|
| /*===================================================================*/
/* 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;
/*===================================================================*/
|