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 /* NRDF D1915 Data No.6                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,6;
 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 */
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 /* Experimental Conditions                                           */
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 \\EXP,6;
 /* 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=ANGL-DSTRN;
 THK-TGT=224MG/CM**2;
 INC-ENGY-LAB-RANGE=68.7MEV/A;
 ERS-DET=XMEV'34';
 /* '34' Relatvie energy resolution (FWHM) was estimated to be
         0.44 times square root of relative energy [MeV] */
 ANL=(DWBA'35',SEMICL-MODEL'36');
 /* '35' ECIS code [ J. Raynal, coupled channel code ECIS97, also
         notes on ECIS94 (unpublished) ] */
 /* '36' Equivalent photon method [ J.D. Jackson, Classical
         Electrodynamics, 2nd ed. (Wiley, New York 1975), C. Bertulani
         and G. Baur, Phys. Rep. 163(1988)299 ] */
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,6;
 INC-ENGY-LAB=68.7MEV/A;
 INTRM=11BE;
 EXC-ENGY-INTRM=0[1MEV'37';
 /* '37' Relative energy between 10Be and neutron (= Excitation
         energy of 11Be measured from 10Be-n threshold) */
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 /* Data Table                                                        */
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 \DATA;
 THTC-INTRM DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (B/SR) (B/SR)
 1.555E-01 5.652E+02 +-NEGLIGIBLE
 4.582E-01 4.802E+02 +-NEGLIGIBLE
 7.609E-01 3.537E+02 +-NEGLIGIBLE
 1.071E+00 2.553E+02 +-NEGLIGIBLE
 1.374E+00 1.769E+02 +-NEGLIGIBLE
 1.661E+00 1.303E+02 +-NEGLIGIBLE
 1.963E+00 9.217E+01 +-NEGLIGIBLE
 2.266E+00 6.258E+01 +-NEGLIGIBLE
 2.569E+00 4.080E+01 +-NEGLIGIBLE
 2.855E+00 2.502E+01 +-NEGLIGIBLE
 3.158E+00 1.664E+01 +-NEGLIGIBLE
 3.460E+00 1.085E+01 +-NEGLIGIBLE
 3.763E+00 5.768E+00 +-NEGLIGIBLE
 4.057E+00 4.426E+00 +-NEGLIGIBLE
 4.360E+00 2.353E+00 +-5.913E-01
 4.655E+00 2.040E+00 +-5.127E-01
 4.949E+00 9.031E-01 +-4.002E-01
 5.259E+00 2.827E-01 +-3.963E-01
 5.546E+00 3.328E-01 +-2.441E-01
 \END;
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