/*===================================================================*/ /* NRDF D0785 Data No.6 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,6; 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,6; /* 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=124SN(P,D)123SN; PHQ=DBL-DIFF-XSECTN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,6; 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) -3.774E-01 6.615E-02 4.723E-03 1.444E+01 4.692E-01 6.020E-01 8.817E-01 1.627E+00 1.079E+00 1.022E+01 1.311E+00 1.131E+01 1.506E+00 4.536E+00 1.767E+00 1.154E+00 1.946E+00 1.449E+00 2.172E+00 1.329E+00 2.199E+00 1.387E+00 2.362E+00 1.320E+00 2.613E+00 9.699E-01 2.633E+00 1.114E+00 3.046E+00 9.714E-01 3.483E+00 7.927E-01 3.918E+00 6.932E-01 4.347E+00 8.824E-01 4.761E+00 9.200E-01 5.204E+00 1.261E+00 5.614E+00 1.457E+00 6.049E+00 1.372E+00 6.446E+00 1.388E+00 6.901E+00 1.216E+00 6.991E+00 1.231E+00 7.301E+00 1.088E+00 7.372E+00 1.117E+00 7.716E+00 1.082E+00 7.735E+00 1.032E+00 8.113E+00 1.055E+00 8.114E+00 1.026E+00 8.474E+00 1.027E+00 8.565E+00 9.988E-01 8.854E+00 9.782E-01 8.944E+00 1.007E+00 9.216E+00 9.218E-01 9.378E+00 9.368E-01 9.596E+00 8.871E-01 9.777E+00 8.444E-01 9.939E+00 8.955E-01 1.019E+01 8.243E-01 1.032E+01 8.176E-01 1.057E+01 8.113E-01 1.068E+01 7.972E-01 1.099E+01 7.551E-01 1.106E+01 7.842E-01 1.137E+01 7.420E-01 1.142E+01 7.927E-01 1.176E+01 7.579E-01 1.178E+01 7.291E-01 1.211E+01 7.014E-01 1.214E+01 7.448E-01 1.249E+01 6.956E-01 1.256E+01 7.247E-01 1.287E+01 6.898E-01 1.294E+01 6.972E-01 1.317E+01 6.909E-01 1.330E+01 7.058E-01 1.355E+01 7.211E-01 1.391E+01 7.008E-01 1.425E+01 7.020E-01 1.461E+01 7.033E-01 1.498E+01 6.974E-01 1.530E+01 7.203E-01 1.564E+01 7.071E-01 1.599E+01 6.939E-01 1.631E+01 6.879E-01 1.665E+01 7.036E-01 \END; /*===================================================================*/ |