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| /*===================================================================*/
/* NRDF D1915 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
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,4;
/* 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'26';
/* '26' Relative energy spectrum */
THK-TGT=376MG/CM**2;
INC-ENGY-LAB-RANGE=67.0MEV/A;
ERS-DET=XMEV'27';
/* '27' Relatvie energy resolution (FWHM) was estimated to be
0.45 times square root of relative energy [MeV] */
ANL=DWBA'28';
/* '28' ECIS code [ J. Raynal, coupled channel code ECIS97, also
notes on ECIS94 (unpublished) ] */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,4;
INC-ENGY-LAB=67.0MEV/A;
INTRM=11BE;
THTC-INTRM=0[0.5DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY-INTRM'29' DSIGMA/DE DELTA-DSIGMA/DE
(MEV) (B/MEV) (B/MEV)
5.528E-02 4.730E-03 +-1.255E-03
1.536E-01 1.300E-02 +-1.161E-03
2.518E-01 1.578E-02 +-1.154E-03
3.494E-01 1.620E-02 +-1.022E-03
4.518E-01 1.533E-02 +-1.314E-03
5.467E-01 1.238E-02 +-1.197E-03
6.511E-01 1.187E-02 +-1.269E-03
7.555E-01 9.377E-03 +-1.134E-03
8.477E-01 1.253E-02 +-1.193E-03
9.521E-01 6.766E-03 +-1.117E-03
1.052E+00 9.051E-03 +-1.168E-03
1.155E+00 8.488E-03 +-1.182E-03
1.250E+00 5.985E-03 +-1.168E-03
1.357E+00 6.270E-03 +-1.175E-03
1.450E+00 4.308E-03 +-1.093E-03
1.554E+00 6.810E-03 +-1.073E-03
1.652E+00 3.666E-03 +-1.006E-03
1.749E+00 5.255E-03 +-1.168E-03
1.851E+00 1.898E-03 +-1.168E-03
1.947E+00 3.066E-03 +-1.168E-03
2.049E+00 3.066E-03 +-1.460E-03
2.150E+00 2.390E-03 +-1.260E-03
2.247E+00 2.920E-03 +-1.168E-03
2.350E+00 2.628E-03 +-1.314E-03
2.452E+00 3.504E-03 +-1.168E-03
2.548E+00 8.759E-04 +-1.022E-03
2.650E+00 3.066E-03 +-1.314E-03
2.752E+00 1.022E-03 +-1.168E-03
2.850E+00 2.099E-04 +-1.104E-03
2.951E+00 1.606E-03 +-1.022E-03
3.053E+00 2.044E-03 +-1.168E-03
3.145E+00 8.881E-04 +-8.637E-04
3.251E+00 1.606E-03 +-1.460E-03
3.347E+00 1.460E-04 +-1.168E-03
3.450E+00 1.898E-03 +-1.314E-03
3.545E+00 1.460E-04 +-1.168E-03
3.648E+00 5.839E-04 +-1.022E-03
3.750E+00 7.299E-04 +-1.314E-03
3.846E+00 1.314E-03 +-8.759E-04
3.948E+00 1.314E-03 +-1.168E-03
4.051E+00 4.380E-04 +-1.022E-03
4.146E+00 7.299E-04 +-1.022E-03
4.249E+00 1.168E-03 +-1.168E-03
4.344E+00 5.839E-04 +-1.314E-03
4.447E+00 4.380E-04 +-1.022E-03
4.549E+00 1.168E-03 +-1.168E-03
4.659E+00 1.168E-03 +-1.168E-03
4.761E+00 0.000E+00 +-1.168E-03
4.850E+00 1.460E-04 +-1.022E-03
4.951E+00 7.585E-04 +-1.444E-03
\END;
/*===================================================================*/
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