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/* NRDF D1803 Data No.2 */
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/* Bibliography */
/*===================================================================*/
\\BIB,2;
D#=D1803;
TITLE=/Study of resonance states in 12N using a radioactive ion beam
of 11C/;
PURPOSE=/The authors report the first experimental result on the
elastic resonance scattering of 11C+p using the RI beam of
11C./;
ATH=(T.TERANISHI'1', S.KUBONO'1', S.SHIMOURA'1', M.NOTANI'1',
Y.YANAGISAWA'2', S.MICHIMASA'1', K.UE'1', H.IWASAKI'1',
M.KUROKAWA'1', Y.SATOU'1', T.MORIKAWA'3', A.SAITO'4', H.BABA'4',
J.H.LEE'5', C.S.LEE'5', ZS.FULOP'6', S.KATO'7');
INST-ATH=(2JPNTOK'1', 2JPNIPC'2', 2JPNKYU'3', 2JPNYOK'4', 3KORKOR'5',
3HUNDEB'6', 2JPNYMG'7');
/* '1' Center for Nuclear Study (CNS) */
/* '3' Department of Physics */
/* '4' Department of Physics */
/* '5' Department of Physics, Chun-Ang University, Seoul */
/* '7' Department of Physics */
REF=PL/B;
VLP=556(2003)27;
RCTS=1H(11C,11C)1H;
PHQS=(EXC-FUNCT, PTY);
/*===================================================================*/
/* Experimental Conditions */
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\\EXP,2;
/* 2004-08-06 : Compiled */
ENR=NAT;
CHM=CH2'8';
/* '8' Data with carbon target was also taken in a separate run to
evaluate the background contribution from the reactions of 11C
with C atoms in the (CH2)n target. */
PHYS-FORM=SLD;
THK-TGT=XMG/CM**2'9';
/* '9' Thickness of (CH2)n target is 8.0 mg/cm2 and C target is
10.7 mg/cm2 */
POL-TGT=0%;
ALGN-TGT=0%;
ACC=(CYC'10',PRJFS'11');
/* '10' Isochronous cyclotron, Primary 10B beam with 7.8 MeV/A
/* '11' To produce 11C secondary beam by the 3He(10B,12N*)n
reaction, where the 11C particles were emitted from the unbound
levels in 12N. */
INST-ACC=(2JPNIPC'10',2JPNIPC'11');
INC-ENGY-CM=0.3125[3.0375MEV'12';
/* '12' Excitation function obtained by thick target method */
BEAM-INTNSTY=17000PPS;
POL-PRJ=0%;
DET-PARTCL=P;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(PPAC'13',SI'14',TOF'15',EDE'16');
/* '13' 2 parallel plate avalanche counters 1) to identify proton
usign ToF information and 2) to determin scattering angle with
a resolution of 0.6 deg (FWHM) */
/* '14' To identify proton using E-Delta E infomation */
/* '15' Particle identification, measured by 2 PPACs and Delta-E
detector */
/* '16' Particle identification */
/* Experimental Method:
- Time-of-flight (Particle identification, measured by 2 PPACs
and Delta-E detector)
- Particle identification by 'E/Delta E' measurement (Particle
identification)
- Thick-target method (11C beam particles were fully stopped in
the (CH2)n target and energies of recoil protons, coming out from
a thick target, are measured at a forward angle in the laboratory
frame and the converted to the center-of-mass energies of
scattering. Due to the thick target, a wide range of the
excitation function for the elastic scattering can be measured
with a beam of fixed energy. See S. Kubono, Nucl. Phys.
A693(2001)221 for detail.)
RCT=1H(11C,11C)1H;
PHQ=PTY;
/* Analysis:
- Resonance formula based on [J.M. Blatt and L.C. Biedenharn,
Rev. Mod. Phys. 24(1952)258]
/*===================================================================*/
/* Descriptive Parameters */
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\\DATA,2;
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/* Data Table */
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\DATA;
RESN-ENGY'21' EXC-ENGY'22' RESN-WDTH'23' SPIN'24' PTY
(MEV) (MEV) (MEV) (NODIM) (NODIM)
2.53 3.1 0.22 3 -1
2.96 3.6 0.22 2 +1
\END;
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