/*===================================================================*/ /* NRDF D0785 Data No.11 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,11; 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,11; /* 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=112CD(P,D)111CD; PHQ=ANGL-DSTRN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,11; 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=2.6[10.6MEV; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA (DEG) (MB/SR) 5.744E+00 1.496E+01 8.209E+00 1.541E+01 1.135E+01 1.299E+01 1.435E+01 1.022E+01 1.749E+01 8.973E+00 2.050E+01 8.616E+00 2.336E+01 7.341E+00 2.636E+01 5.280E+00 3.044E+01 3.505E+00 3.441E+01 3.331E+00 3.851E+01 3.042E+00 4.246E+01 2.232E+00 4.655E+01 1.653E+00 5.052E+01 1.540E+00 5.461E+01 1.325E+00 5.857E+01 1.095E+00 \END; /*===================================================================*/ |