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| /*===================================================================*/
/* NRDF D1912 Data No.20 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,20;
D#=D1912;
TITLE=/ Isovector and isoscalar spin-flip M1 strengths in 11B /;
ATH=(T.KAWABATA'1', H.AKIMUNE'2', H.FUJIMURA'3', H.FUJITA'4',
Y.FUJITA'5', M.FUJIWARA'6,7', K.HARA'8', K.Y.HARA'2',
K.HATANAKA'6', T.ISHIKAWA'9', M.ITOH'6', J.KAMIYA'10', S.KISHI'3',
M.NAKAMURA'11', K.NAKANISHI'6', T.NORO'12', H.SAKAGUCHI'3',
Y.SHIMBARA'6', H.TAKEDA'13', A.TAMII'6', S.TERASHIMA'3',
H.TOYOKAWA'14', M.UCHIDA'3', H.UENO'13', T.WAKASA'12',
Y.YASUDA'3', H.P.YOSHIDA'6', M.YOSOI'3');
INST-ATH=(2JPNTOK'1', 2JPNKON'2', 2JPNKTO'3', 3SAFWIT'4', 2JPNOSA'5',
2JPNRCN'6', 2JPNJAE'7', 2JPNKEK'8', 2JPNTOH'9', 2JPNJAE'10',
2JPNJPN'11', 2JPNKYU'12', 2JPNIPC'13', 2JPNJSR'14');
/* '1' Center for Nuclear Study (CNS) */
/* '2' Department of Physics */
/* '3' Department of Physics */
/* '4' School of Physics */
/* '5' Department of Physics */
/* '7' Advanced Photon Research Center */
/* '9' Laboratory of Nuclear Science */
/* '11' Wakayama Medical University, Wakayama */
/* '12' Department of Physics */
REF=PR/C;
VLP=70(2004)034318;
RCTS=(11B(3HE,T)11C, 11B(D,D)11B, 12C(D,D)12C, 11B(P,P)11B);
PHQS=(ANGL-DSTRN, VCTR-ANALPW, TNSR-ANALPW, POL'15', POL-TRNSF'16',
OPT-POTL-PARA);
/* '15' Induced polarization */
/* '16' Polarization transfer coefficient */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,20;
/* 2005-03-10 : Compiled, Kc + On */
ENR=X%'17';
/* '17' Contamining impurities in the 11B target were identified
by the kinematic energy shift in the elastic scattering at
backward angles, and those contributions were estimated to be
less than 1, 0.8 and 0.08 % for 10B, 12C and 16O,
respectively. */
CHM=ELM;
PHYS-FORM=SLD;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC;
INST-ACC=2JPNRCN;
BEAM-INTNSTY=1[10PNA;
POL-PRJ=X%'18';
/* '18' 200-MeV polarized deuteron and 392-MeV polarized proton
beams were used. Both beams were obtaned from the
high-intensity polarized ion source [ K.Hatanaka et al., Nucl.
Instrum. Methods Phs, Res. A 384(1997)575]. */
ION-SOURCE=/ Polarized ion source /;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG'19',MWDC'19',SCT'19');
/* '19' Grand Raiden [M.Fujiwara et al., Nucl. Instrum. Methods
Phys. Res. A 422(1999)484] for momentum analisis */
ANL=DWIA'20';
/* '20' Using a computer code DWBA98 */
RCT=11B(D,D)11B;
RTY=ELA-SCATT;
PHQ=VCTR-ANALPW;
THK-TGT=16.7MG/CM**2;
BAC=SELF;
INC-ENGY-LAB=200MEV;
DET-PARTCL=D;
ERS-DET=150KEV'53';
/* '53' FWHM */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,20;
INC-ENGY-LAB=200MEV;
EMT=D;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC AY DELTA-AY'54'
(DEG) (NODIM) (NODIM)
5.396 0.076 +-0.056
6.594 0.060 +-0.062
7.792 0.111 +-0.016
8.990 0.122 +-0.017
10.187 0.165 +-0.014
11.384 0.203 +-0.015
12.580 0.248 +-0.015
13.776 0.333 +-0.016
14.971 0.481 +-0.020
16.165 0.580 +-0.020
17.358 0.632 +-0.014
18.551 0.622 +-0.008
20.337 0.583 +-0.012
21.527 0.575 +-0.008
23.310 0.585 +-0.019
24.497 0.615 +-0.017
26.275 0.694 +-0.026
27.459 0.748 +-0.025
29.232 0.835 +-0.035
30.412 0.848 +-0.036
\END;
/*===================================================================*/
|