|
| /*===================================================================*/
/* NRDF D0785 Data No.5 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,5;
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,5;
/* 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=115IN(P,D)114IN;
PHQ=DBL-DIFF-XSECTN;
ENR=>94%;
THK-TGT=1.5[4.0MG/CM**2;
BAC=SELF;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,5;
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)
-3.064E-01 3.072E-02
7.630E-02 1.766E+00
5.724E-01 5.636E+00
9.953E-01 9.037E+00
1.415E+00 3.998E+00
1.842E+00 1.784E+00
2.268E+00 1.242E+00
2.273E+00 1.236E+00
2.719E+00 9.749E-01
2.723E+00 9.783E-01
3.115E+00 8.885E-01
3.119E+00 8.294E-01
3.566E+00 7.804E-01
3.998E+00 8.166E-01
4.412E+00 1.084E+00
4.826E+00 1.502E+00
5.184E+00 1.702E+00
5.546E+00 1.719E+00
5.690E+00 1.675E+00
5.890E+00 1.556E+00
6.079E+00 1.412E+00
6.286E+00 1.308E+00
6.503E+00 1.237E+00
6.664E+00 1.178E+00
6.930E+00 1.164E+00
7.017E+00 1.104E+00
7.349E+00 1.113E+00
7.400E+00 1.037E+00
7.764E+00 1.027E+00
7.783E+00 9.695E-01
8.160E+00 9.549E-01
8.160E+00 9.332E-01
8.521E+00 9.261E-01
8.575E+00 9.189E-01
8.889E+00 8.760E-01
8.963E+00 8.876E-01
9.242E+00 8.254E-01
9.386E+00 8.399E-01
9.656E+00 7.967E-01
9.782E+00 7.967E-01
1.002E+01 7.751E-01
1.018E+01 7.824E-01
1.038E+01 7.320E-01
1.058E+01 7.393E-01
1.073E+01 7.080E-01
1.099E+01 7.177E-01
1.110E+01 6.888E-01
1.137E+01 6.890E-01
1.146E+01 6.818E-01
1.175E+01 6.963E-01
1.182E+01 6.563E-01
1.214E+01 7.037E-01
1.219E+01 6.789E-01
1.254E+01 6.821E-01
1.290E+01 6.534E-01
1.328E+01 6.391E-01
1.360E+01 6.608E-01
1.396E+01 6.465E-01
1.432E+01 6.683E-01
1.467E+01 6.611E-01
1.503E+01 6.468E-01
1.537E+01 6.469E-01
1.571E+01 6.470E-01
1.605E+01 6.255E-01
1.636E+01 6.400E-01
\END;
/*===================================================================*/
|