|
| /*===================================================================*/
/* NRDF D0785 Data No.7 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,7;
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,7;
/* 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=130TE(P,D)129TE;
PHQ=DBL-DIFF-XSECTN;
ENR=99.5%;
THK-TGT=2.09MG/CM**2;
BAC=MYLAR'5';
/* '5' 4 micro-meter thick */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,7;
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)
-4.137E-01 -1.450E-03
2.839E-02 1.424E+01
4.599E-01 4.565E+00
5.677E-01 4.641E+00
8.945E-01 3.060E+00
9.653E-01 3.713E+00
1.341E+00 5.169E+00
1.396E+00 4.665E+00
1.756E+00 4.459E+00
1.828E+00 4.316E+00
2.157E+00 1.434E+00
2.247E+00 1.437E+00
2.615E+00 1.721E+00
2.624E+00 1.809E+00
2.648E+00 1.880E+00
2.678E+00 1.883E+00
3.037E+00 1.252E+00
3.075E+00 1.316E+00
3.092E+00 1.209E+00
3.468E+00 1.289E+00
3.504E+00 1.318E+00
3.507E+00 1.329E+00
3.908E+00 8.714E-01
3.922E+00 1.052E+00
3.925E+00 9.004E-01
4.322E+00 8.582E-01
4.340E+00 8.727E-01
4.754E+00 8.378E-01
4.773E+00 8.089E-01
5.185E+00 9.258E-01
5.185E+00 8.824E-01
5.578E+00 1.050E+00
5.597E+00 1.021E+00
6.007E+00 1.210E+00
6.025E+00 1.246E+00
6.440E+00 1.168E+00
6.457E+00 1.211E+00
6.836E+00 1.147E+00
6.873E+00 1.126E+00
7.234E+00 1.069E+00
7.270E+00 1.040E+00
7.666E+00 1.056E+00
7.685E+00 9.981E-01
8.062E+00 1.035E+00
8.116E+00 1.014E+00
8.476E+00 1.037E+00
8.513E+00 1.001E+00
8.891E+00 9.655E-01
8.928E+00 9.439E-01
9.270E+00 9.377E-01
9.341E+00 9.596E-01
9.667E+00 8.594E-01
9.739E+00 8.740E-01
1.008E+01 8.461E-01
1.013E+01 8.607E-01
1.048E+01 8.545E-01
1.055E+01 8.258E-01
1.087E+01 8.123E-01
1.093E+01 7.691E-01
1.125E+01 7.989E-01
1.134E+01 7.775E-01
1.165E+01 7.856E-01
1.174E+01 8.148E-01
1.203E+01 7.651E-01
1.212E+01 7.870E-01
1.240E+01 7.734E-01
1.249E+01 7.737E-01
1.284E+01 7.674E-01
1.291E+01 7.749E-01
1.318E+01 7.323E-01
1.327E+01 7.687E-01
1.393E+01 7.489E-01
1.404E+01 7.276E-01
1.429E+01 7.355E-01
1.442E+01 7.431E-01
1.467E+01 7.294E-01
\END;
/*===================================================================*/
|