/*===================================================================*/ /* NRDF D0785 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; 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,3; /* 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=DBL-DIFF-XSECTN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,3; 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) -2.789E-01 6.434E-02 1.316E-01 1.786E+00 5.573E-01 1.086E+01 1.002E+00 2.514E+00 1.396E+00 2.580E+00 1.821E+00 1.721E+00 1.824E+00 1.786E+00 2.234E+00 1.322E+00 2.249E+00 1.251E+00 2.660E+00 8.473E-01 2.678E+00 8.589E-01 3.071E+00 8.341E-01 3.513E+00 1.642E+00 3.907E+00 1.920E+00 4.335E+00 1.523E+00 4.762E+00 1.443E+00 5.173E+00 1.529E+00 5.600E+00 1.298E+00 5.699E+00 1.351E+00 6.011E+00 1.205E+00 6.077E+00 1.225E+00 6.389E+00 1.119E+00 6.471E+00 1.106E+00 6.800E+00 1.053E+00 6.800E+00 1.039E+00 7.162E+00 9.996E-01 7.227E+00 1.013E+00 7.556E+00 9.599E-01 7.638E+00 1.019E+00 7.934E+00 9.135E-01 8.032E+00 9.268E-01 8.262E+00 8.672E-01 8.427E+00 9.003E-01 8.640E+00 8.275E-01 8.837E+00 8.672E-01 9.002E+00 7.679E-01 9.215E+00 8.010E-01 9.347E+00 7.281E-01 9.626E+00 7.348E-01 9.741E+00 7.215E-01 1.000E+01 7.414E-01 1.010E+01 7.149E-01 1.040E+01 7.149E-01 1.046E+01 6.752E-01 1.079E+01 6.487E-01 1.081E+01 6.288E-01 1.117E+01 6.619E-01 1.119E+01 6.288E-01 1.152E+01 5.957E-01 1.155E+01 6.421E-01 1.189E+01 6.023E-01 1.194E+01 6.354E-01 1.222E+01 5.891E-01 1.262E+01 5.759E-01 1.291E+01 5.891E-01 1.329E+01 5.891E-01 1.363E+01 6.023E-01 1.398E+01 5.957E-01 1.434E+01 6.023E-01 1.467E+01 5.957E-01 1.500E+01 5.891E-01 1.536E+01 6.023E-01 1.570E+01 6.023E-01 \END; /*===================================================================*/ |