|
| /*===================================================================*/
/* NRDF D0785 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
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,4;
/* 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=116CD(P,D)115CD;
PHQ=DBL-DIFF-XSECTN;
ENR=>94%;
THK-TGT=1.5[4.0MG/CM**2;
BAC=SELF;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,4;
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)
-2.968E-01 1.539E-02
2.292E-01 6.908E+00
6.295E-01 7.329E+00
1.031E+00 2.969E+00
1.476E+00 2.525E+00
1.919E+00 1.883E+00
2.347E+00 1.439E+00
2.387E+00 1.503E+00
2.759E+00 1.130E+00
2.809E+00 1.255E+00
3.232E+00 1.014E+00
3.668E+00 1.191E+00
4.108E+00 1.454E+00
4.558E+00 1.531E+00
4.986E+00 1.463E+00
5.413E+00 1.341E+00
5.757E+00 1.233E+00
5.841E+00 1.259E+00
6.170E+00 1.191E+00
6.254E+00 1.217E+00
6.532E+00 1.136E+00
6.682E+00 1.142E+00
6.928E+00 1.067E+00
7.093E+00 1.053E+00
7.290E+00 1.012E+00
7.506E+00 1.024E+00
7.653E+00 9.570E-01
7.918E+00 9.556E-01
8.050E+00 9.483E-01
8.347E+00 9.069E-01
8.431E+00 9.263E-01
8.745E+00 9.048E-01
8.795E+00 9.244E-01
9.140E+00 8.362E-01
9.189E+00 8.094E-01
9.535E+00 7.744E-01
9.569E+00 8.008E-01
9.932E+00 7.457E-01
9.967E+00 8.053E-01
1.030E+01 7.039E-01
1.038E+01 7.300E-01
1.066E+01 7.086E-01
1.077E+01 6.682E-01
1.102E+01 6.602E-01
1.139E+01 6.583E-01
1.175E+01 6.431E-01
1.213E+01 6.278E-01
1.248E+01 6.259E-01
1.286E+01 6.040E-01
1.321E+01 5.888E-01
1.357E+01 5.935E-01
1.394E+01 5.783E-01
1.427E+01 5.832E-01
1.465E+01 5.745E-01
\END;
/*===================================================================*/
|