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| /*===================================================================*/
/* NRDF D0785 Data No.18 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,18;
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,18;
/* 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=100MO(P,D)99MO;
PHQ=ANGL-DSTRN;
ENR=>94%;
THK-TGT=1.5[4.0MG/CM**2;
BAC=SELF;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,18;
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'8'
(MEV) (DEG) (MB/SR) (MB/SR) (NODIM)
0.0 4.864E+00 7.116E-01 +-1.410E-01 7
0.0 8.182E+00 1.478E-01 +-2.191E-02 7
0.0 1.108E+01 3.359E-01 +-5.850E-02 7
0.0 1.420E+01 3.664E-01 +-7.642E-02 7
0.0 1.734E+01 3.672E-01 +-7.274E-02 7
0.0 2.024E+01 2.456E-01 +-4.865E-02 7
0.0 2.351E+01 7.641E-02 +-1.263E-02 7
0.0 2.667E+01 6.256E-02 +-1.004E-02 7
0.0 3.061E+01 9.597E-02 +-1.501E-02 7
0.0 3.460E+01 9.319E-02 +-1.846E-02 7
0.0 3.882E+01 4.535E-02 +-7.899E-03 7
0.0 4.281E+01 1.297E-02 +-2.484E-03 7
0.0 4.687E+01 2.540E-02 +-5.032E-03 7
0.0 5.084E+01 2.924E-02 +-5.056E-03 7
0.0 5.498E+01 2.810E-02 +-5.923E-03 7
0.10 5.286E+00 1.229E+01 +-NEGLIGIBLE 8
0.10 8.284E+00 1.071E+01 +-NEGLIGIBLE 8
0.10 1.138E+01 8.220E+00 +-NEGLIGIBLE 8
0.10 1.429E+01 4.587E+00 +-NEGLIGIBLE 8
0.10 1.772E+01 2.788E+00 +-NEGLIGIBLE 8
0.10 2.072E+01 2.672E+00 +-NEGLIGIBLE 8
0.10 2.386E+01 2.759E+00 +-NEGLIGIBLE 8
0.10 2.685E+01 2.429E+00 +-NEGLIGIBLE 8
0.10 3.071E+01 1.105E+00 +-NEGLIGIBLE 8
0.10 3.487E+01 5.338E-01 +-NEGLIGIBLE 8
0.10 3.896E+01 4.674E-01 +-NEGLIGIBLE 8
0.10 4.283E+01 4.366E-01 +-2.590E-02 8
0.10 4.686E+01 3.012E-01 +-1.856E-02 8
0.10 5.087E+01 1.664E-01 +-1.190E-02 8
0.10 5.487E+01 1.149E-01 +-8.843E-03 8
0.24 5.058E+00 1.982E+00 +-3.168E-01 9
0.24 8.193E+00 2.255E+00 +-3.057E-01 9
0.24 1.179E+01 1.827E+00 +-2.182E-01 9
0.24 1.424E+01 1.602E+00 +-1.983E-01 9
0.24 1.746E+01 1.207E+00 +-9.120E-02 9
0.24 2.048E+01 8.046E-01 +-7.332E-02 9
0.24 2.349E+01 5.366E-01 +-5.319E-02 9
0.24 2.665E+01 4.087E-01 +-4.572E-02 9
0.24 3.069E+01 2.709E-01 +-3.028E-02 9
0.24 3.485E+01 2.291E-01 +-2.027E-02 9
0.24 3.887E+01 1.818E-01 +-1.608E-02 9
0.24 4.277E+01 1.205E-01 +-1.066E-02 9
0.24 4.678E+01 1.086E-01 +-9.877E-03 9
0.24 5.094E+01 9.481E-02 +-8.623E-03 9
0.24 5.569E+01 6.770E-02 +-5.989E-03 9
\END;
/*===================================================================*/
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