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| /*===================================================================*/
/* NRDF D1915 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
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,3;
/* 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=ENGY-SPEC'23';
/* '23' Relative energy spectrum */
THK-TGT=376MG/CM**2;
INC-ENGY-LAB-RANGE=67.0MEV/A;
ERS-DET=XMEV'24';
/* '24' Relatvie energy resolution (FWHM) was estimated to be
0.45 times square root of relative energy [MeV] */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,3;
INC-ENGY-LAB=67.0MEV/A;
INTRM=11BE;
THTC-INTRM=0[12DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY-INTRM'25' DSIGMA/DE DELTA-DSIGMA/DE
(MEV) (B/MEV) (B/MEV)
4.713E-02 9.831E-03 +-8.798E-04
1.558E-01 1.776E-02 +-8.798E-04
2.576E-01 2.495E-02 +-1.027E-03
3.532E-01 2.437E-02 +-1.027E-03
4.553E-01 2.658E-02 +-1.027E-03
5.510E-01 2.394E-02 +-1.173E-03
6.601E-01 2.468E-02 +-1.027E-03
7.555E-01 2.586E-02 +-1.026E-03
8.578E-01 2.616E-02 +-1.026E-03
9.601E-01 2.675E-02 +-1.320E-03
1.048E+00 3.189E-02 +-1.320E-03
1.151E+00 3.395E-02 +-1.467E-03
1.253E+00 3.571E-02 +-1.467E-03
1.362E+00 3.572E-02 +-1.613E-03
1.458E+00 3.367E-02 +-1.613E-03
1.553E+00 3.074E-02 +-1.613E-03
1.649E+00 2.664E-02 +-1.467E-03
1.752E+00 2.136E-02 +-1.614E-03
1.854E+00 2.020E-02 +-1.467E-03
1.950E+00 1.785E-02 +-1.467E-03
2.052E+00 2.006E-02 +-1.467E-03
2.148E+00 1.874E-02 +-1.614E-03
2.257E+00 1.816E-02 +-1.467E-03
2.352E+00 1.743E-02 +-1.320E-03
2.455E+00 1.803E-02 +-1.174E-03
2.557E+00 1.480E-02 +-1.467E-03
2.652E+00 1.833E-02 +-1.320E-03
2.755E+00 1.760E-02 +-1.467E-03
2.850E+00 1.849E-02 +-1.467E-03
2.952E+00 2.025E-02 +-1.760E-03
3.055E+00 1.850E-02 +-1.467E-03
3.150E+00 1.777E-02 +-1.467E-03
3.246E+00 1.953E-02 +-1.907E-03
3.355E+00 1.558E-02 +-1.760E-03
3.451E+00 1.456E-02 +-1.320E-03
3.546E+00 1.251E-02 +-1.320E-03
3.655E+00 1.354E-02 +-1.467E-03
3.751E+00 1.208E-02 +-1.320E-03
3.853E+00 1.179E-02 +-1.173E-03
3.956E+00 1.106E-02 +-1.173E-03
4.058E+00 1.048E-02 +-1.467E-03
4.147E+00 1.034E-02 +-1.467E-03
4.249E+00 7.998E-03 +-1.320E-03
4.351E+00 8.444E-03 +-1.320E-03
4.454E+00 8.596E-03 +-1.320E-03
4.549E+00 9.335E-03 +-1.467E-03
4.652E+00 6.406E-03 +-1.174E-03
4.754E+00 8.465E-03 +-1.614E-03
4.856E+00 7.297E-03 +-1.027E-03
4.959E+00 7.596E-03 +-1.173E-03
\END;
/*===================================================================*/
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