/*===================================================================*/ /* NRDF D1912 Data No.24 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,24; 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,24; /* 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(P,P)11B; RTY=INEL-SCATT; PHQ=POL'61'; /* '61' Induced polarization */ INC-ENGY-LAB=392MEV; DET-PARTCL=P; DET-SYS=MWPC'62'; /* '62' Focal plane polarimeter (FPP) used to measure the polarization of protons */ ERS-DET=200KEV'63'; /* '63' FWHM */ /* Experimental Method: - Double scattering (Carbon slab used as polarization analyzer) /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,24; INC-ENGY-LAB=392MEV; EMT=P; EXC-ENGY=2.12MEV; J-PTY=1/2-; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC POL'64' DELTA-POL'64,65' (DEG) (NODIM) (NODIM) 2.815 0.01 +-0.04 3.941 0.13 +-0.12 5.067 0.16 +-0.05 7.318 0.37 +-0.15 9.568 0.52 +-0.13 11.817 0.56 +-0.12 \END; /*===================================================================*/ |