/*===================================================================*/ /* NRDF D0785 Data No.19 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,19; 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,19; /* 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=142ND(P,D)141ND; PHQ=ANGL-DSTRN; ENR=>94%; THK-TGT=1.5[4.0MG/CM**2; BAC=SELF; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,19; 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. */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA FLAG'9' (MEV) (DEG) (MB/SR) (MB/SR) (NODIM) 0.0 5.799E+00 1.042E+01 +-X 10 0.0 8.529E+00 8.901E+00 +-X 10 0.0 1.142E+01 5.842E+00 +-X 10 0.0 1.433E+01 3.204E+00 +-X 10 0.0 1.750E+01 2.313E+00 +-X 10 0.0 2.064E+01 2.629E+00 +-X 10 0.0 2.364E+01 2.688E+00 +-X 10 0.0 2.667E+01 1.821E+00 +-X 10 0.0 3.060E+01 7.921E-01 +-X 10 0.0 3.476E+01 6.844E-01 +-X 10 0.0 3.876E+01 7.303E-01 +-X 10 0.0 4.267E+01 4.050E-01 +-X 10 0.0 4.659E+01 1.725E-01 +-X 10 0.0 5.060E+01 1.765E-01 +-X 10 0.0 5.460E+01 1.824E-01 +-X 10 0.0 5.864E+01 1.173E-01 +-X 10 0.0 6.271E+01 4.943E-02 +-X 10 0.19 5.666E+00 1.663E+00 +-X 11 0.19 8.306E+00 6.465E-01 +-X 11 0.19 1.109E+01 2.220E+00 +-X 11 0.19 1.436E+01 3.400E+00 +-X 11 0.19 1.739E+01 2.694E+00 +-X 11 0.19 2.002E+01 1.058E+00 +-X 11 0.19 2.296E+01 3.363E-01 +-X 11 0.19 2.622E+01 6.437E-01 +-X 11 0.19 3.049E+01 9.155E-01 +-X 11 0.19 3.440E+01 5.220E-01 +-X 11 0.19 3.864E+01 1.492E-01 +-X 11 0.19 4.249E+01 1.969E-01 +-X 11 0.19 4.633E+01 2.800E-01 +-X 11 0.19 5.025E+01 1.237E-01 +-X 11 0.19 5.441E+01 3.283E-02 +-X 11 0.19 5.839E+01 3.914E-02 +-X 11 0.19 6.248E+01 6.012E-02 +-X 11 0.76 5.742E+00 2.053E+00 +-X 12 0.76 8.291E+00 2.769E+00 +-X 12 0.76 1.113E+01 3.394E+00 +-X 12 0.76 1.428E+01 3.435E+00 +-X 12 0.76 1.728E+01 3.403E+00 +-X 12 0.76 2.029E+01 3.266E+00 +-X 12 0.76 2.345E+01 2.588E+00 +-X 12 0.76 2.662E+01 1.965E+00 +-X 12 0.76 3.039E+01 1.051E+00 +-X 12 0.76 3.457E+01 7.330E-01 +-X 12 0.76 3.858E+01 6.963E-01 +-X 12 0.76 4.232E+01 5.345E-01 +-X 12 0.76 4.664E+01 3.612E-01 +-X 12 0.76 5.066E+01 2.864E-01 +-X 12 0.76 5.467E+01 2.779E-01 +-X 12 0.76 5.869E+01 2.250E-01 +-X 12 0.76 6.273E+01 1.473E-01 +-X 12 1.56 5.592E+00 6.036E-01 +-NEGLIGIBLE 13 1.56 8.039E+00 5.669E-01 +-NEGLIGIBLE 13 1.56 1.108E+01 4.214E-01 +-NEGLIGIBLE 13 1.56 1.414E+01 2.586E-01 +-NEGLIGIBLE 13 1.56 1.732E+01 1.943E-01 +-NEGLIGIBLE 13 1.56 2.037E+01 1.940E-01 +-NEGLIGIBLE 13 1.56 2.349E+01 2.144E-01 +-NEGLIGIBLE 13 1.56 2.653E+01 1.594E-01 +-NEGLIGIBLE 13 1.56 3.054E+01 8.126E-02 +-NEGLIGIBLE 13 1.56 3.464E+01 7.278E-02 +-NEGLIGIBLE 13 1.56 3.866E+01 7.062E-02 +-NEGLIGIBLE 13 1.56 4.286E+01 4.722E-02 +-NEGLIGIBLE 13 1.56 4.666E+01 2.343E-02 +-1.545E-03 13 1.56 5.069E+01 2.156E-02 +-1.548E-03 13 1.56 5.471E+01 2.206E-02 +-1.801E-03 13 1.56 5.861E+01 1.539E-02 +-1.105E-03 13 1.56 6.269E+01 7.886E-03 +-7.928E-04 13 \END; /*===================================================================*/ |