/*===================================================================*/ /* NRDF D0785 Data No.16 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,16; 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,16; /* 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=141PR(P,D)140PR; PHQ=ANGL-DSTRN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,16; 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. */ EXC-ENGY=6.6[14.5MEV; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 8.262E+00 1.030E+01 1.123E+01 8.411E+00 1.439E+01 6.806E+00 1.746E+01 5.763E+00 2.043E+01 5.967E+00 2.345E+01 5.504E+00 2.646E+01 4.636E+00 3.044E+01 3.392E+00 3.456E+01 3.035E+00 3.840E+01 2.771E+00 4.252E+01 2.219E+00 4.664E+01 1.778E+00 5.062E+01 1.591E+00 5.460E+01 1.409E+00 5.872E+01 1.175E+00 \END; /*===================================================================*/ |