|
| /*===================================================================*/
/* NRDF D0785 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
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,1;
/* 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=95MO(P,D)94MO;
PHQ=DBL-DIFF-XSECTN;
ENR=>94%;
THK-TGT=1.5[4.0MG/CM**2;
BAC=SELF;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
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)
-3.783E-01 7.524E-04
7.723E-02 1.140E+00
5.048E-01 5.091E-02
9.395E-01 9.118E-01
1.402E+00 1.218E+00
1.858E+00 8.016E-01
2.313E+00 1.018E+00
2.741E+00 4.073E-01
3.173E+00 7.027E-01
3.620E+00 5.697E-01
4.075E+00 1.047E+00
4.504E+00 2.990E+00
4.952E+00 3.285E+00
5.348E+00 2.938E+00
5.811E+00 2.706E+00
6.256E+00 1.831E+00
6.670E+00 1.616E+00
7.099E+00 1.137E+00
7.193E+00 1.253E+00
7.546E+00 1.136E+00
7.553E+00 1.073E+00
7.931E+00 1.108E+00
8.309E+00 9.990E-01
8.406E+00 9.355E-01
8.456E+00 9.848E-01
8.705E+00 9.441E-01
8.787E+00 8.850E-01
9.084E+00 8.534E-01
9.251E+00 8.672E-01
9.449E+00 8.337E-01
9.648E+00 8.496E-01
9.814E+00 8.162E-01
1.006E+01 7.331E-01
1.022E+01 7.964E-01
1.048E+01 7.155E-01
1.058E+01 7.237E-01
1.089E+01 6.320E-01
1.094E+01 6.977E-01
1.125E+01 7.039E-01
1.129E+01 6.638E-01
1.165E+01 6.628E-01
1.172E+01 6.297E-01
1.202E+01 6.480E-01
1.212E+01 6.615E-01
1.240E+01 5.948E-01
1.276E+01 6.459E-01
1.314E+01 6.090E-01
\END;
/*===================================================================*/
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