/*===================================================================*/ /* NRDF D0785 Data No.8 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,8; 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,8; /* 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=DBL-DIFF-XSECTN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,8; 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) -3.421E-01 1.727E-02 7.947E-02 3.618E+00 4.912E-01 4.357E+00 9.170E-01 6.490E+00 1.358E+00 3.156E+00 1.755E+00 3.014E+00 2.168E+00 3.276E+00 2.601E+00 2.951E+00 3.017E+00 2.039E+00 3.432E+00 1.750E+00 3.847E+00 1.241E+00 3.905E+00 1.237E+00 4.262E+00 1.026E+00 4.268E+00 9.819E-01 4.684E+00 8.656E-01 5.098E+00 8.300E-01 5.531E+00 7.724E-01 5.837E+00 8.024E-01 5.945E+00 7.514E-01 6.197E+00 7.520E-01 6.323E+00 7.596E-01 6.593E+00 7.456E-01 6.737E+00 7.533E-01 6.954E+00 7.098E-01 7.169E+00 7.617E-01 7.313E+00 7.693E-01 7.564E+00 8.286E-01 7.690E+00 8.142E-01 7.959E+00 8.515E-01 8.050E+00 8.004E-01 8.355E+00 8.231E-01 8.446E+00 8.160E-01 8.752E+00 8.094E-01 8.788E+00 7.802E-01 9.130E+00 8.058E-01 9.148E+00 7.664E-01 9.509E+00 7.086E-01 9.544E+00 7.527E-01 9.887E+00 7.096E-01 9.896E+00 7.391E-01 1.025E+01 7.471E-01 1.032E+01 7.253E-01 1.061E+01 6.966E-01 1.073E+01 7.262E-01 1.095E+01 6.828E-01 1.109E+01 7.271E-01 1.133E+01 6.617E-01 1.149E+01 6.914E-01 1.167E+01 6.552E-01 1.190E+01 6.265E-01 1.205E+01 6.268E-01 1.226E+01 6.200E-01 1.239E+01 6.350E-01 1.262E+01 6.462E-01 1.275E+01 6.212E-01 1.311E+01 6.220E-01 1.343E+01 6.228E-01 1.379E+01 6.017E-01 1.412E+01 6.245E-01 1.448E+01 6.180E-01 1.484E+01 5.969E-01 1.518E+01 6.197E-01 1.548E+01 5.984E-01 \END; /*===================================================================*/ |