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| /*===================================================================*/
/* NRDF D1915 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
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,1;
/* 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'13';
/* '13' Relative energy spectrum */
THK-TGT=224MG/CM**2;
INC-ENGY-LAB-RANGE=68.7MEV/A;
ERS-DET=XMEV'14';
/* '14' Relatvie energy resolution (FWHM) was estimated to be
0.44 times square root of relative energy [MeV] */
ANL=(DWBA'15',SEMICL-MODEL'16');
/* '15' ECIS code [ J. Raynal, coupled channel code ECIS97, also
notes on ECIS94 (unpublished) ] */
/* '16' 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,1;
INC-ENGY-LAB=68.7MEV/A;
INTRM=11BE;
THTC-INTRM=0[6DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY-INTRM'17' DSIGMA/DE DELTA-DSIGMA/DE
(MEV) (B/MEV) (B/MEV)
5.576E-02 6.695E-01 +-3.474E-02
1.504E-01 1.337E+00 +-2.963E-02
2.516E-01 1.513E+00 +-2.842E-02
3.451E-01 1.468E+00 +-2.459E-02
4.562E-01 1.386E+00 +-3.158E-02
5.538E-01 1.244E+00 +-3.704E-02
6.496E-01 1.152E+00 +-3.704E-02
7.550E-01 9.505E-01 +-3.474E-02
8.445E-01 9.037E-01 +-3.333E-02
9.563E-01 7.857E-01 +-3.221E-02
1.051E+00 7.315E-01 +-3.900E-02
1.149E+00 6.519E-01 +-3.704E-02
1.257E+00 6.411E-01 +-4.105E-02
1.352E+00 5.368E-01 +-3.789E-02
1.457E+00 4.200E-01 +-4.105E-02
1.550E+00 3.979E-01 +-3.789E-02
1.655E+00 3.632E-01 +-3.789E-02
1.755E+00 2.621E-01 +-3.474E-02
1.853E+00 2.968E-01 +-3.474E-02
1.949E+00 1.963E-01 +-3.704E-02
2.058E+00 1.926E-01 +-3.704E-02
2.158E+00 1.295E-01 +-2.842E-02
2.256E+00 1.296E-01 +-2.963E-02
2.362E+00 1.642E-01 +-3.158E-02
2.456E+00 7.579E-02 +-2.842E-02
2.549E+00 6.316E-02 +-3.158E-02
2.654E+00 2.848E-02 +-2.532E-02
2.762E+00 1.185E-01 +-2.963E-02
2.856E+00 1.298E-01 +-2.812E-02
2.956E+00 7.863E-02 +-3.190E-02
3.056E+00 6.058E-02 +-3.100E-02
3.152E+00 1.148E-01 +-2.963E-02
3.255E+00 4.444E-02 +-2.963E-02
3.357E+00 1.074E-01 +-2.963E-02
3.459E+00 6.947E-02 +-2.842E-02
3.552E+00 6.316E-02 +-2.842E-02
3.657E+00 8.526E-02 +-2.526E-02
3.754E+00 7.037E-02 +-2.963E-02
3.856E+00 4.105E-02 +-2.526E-02
3.961E+00 2.842E-02 +-2.211E-02
4.060E+00 7.579E-02 +-2.791E-02
4.153E+00 3.158E-02 +-2.842E-02
4.258E+00 2.526E-02 +-2.211E-02
4.451E+00 1.111E-02 +-2.593E-02
4.556E+00 3.158E-02 +-2.768E-02
4.663E+00 2.447E-02 +-2.606E-02
4.766E+00 -3.158E-03 +-2.908E-02
4.862E+00 5.926E-02 +-2.593E-02
4.964E+00 2.593E-02 +-2.593E-02
\END;
/*===================================================================*/
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