/*===================================================================*/ /* NRDF D0785 Data No.5 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,5; D#=D785; TITLE=/ A systematic study of the (p,d) strength for transitions to deeply bound hole states /; ATH=(T.ISHIMATSU'1', M.NIWANO'1', N.KAWAMURA'1', H.OHMURA'2', T.AWAYA'3'); INST-ATH=(2JPNTOH'1', 2JPNJTD'2', 2JPNAOY'3'); /* '1' Department of Physics */ /* '2' School of Medicine */ /* '3' College of Science and Engineering */ REF=NP/A; VLP=336(1980)205; RCTS=(95MO(P,D)94MO, 98MO(P,D)97MO, 112CD(P,D)111CD, 116CD(P,D)115CD, 115IN(P,D)114IN, 124SN(P,D)123SN, 130TE(P,D)129TE, 141PR(P,D)140PR, 94MO(P,D)93MO, 100MO(P,D)99MO, 142ND(P,D)141ND); PHQS=(DBL-DIFF-XSECTN, ANGL-DSTRN); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,5; /* 2009-08-06 : Compiled+Checked, Nh */ CHM=ELM; PHYS-FORM=SLD; POL-TGT=0%; ALGN-TGT=0%; ACC=SYNCYC; INST-ACC=2JPNINS; INC-ENGY-LAB-RANGE=52MEV; POL-PRJ=0%; DET-PARTCL=D; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG,PROP-CNTR,SCT); ANL=(DWBA,OPT-MODEL); RCT=115IN(P,D)114IN; PHQ=DBL-DIFF-XSECTN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,5; INC-ENGY-LAB=52MEV; SYS-ERR=X%'4'; /* '4' Total systematic error. Largest contribution to uncertainties comes from error in calibrated values of solid angle of spectrometer. */ THTL=20DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY DSIGMA/DOMEGA/DE (MEV) (MB/SR/MEV) -3.064E-01 3.072E-02 7.630E-02 1.766E+00 5.724E-01 5.636E+00 9.953E-01 9.037E+00 1.415E+00 3.998E+00 1.842E+00 1.784E+00 2.268E+00 1.242E+00 2.273E+00 1.236E+00 2.719E+00 9.749E-01 2.723E+00 9.783E-01 3.115E+00 8.885E-01 3.119E+00 8.294E-01 3.566E+00 7.804E-01 3.998E+00 8.166E-01 4.412E+00 1.084E+00 4.826E+00 1.502E+00 5.184E+00 1.702E+00 5.546E+00 1.719E+00 5.690E+00 1.675E+00 5.890E+00 1.556E+00 6.079E+00 1.412E+00 6.286E+00 1.308E+00 6.503E+00 1.237E+00 6.664E+00 1.178E+00 6.930E+00 1.164E+00 7.017E+00 1.104E+00 7.349E+00 1.113E+00 7.400E+00 1.037E+00 7.764E+00 1.027E+00 7.783E+00 9.695E-01 8.160E+00 9.549E-01 8.160E+00 9.332E-01 8.521E+00 9.261E-01 8.575E+00 9.189E-01 8.889E+00 8.760E-01 8.963E+00 8.876E-01 9.242E+00 8.254E-01 9.386E+00 8.399E-01 9.656E+00 7.967E-01 9.782E+00 7.967E-01 1.002E+01 7.751E-01 1.018E+01 7.824E-01 1.038E+01 7.320E-01 1.058E+01 7.393E-01 1.073E+01 7.080E-01 1.099E+01 7.177E-01 1.110E+01 6.888E-01 1.137E+01 6.890E-01 1.146E+01 6.818E-01 1.175E+01 6.963E-01 1.182E+01 6.563E-01 1.214E+01 7.037E-01 1.219E+01 6.789E-01 1.254E+01 6.821E-01 1.290E+01 6.534E-01 1.328E+01 6.391E-01 1.360E+01 6.608E-01 1.396E+01 6.465E-01 1.432E+01 6.683E-01 1.467E+01 6.611E-01 1.503E+01 6.468E-01 1.537E+01 6.469E-01 1.571E+01 6.470E-01 1.605E+01 6.255E-01 1.636E+01 6.400E-01 \END; /*===================================================================*/ |