|
| /*===================================================================*/
/* NRDF D0785 Data No.8 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,8;
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,8;
/* 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=141PR(P,D)140PR;
PHQ=DBL-DIFF-XSECTN;
ENR=>94%;
THK-TGT=1.5[4.0MG/CM**2;
BAC=SELF;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,8;
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)
-3.421E-01 1.727E-02
7.947E-02 3.618E+00
4.912E-01 4.357E+00
9.170E-01 6.490E+00
1.358E+00 3.156E+00
1.755E+00 3.014E+00
2.168E+00 3.276E+00
2.601E+00 2.951E+00
3.017E+00 2.039E+00
3.432E+00 1.750E+00
3.847E+00 1.241E+00
3.905E+00 1.237E+00
4.262E+00 1.026E+00
4.268E+00 9.819E-01
4.684E+00 8.656E-01
5.098E+00 8.300E-01
5.531E+00 7.724E-01
5.837E+00 8.024E-01
5.945E+00 7.514E-01
6.197E+00 7.520E-01
6.323E+00 7.596E-01
6.593E+00 7.456E-01
6.737E+00 7.533E-01
6.954E+00 7.098E-01
7.169E+00 7.617E-01
7.313E+00 7.693E-01
7.564E+00 8.286E-01
7.690E+00 8.142E-01
7.959E+00 8.515E-01
8.050E+00 8.004E-01
8.355E+00 8.231E-01
8.446E+00 8.160E-01
8.752E+00 8.094E-01
8.788E+00 7.802E-01
9.130E+00 8.058E-01
9.148E+00 7.664E-01
9.509E+00 7.086E-01
9.544E+00 7.527E-01
9.887E+00 7.096E-01
9.896E+00 7.391E-01
1.025E+01 7.471E-01
1.032E+01 7.253E-01
1.061E+01 6.966E-01
1.073E+01 7.262E-01
1.095E+01 6.828E-01
1.109E+01 7.271E-01
1.133E+01 6.617E-01
1.149E+01 6.914E-01
1.167E+01 6.552E-01
1.190E+01 6.265E-01
1.205E+01 6.268E-01
1.226E+01 6.200E-01
1.239E+01 6.350E-01
1.262E+01 6.462E-01
1.275E+01 6.212E-01
1.311E+01 6.220E-01
1.343E+01 6.228E-01
1.379E+01 6.017E-01
1.412E+01 6.245E-01
1.448E+01 6.180E-01
1.484E+01 5.969E-01
1.518E+01 6.197E-01
1.548E+01 5.984E-01
\END;
/*===================================================================*/
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