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/* NRDF D1573 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
D#=D1573;
TITLE=/ Coulomb dissociation of a halo nucleus 11Be at 72A MeV /;
PURPOSE=/ To perform the coincidence measurement of 11Be
dissociation /;
ATH=(T.NAKAMURA'1', S.SHIMOURA'1', T.KOBAYASHI'2', T.TERANISHI'1',
K.ABE'3', N.AOI'1', Y.DOKI'1', M.FUJIMAKI'2', N.INABE'2',
N.IWASA'4', K.KATORI'3', T.KUBO'2', H.OKUNO'1', T.SUZUKI'2',
I.TANIHATA'2', Y.WATANABE'2', A.YOSHIDA'2', M.ISHIHARA'1,2');
INST-ATH=(2JPNTOK'1', 2JPNIPC'2', 2JPNOSA'3', 2JPNRIK'4');
/* '1' Department of Physics */
/* '3' Department of Physics */
/* '4' Department of Physics */
REF=PL/B;
VLP=331(1994)296;
RCTS=(PB(11BE,11BE)PB, 12C(11BE,11BE)12C, PB(11BE,N,10BE)PB);
PHQS=(ENGY-SPEC, STRGTH-FUNCT, ANGL-DSTRN'5', MOM-DSTRN'6',
ANGL-DSTRN'7', ANGL-DSTRN'8');
/* '5' dsigma/db (b=impact parameter. b is related to the
scattering angle theta of the c.m. of 10Be+n system as b=a cot
(theta/2), where a represents half the distance of closest approach
in the classical Coulomb head-on collision) */
/* '6' Mean values of longitudinal momentum distributions */
/* '7' dsigma/dphi (azimuthal angular distibution of 10Be in 11Be
rest frame) */
/* '8' dsigma/dcos(theta) (polar angular distibution of 10Be in
11Be rest frame) */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,3;
/* 2005-09-13 : Converted, Sr + On. Converted to EXFOR E1573 */
/* 2005-10-18 : Altered, Ah + Sr. Re-digitized */
CHM=ELM;
PHYS-FORM=SLD;
ACC=PRJFS'9';
/* '9' 11Be is provided by using a projectile fragmentation of
100A MeV 18O */
INST-ACC=2JPNIPC'10';
/* '10' RIPS */
INC-ENGY-LAB=72.0MEV/A;
ERS-PRJ=0.2MEV/A'11';
/* '11' FWHM */
DET-PARTCL=(N,10BE);
COINC=(N,10BE);
ANT-COINC=NO;
DET-SYS=(MAG'12',SCT'12',X'13',SCT'14',EDE'15',TOF'16');
/* '12' To detect 10Be */
/* '13' Drift chamber (To detect 10Be) */
/* '14' To detect neutron */
/* '15' To identify 10Be */
/* '16' To determine momentum vector of 10Be and neutron */
ERS-DET=XKEV'17';
/* '17' Energy resolution is proportional to square root of
relative energy between 10Be and neutron. 450 keV FWHM is
estimated at 1 MeV (relative energy). */
/* Experimental Method:
- Particle identification by 'E/Delta E' measurement (To identify
10Be)
- Time-of-flight (To determine momentum vector of 10Be and
neutron)
RCT=(PB(11BE,11BE)PB, 12C(11BE,11BE)12C);
RTY=(INEL-SCATT,X'21');
/* '21' Coulomb breakup reaction */
PHQ=STRGTH-FUNCT;
THK-TGT=XMG/CM**2'22';
/* '22' 104 mg/cm**2 for Pb target, 184 mg/cm**2 for C target */
ANL=X'23';
/* '23' Direct breakup model */
/* Analysis:
- Coulomb part of the dissociation on Pb is obtained by
subtraction the nuclear contribution from the original spectrum.
Cross section for C target is used to estimate the nuclear
contribution.
- Equivalent photon method [C.A. Bertulani and G. Banr, Phys.
Rep. 163 (1988) 299.]
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,3;
INC-ENGY-LAB=72.0MEV/A;
SYS-ERR=[20%'24';
/* '24' Total systematic error. Uncertainty in the absolute
normalization (mainly coming from uncertainties in neutron
detection efficiency) */
EMT-2=N;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY-EMT BE-L'25' DELTA-BE-L'25,26'
(MEV) (UNIT) (UNIT)
5.452E-01 2.996E-01 +-8.126E-02
6.592E-01 7.202E-01 +-1.308E-01
7.618E-01 9.108E-01 +-1.308E-01
8.610E-01 9.091E-01 +-1.427E-01
9.603E-01 9.014E-01 +-1.546E-01
1.064E+00 8.442E-01 +-1.546E-01
1.213E+00 7.158E-01 +-1.269E-01
1.412E+00 7.124E-01 +-1.308E-01
1.611E+00 6.535E-01 +-1.487E-01
1.806E+00 5.390E-01 +-1.789E-01
1.997E+00 1.966E-01 +-2.064E-01
2.310E+00 4.183E-01 +-1.633E-01
2.706E+00 8.928E-02 +-1.847E-01
3.104E+00 1.734E-01 +-2.345E-01
3.504E+00 8.450E-03 +-2.816E-01
3.999E+00 8.077E-03 +-2.628E-01
\END;
/*===================================================================*/
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