/*===================================================================*/ /* NRDF D1842 Data No.176 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,176; D#=D1842; TITLE=/Preequilibrium (p,p') spectra for nuclei around neutron number 50/; PURPOSE=/To see how the shell and odd-even effects will appear in the continuum proton spectra, and to interpret the experimental results in terms of realistic partial state density within the framework of the preequilibrium model/; ATH=(Y.WATANABE'1', I.KUMABE'1', M.HYAKUTAKE'1', N.KOORI'1', K.OGAWA'1', K.ORITO'1', K.AKAGI'1', N.ODA'1'); INST-ATH=(2JPNKYU'1'); /* '1' Department of Nuclear Engineering */ REF=PR/C; VLP=36(1987)1325; RCTS=(90ZR(P,P)X, 92MO(P,P)X, 94MO(P,P)X, 96MO(P,P)X, 98MO(P,P)X, 100MO(P,P)X, 93NB(P,P)X, 106PD(P,P)X, AG(P,P)X); PHQS=(ENGY-SPEC, ANGL-DSTRN, ENGY-SPEC'2'); /* '2' angular-integrated energy spectrum */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,176; /* 2003-07-16 : Converted, Data converted to EXFOR E1320 and EXFOR O0504. Numerical data are exchanged with author's one and data which are obtained in the same work but not shown in the original reference are added. */ ENR=NAT; CHM=ELM; PHYS-FORM=SLD; THK-TGT=0.5[1MG/CM**2'3'; /* '3' Detailed information on the target is listed in Table I of [I.Kumabe et al., Phys. Rev. C35 (1987) 467]. */ BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=VDGT; INST-ACC=2JPNKYU; INC-ENGY-LAB=18MEV; POL-PRJ=0%; DET-PARTCL=P; COINC=NO; ANT-COINC=NO; DET-SYS=(SBD'4',SI(LI)'5'); /* '4' Used as Delta E counter, 75 micro-meter */ /* '5' Used as E counter, 2500 micro-meter */ /* Experimental Method: - Beam current integrated (Beam intensity was determined with a current integrator connected to a Faraday cup and was also monitored by a detector located at a fixed backward angle to the beam.) - Particle identification by 'E/Delta E' measurement (Signals of protons were separated from those of other charged particles with a particle identification circuit.) RCT=100MO(P,P)X; PHQ=ANGL-DSTRN; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,176; INC-ENGY-LAB=18MEV; SYS-ERR=X%'356'; /* '356' Uncertainties associated with the normalization was estimated to be within 10% for each target. However, the relative uncertainties of the cross sections for different targets is believed to be less than 4%. */ NORM=/ Absolute cross sections were determined by normalizing the experimental elastic cross sections to the optical model predictions at forward angles. The normalization factors for two sets of global optical model parameters were compared in order to estimate the uncertainties involved in this method. Optical model parameter [F.D. Becchetti, Jr. and G.W. Greenlees, Phys. Rev. 182(1969)1190] were adopted. /; EMT=P; ENGY-EMT-CM=8.0MEV; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTL DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE'357' (DEG) (MB/SR/MEV) (MB/SR/MEV) 30.0 2.101 +-0.113 40.0 1.791 +-0.031 50.0 1.541 +-0.024 60.0 1.424 +-0.023 70.0 1.302 +-0.021 80.0 1.189 +-0.020 90.0 1.077 +-0.019 100.0 0.969 +-0.018 110.0 0.895 +-0.017 120.0 0.838 +-0.016 130.0 0.825 +-0.016 140.0 0.831 +-0.016 150.0 0.851 +-0.017 160.0 0.828 +-0.016 \END; /*===================================================================*/ |