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| /*===================================================================*/
/* NRDF D0785 Data No.19 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,19;
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,19;
/* 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=142ND(P,D)141ND;
PHQ=ANGL-DSTRN;
ENR=>94%;
THK-TGT=1.5[4.0MG/CM**2;
BAC=SELF;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,19;
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. */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA FLAG'9'
(MEV) (DEG) (MB/SR) (MB/SR) (NODIM)
0.0 5.799E+00 1.042E+01 +-X 10
0.0 8.529E+00 8.901E+00 +-X 10
0.0 1.142E+01 5.842E+00 +-X 10
0.0 1.433E+01 3.204E+00 +-X 10
0.0 1.750E+01 2.313E+00 +-X 10
0.0 2.064E+01 2.629E+00 +-X 10
0.0 2.364E+01 2.688E+00 +-X 10
0.0 2.667E+01 1.821E+00 +-X 10
0.0 3.060E+01 7.921E-01 +-X 10
0.0 3.476E+01 6.844E-01 +-X 10
0.0 3.876E+01 7.303E-01 +-X 10
0.0 4.267E+01 4.050E-01 +-X 10
0.0 4.659E+01 1.725E-01 +-X 10
0.0 5.060E+01 1.765E-01 +-X 10
0.0 5.460E+01 1.824E-01 +-X 10
0.0 5.864E+01 1.173E-01 +-X 10
0.0 6.271E+01 4.943E-02 +-X 10
0.19 5.666E+00 1.663E+00 +-X 11
0.19 8.306E+00 6.465E-01 +-X 11
0.19 1.109E+01 2.220E+00 +-X 11
0.19 1.436E+01 3.400E+00 +-X 11
0.19 1.739E+01 2.694E+00 +-X 11
0.19 2.002E+01 1.058E+00 +-X 11
0.19 2.296E+01 3.363E-01 +-X 11
0.19 2.622E+01 6.437E-01 +-X 11
0.19 3.049E+01 9.155E-01 +-X 11
0.19 3.440E+01 5.220E-01 +-X 11
0.19 3.864E+01 1.492E-01 +-X 11
0.19 4.249E+01 1.969E-01 +-X 11
0.19 4.633E+01 2.800E-01 +-X 11
0.19 5.025E+01 1.237E-01 +-X 11
0.19 5.441E+01 3.283E-02 +-X 11
0.19 5.839E+01 3.914E-02 +-X 11
0.19 6.248E+01 6.012E-02 +-X 11
0.76 5.742E+00 2.053E+00 +-X 12
0.76 8.291E+00 2.769E+00 +-X 12
0.76 1.113E+01 3.394E+00 +-X 12
0.76 1.428E+01 3.435E+00 +-X 12
0.76 1.728E+01 3.403E+00 +-X 12
0.76 2.029E+01 3.266E+00 +-X 12
0.76 2.345E+01 2.588E+00 +-X 12
0.76 2.662E+01 1.965E+00 +-X 12
0.76 3.039E+01 1.051E+00 +-X 12
0.76 3.457E+01 7.330E-01 +-X 12
0.76 3.858E+01 6.963E-01 +-X 12
0.76 4.232E+01 5.345E-01 +-X 12
0.76 4.664E+01 3.612E-01 +-X 12
0.76 5.066E+01 2.864E-01 +-X 12
0.76 5.467E+01 2.779E-01 +-X 12
0.76 5.869E+01 2.250E-01 +-X 12
0.76 6.273E+01 1.473E-01 +-X 12
1.56 5.592E+00 6.036E-01 +-NEGLIGIBLE 13
1.56 8.039E+00 5.669E-01 +-NEGLIGIBLE 13
1.56 1.108E+01 4.214E-01 +-NEGLIGIBLE 13
1.56 1.414E+01 2.586E-01 +-NEGLIGIBLE 13
1.56 1.732E+01 1.943E-01 +-NEGLIGIBLE 13
1.56 2.037E+01 1.940E-01 +-NEGLIGIBLE 13
1.56 2.349E+01 2.144E-01 +-NEGLIGIBLE 13
1.56 2.653E+01 1.594E-01 +-NEGLIGIBLE 13
1.56 3.054E+01 8.126E-02 +-NEGLIGIBLE 13
1.56 3.464E+01 7.278E-02 +-NEGLIGIBLE 13
1.56 3.866E+01 7.062E-02 +-NEGLIGIBLE 13
1.56 4.286E+01 4.722E-02 +-NEGLIGIBLE 13
1.56 4.666E+01 2.343E-02 +-1.545E-03 13
1.56 5.069E+01 2.156E-02 +-1.548E-03 13
1.56 5.471E+01 2.206E-02 +-1.801E-03 13
1.56 5.861E+01 1.539E-02 +-1.105E-03 13
1.56 6.269E+01 7.886E-03 +-7.928E-04 13
\END;
/*===================================================================*/
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