/*===================================================================*/ /* NRDF D0785 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; 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,2; /* 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=98MO(P,D)97MO; PHQ=DBL-DIFF-XSECTN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,2; 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) -3.733E-01 7.989E-02 -1.214E-01 7.321E+00 2.777E-02 7.484E+00 3.062E-01 5.660E-01 4.891E-01 2.046E+00 4.929E-01 2.055E+00 7.541E-01 1.960E+00 7.743E-01 1.923E+00 9.194E-01 1.135E+00 9.213E-01 1.050E+00 1.204E+00 1.708E+00 1.354E+00 1.905E+00 1.617E+00 1.016E+00 1.783E+00 9.988E-01 2.066E+00 1.673E+00 2.184E+00 2.067E+00 2.483E+00 3.105E+00 2.648E+00 2.808E+00 2.928E+00 1.852E+00 3.062E+00 2.725E+00 3.346E+00 3.514E+00 3.496E+00 4.024E+00 3.793E+00 3.332E+00 3.907E+00 2.558E+00 4.221E+00 2.310E+00 4.337E+00 2.178E+00 4.634E+00 1.717E+00 4.766E+00 1.585E+00 5.048E+00 1.716E+00 5.197E+00 1.518E+00 5.511E+00 1.451E+00 5.610E+00 1.402E+00 5.925E+00 1.286E+00 6.024E+00 1.285E+00 6.355E+00 1.186E+00 6.438E+00 1.120E+00 6.753E+00 1.086E+00 6.852E+00 1.069E+00 7.167E+00 1.003E+00 7.266E+00 1.003E+00 7.597E+00 9.854E-01 7.697E+00 9.687E-01 7.978E+00 8.927E-01 8.082E+00 8.770E-01 8.406E+00 8.748E-01 8.495E+00 8.592E-01 8.840E+00 9.002E-01 8.893E+00 8.415E-01 9.204E+00 8.336E-01 9.287E+00 8.004E-01 9.616E+00 7.320E-01 9.734E+00 7.829E-01 1.004E+01 7.887E-01 1.013E+01 7.656E-01 1.046E+01 6.989E-01 1.050E+01 7.318E-01 1.083E+01 6.981E-01 1.124E+01 6.972E-01 1.162E+01 7.292E-01 1.202E+01 7.283E-01 1.242E+01 6.780E-01 1.280E+01 7.594E-01 1.318E+01 6.927E-01 \END; /*===================================================================*/ |