/*===================================================================*/ /* NRDF D0785 Data No.7 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,7; 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,7; /* 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=130TE(P,D)129TE; PHQ=DBL-DIFF-XSECTN; ENR=99.5%; THK-TGT=2.09MG/CM**2; BAC=MYLAR'5'; /* '5' 4 micro-meter thick */ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,7; 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) -4.137E-01 -1.450E-03 2.839E-02 1.424E+01 4.599E-01 4.565E+00 5.677E-01 4.641E+00 8.945E-01 3.060E+00 9.653E-01 3.713E+00 1.341E+00 5.169E+00 1.396E+00 4.665E+00 1.756E+00 4.459E+00 1.828E+00 4.316E+00 2.157E+00 1.434E+00 2.247E+00 1.437E+00 2.615E+00 1.721E+00 2.624E+00 1.809E+00 2.648E+00 1.880E+00 2.678E+00 1.883E+00 3.037E+00 1.252E+00 3.075E+00 1.316E+00 3.092E+00 1.209E+00 3.468E+00 1.289E+00 3.504E+00 1.318E+00 3.507E+00 1.329E+00 3.908E+00 8.714E-01 3.922E+00 1.052E+00 3.925E+00 9.004E-01 4.322E+00 8.582E-01 4.340E+00 8.727E-01 4.754E+00 8.378E-01 4.773E+00 8.089E-01 5.185E+00 9.258E-01 5.185E+00 8.824E-01 5.578E+00 1.050E+00 5.597E+00 1.021E+00 6.007E+00 1.210E+00 6.025E+00 1.246E+00 6.440E+00 1.168E+00 6.457E+00 1.211E+00 6.836E+00 1.147E+00 6.873E+00 1.126E+00 7.234E+00 1.069E+00 7.270E+00 1.040E+00 7.666E+00 1.056E+00 7.685E+00 9.981E-01 8.062E+00 1.035E+00 8.116E+00 1.014E+00 8.476E+00 1.037E+00 8.513E+00 1.001E+00 8.891E+00 9.655E-01 8.928E+00 9.439E-01 9.270E+00 9.377E-01 9.341E+00 9.596E-01 9.667E+00 8.594E-01 9.739E+00 8.740E-01 1.008E+01 8.461E-01 1.013E+01 8.607E-01 1.048E+01 8.545E-01 1.055E+01 8.258E-01 1.087E+01 8.123E-01 1.093E+01 7.691E-01 1.125E+01 7.989E-01 1.134E+01 7.775E-01 1.165E+01 7.856E-01 1.174E+01 8.148E-01 1.203E+01 7.651E-01 1.212E+01 7.870E-01 1.240E+01 7.734E-01 1.249E+01 7.737E-01 1.284E+01 7.674E-01 1.291E+01 7.749E-01 1.318E+01 7.323E-01 1.327E+01 7.687E-01 1.393E+01 7.489E-01 1.404E+01 7.276E-01 1.429E+01 7.355E-01 1.442E+01 7.431E-01 1.467E+01 7.294E-01 \END; /*===================================================================*/ |