'20',SEMICL-MODEL'21');
 /* '20' ECIS code [ J. Raynal, coupled channel code ECIS97, also
         notes on ECIS94 (unpublished) ] */
 /* '21' Equivalent photon method [ J.D. Jackson, Classical
         Electrodynamics, 2nd ed. (Wiley, New York 1975), C. Bertulani
         and G. Baur, Phys. Rep. 163(1988)299 ] */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=68.7MEV/A;
 INTRM=11BE;
 THTC-INTRM=0[1.3DEG;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 EXC-ENGY-INTRM'22' DSIGMA/DE DELTA-DSIGMA/DE
 (MEV) (B/MEV) (B/MEV)
 5.519E-02 3.436E-01 +-2.677E-02
 1.583E-01 7.537E-01 +-2.778E-02
 2.540E-01 8.054E-01 +-3.164E-02
 3.450E-01 7.306E-01 +-2.866E-02
 4.504E-01 6.767E-01 +-2.700E-02
 5.504E-01 5.500E-01 +-2.778E-02
 6.501E-01 4.898E-01 +-2.872E-02
 7.520E-01 3.768E-01 +-3.061E-02
 8.475E-01 3.362E-01 +-3.047E-02
 9.493E-01 2.616E-01 +-3.099E-02
 1.054E+00 2.481E-01 +-2.963E-02
 1.148E+00 1.917E-01 +-2.682E-02
 1.247E+00 1.663E-01 +-2.000E-02
 1.354E+00 1.778E-01 +-3.333E-02
 1.456E+00 1.182E-01 +-2.995E-02
 1.551E+00 1.034E-01 +-3.364E-02
 1.654E+00 1.034E-01 +-2.993E-02
 1.750E+00 6.129E-02 +-2.760E-02
 1.851E+00 7.389E-02 +-2.981E-02
 1.949E+00 4.840E-02 +-2.567E-02
 2.054E+00 2.613E-02 +-2.943E-02
 2.254E+00 3.695E-03 +-2.964E-02
 2.352E+00 1.481E-02 +-2.963E-02
 2.445E+00 1.108E-02 +-2.966E-02
 2.753E+00 1.478E-02 +-2.966E-02
 2.848E+00 2.956E-02 +-2.970E-02
 2.954E+00 0.000E+00 +-3.333E-02
 3.149E+00 3.695E-03 +-3.334E-02
 3.354E+00 2.217E-02 +-2.968E-02
 3.448E+00 1.188E-02 +-2.886E-02
 3.552E+00 2.217E-02 +-2.598E-02
 3.651E+00 4.815E-02 +-2.222E-02
 3.750E+00 3.695E-03 +-2.223E-02
 4.051E+00 1.847E-02 +-2.597E-02
 4.857E+00 2.217E-02 +-2.227E-02
 4.959E+00 1.478E-02 +-2.596E-02
 \END;
 /*===================================================================*/