/*===================================================================*/ /* NRDF D1803 Data No.2 */ /*===================================================================*/ /* 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 */ /*===================================================================*/ \\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 */ /*===================================================================*/ \\DATA,2; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \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; /*===================================================================*/ |