/*===================================================================*/ /* NRDF D0785 Data No.4 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,4; 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,4; /* 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=116CD(P,D)115CD; PHQ=DBL-DIFF-XSECTN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,4; 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) -2.968E-01 1.539E-02 2.292E-01 6.908E+00 6.295E-01 7.329E+00 1.031E+00 2.969E+00 1.476E+00 2.525E+00 1.919E+00 1.883E+00 2.347E+00 1.439E+00 2.387E+00 1.503E+00 2.759E+00 1.130E+00 2.809E+00 1.255E+00 3.232E+00 1.014E+00 3.668E+00 1.191E+00 4.108E+00 1.454E+00 4.558E+00 1.531E+00 4.986E+00 1.463E+00 5.413E+00 1.341E+00 5.757E+00 1.233E+00 5.841E+00 1.259E+00 6.170E+00 1.191E+00 6.254E+00 1.217E+00 6.532E+00 1.136E+00 6.682E+00 1.142E+00 6.928E+00 1.067E+00 7.093E+00 1.053E+00 7.290E+00 1.012E+00 7.506E+00 1.024E+00 7.653E+00 9.570E-01 7.918E+00 9.556E-01 8.050E+00 9.483E-01 8.347E+00 9.069E-01 8.431E+00 9.263E-01 8.745E+00 9.048E-01 8.795E+00 9.244E-01 9.140E+00 8.362E-01 9.189E+00 8.094E-01 9.535E+00 7.744E-01 9.569E+00 8.008E-01 9.932E+00 7.457E-01 9.967E+00 8.053E-01 1.030E+01 7.039E-01 1.038E+01 7.300E-01 1.066E+01 7.086E-01 1.077E+01 6.682E-01 1.102E+01 6.602E-01 1.139E+01 6.583E-01 1.175E+01 6.431E-01 1.213E+01 6.278E-01 1.248E+01 6.259E-01 1.286E+01 6.040E-01 1.321E+01 5.888E-01 1.357E+01 5.935E-01 1.394E+01 5.783E-01 1.427E+01 5.832E-01 1.465E+01 5.745E-01 \END; /*===================================================================*/ |