|
| /*===================================================================*/
/* NRDF D0785 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
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,3;
/* 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=112CD(P,D)111CD;
PHQ=DBL-DIFF-XSECTN;
ENR=>94%;
THK-TGT=1.5[4.0MG/CM**2;
BAC=SELF;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,3;
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)
-2.789E-01 6.434E-02
1.316E-01 1.786E+00
5.573E-01 1.086E+01
1.002E+00 2.514E+00
1.396E+00 2.580E+00
1.821E+00 1.721E+00
1.824E+00 1.786E+00
2.234E+00 1.322E+00
2.249E+00 1.251E+00
2.660E+00 8.473E-01
2.678E+00 8.589E-01
3.071E+00 8.341E-01
3.513E+00 1.642E+00
3.907E+00 1.920E+00
4.335E+00 1.523E+00
4.762E+00 1.443E+00
5.173E+00 1.529E+00
5.600E+00 1.298E+00
5.699E+00 1.351E+00
6.011E+00 1.205E+00
6.077E+00 1.225E+00
6.389E+00 1.119E+00
6.471E+00 1.106E+00
6.800E+00 1.053E+00
6.800E+00 1.039E+00
7.162E+00 9.996E-01
7.227E+00 1.013E+00
7.556E+00 9.599E-01
7.638E+00 1.019E+00
7.934E+00 9.135E-01
8.032E+00 9.268E-01
8.262E+00 8.672E-01
8.427E+00 9.003E-01
8.640E+00 8.275E-01
8.837E+00 8.672E-01
9.002E+00 7.679E-01
9.215E+00 8.010E-01
9.347E+00 7.281E-01
9.626E+00 7.348E-01
9.741E+00 7.215E-01
1.000E+01 7.414E-01
1.010E+01 7.149E-01
1.040E+01 7.149E-01
1.046E+01 6.752E-01
1.079E+01 6.487E-01
1.081E+01 6.288E-01
1.117E+01 6.619E-01
1.119E+01 6.288E-01
1.152E+01 5.957E-01
1.155E+01 6.421E-01
1.189E+01 6.023E-01
1.194E+01 6.354E-01
1.222E+01 5.891E-01
1.262E+01 5.759E-01
1.291E+01 5.891E-01
1.329E+01 5.891E-01
1.363E+01 6.023E-01
1.398E+01 5.957E-01
1.434E+01 6.023E-01
1.467E+01 5.957E-01
1.500E+01 5.891E-01
1.536E+01 6.023E-01
1.570E+01 6.023E-01
\END;
/*===================================================================*/
|