/*===================================================================*/ /* NRDF D0785 Data No.1 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,1; 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,1; /* 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=95MO(P,D)94MO; PHQ=DBL-DIFF-XSECTN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,1; 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) -3.783E-01 7.524E-04 7.723E-02 1.140E+00 5.048E-01 5.091E-02 9.395E-01 9.118E-01 1.402E+00 1.218E+00 1.858E+00 8.016E-01 2.313E+00 1.018E+00 2.741E+00 4.073E-01 3.173E+00 7.027E-01 3.620E+00 5.697E-01 4.075E+00 1.047E+00 4.504E+00 2.990E+00 4.952E+00 3.285E+00 5.348E+00 2.938E+00 5.811E+00 2.706E+00 6.256E+00 1.831E+00 6.670E+00 1.616E+00 7.099E+00 1.137E+00 7.193E+00 1.253E+00 7.546E+00 1.136E+00 7.553E+00 1.073E+00 7.931E+00 1.108E+00 8.309E+00 9.990E-01 8.406E+00 9.355E-01 8.456E+00 9.848E-01 8.705E+00 9.441E-01 8.787E+00 8.850E-01 9.084E+00 8.534E-01 9.251E+00 8.672E-01 9.449E+00 8.337E-01 9.648E+00 8.496E-01 9.814E+00 8.162E-01 1.006E+01 7.331E-01 1.022E+01 7.964E-01 1.048E+01 7.155E-01 1.058E+01 7.237E-01 1.089E+01 6.320E-01 1.094E+01 6.977E-01 1.125E+01 7.039E-01 1.129E+01 6.638E-01 1.165E+01 6.628E-01 1.172E+01 6.297E-01 1.202E+01 6.480E-01 1.212E+01 6.615E-01 1.240E+01 5.948E-01 1.276E+01 6.459E-01 1.314E+01 6.090E-01 \END; /*===================================================================*/ |