/*===================================================================*/ /* NRDF D1932 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; D#=D1932; TITLE=/ In-beam gamma-ray spectroscopy of neutron-rich boron isotopes 15,17B via inelastic scattering on 12C /; ATH=(Y.KONDO'1', T.NAKAMURA'1', N.AOI'2', H.BABA'3', D.BAZIN'4', N.FUKUDA'2', T.GOMI'2', H.HASEGAWA'5', N.IMAI'2', M.ISHIHARA'2', T.KOBAYASHI'6', T.KUBO'2', M.MIURA'1', T.MOTOBAYASHI'2', A.SAITO'3', H.SAKURAI'7', S.SHIMOURA'3', T.SUGIMOTO'1', K.WATANABE'6', Y.X.WATANABE'8', T.YAKUSHIJI'6', Y.YANAGISAWA'2', K.YONEDA'4'); INST-ATH=(2JPNTIT'1', 2JPNIPC'2', 2JPNTOK'3', 1USAMSU'4', 2JPNRIK'5', 2JPNTOH'6', 2JPNTOK'7', 2JPNKEK'8'); /* '1' Department of Physics */ /* '3' Center for Nuclear Study (CNS) */ /* '4' National Superconducting Cyclotron Laboratory */ /* '5' Department of Physics */ /* '6' Department of Physics */ /* '7' Department of Physics */ REF=PR/C; VLP=71(2005)044611; RCTS=(12C(17B,17B)12C, 12C(15B,15B)12C); PHQS=(ANGL-DSTRN, XSECTN); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,2; /* 2005-07-28 : Compiled+Checked, C.Kurokawa + N.Otuka */ RTY=INEL-SCATT; CHM=ELM; PHYS-FORM=SLD; THK-TGT=377MG/CM**2; POL-TGT=0%; ALGN-TGT=0%; ACC=(CYC'9',PRJFS'10'); /* '9' 22Ne beam at 110 MeV/nucleon bombarded a primary Be target of thickness 1.1 g/cm**2 to produce the secondary 15B and 17B beams. */ /* '10' RIKEN Projectile Fragment Separator (RIPS) */ INST-ACC=(2JPNIPC'9',2JPNIPC'10'); POL-PRJ=0%; ANT-COINC=NO; DET-SYS=(MAG'11',error,NAI'12',TOF'13',EDE'14'); /* '11' To analyze outgoing boron isotopes */ /* '12' To detect deexcitation gamma rays using about a half-set of the DALI system [T. Motobayashi et al., Phys. Lett. B346(1995)9] */ /* '13' For outgoing boron isotopes. */ /* '14' For outgoing boron isotopes. */ ANL=DWBA'15'; /* '15' Using the code ECIS97 [J. Raynal, Coupled channel code ECIS97 (unpublished)]. */ /* Experimental Method: - The momentum vector of the outgoing particles was reconstructed from tracking analysis. /* 2007-12-31 : Altered, N.Otuka. N1 of BIB corrected */ RCT=12C(15B,15B)12C; PHQ=ANGL-DSTRN; INC-ENGY-LAB-RANGE=72MEV/A'24'; /* '24' Average kinetic energy at the middle of target */ BEAM-INTNSTY=12000PPS; DET-PARTCL=(GAMMA'25',15B); /* '25' Prompt gamma from 15BDoublet of two 15B deexcitation gamma lines 1.30+-0.04 MeV (1st to g.s.) and 1.41+-0.02 MeV (2nd to 1st) could not be separated due to the low statistics. COINC=(GAMMA'26',15B); /* '26' Prompt gamma from 15B */ /* 2 gamma-lines 1.30(4) and 1.41(2) are observed in 12C(17B,15B*) in this work. */ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,2; SYS-ERR=16%'16'; /* '16' Due to the gamma-ray detection efficiency which has been evaluated from the difference between the simulation and the measurement using the 22Na, 60Co, and 137Cs gamma sources. */ INC-ENGY-LAB=72MEV/A'27'; /* '27' Average kinetic energy at the middle of target */ ENGY-GAMMA=1.35MEV'28'; /* '28' Prompt gamma from 15B (Doublet of two 15B deexcitation gamma lines 1.30+-0.04 MeV (1st to g.s.) and 1.41+-0.02 MeV (2nd to 1st) could not be separated due to the low statistics.) */ EXC-ENGY-EMT-1=(1.30MEV,2.71MEV); DATA1=1.44DEG'29'; /* '29' Angular resolution in FWHM at center of mass system */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA'30' DELTA-DSIGMA/DOMEGA'30,31' (DEG) (MB/SR) (MB/SR) 0.7500000 680.5435 +-520.0280 1.250000 723.2661 +-243.9240 1.750000 979.7197 +-161.3323 2.250000 735.7481 +-164.3014 2.750000 838.1882 +-417.2768 3.250000 444.9529 +-100.2425 3.750000 373.2469 +-88.86176 4.250000 169.5277 +-56.88166 4.750000 165.6147 +-53.08438 5.250000 194.5213 +-55.74784 5.750000 171.1736 +-49.53484 6.250000 171.1513 +-48.37786 6.750000 88.21300 +-36.18578 7.250000 92.15921 +-35.21562 7.750000 74.56228 +-38.82680 8.250000 89.47507 +-42.28251 8.750000 63.69012 +-37.54509 9.250000 69.21046 +-60.74707 9.750000 61.31623 +-92.42928 \END; /*===================================================================*/ |