|
| /*===================================================================*/
/* NRDF D0785 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
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,2;
/* 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=98MO(P,D)97MO;
PHQ=DBL-DIFF-XSECTN;
ENR=>94%;
THK-TGT=1.5[4.0MG/CM**2;
BAC=SELF;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
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)
-3.733E-01 7.989E-02
-1.214E-01 7.321E+00
2.777E-02 7.484E+00
3.062E-01 5.660E-01
4.891E-01 2.046E+00
4.929E-01 2.055E+00
7.541E-01 1.960E+00
7.743E-01 1.923E+00
9.194E-01 1.135E+00
9.213E-01 1.050E+00
1.204E+00 1.708E+00
1.354E+00 1.905E+00
1.617E+00 1.016E+00
1.783E+00 9.988E-01
2.066E+00 1.673E+00
2.184E+00 2.067E+00
2.483E+00 3.105E+00
2.648E+00 2.808E+00
2.928E+00 1.852E+00
3.062E+00 2.725E+00
3.346E+00 3.514E+00
3.496E+00 4.024E+00
3.793E+00 3.332E+00
3.907E+00 2.558E+00
4.221E+00 2.310E+00
4.337E+00 2.178E+00
4.634E+00 1.717E+00
4.766E+00 1.585E+00
5.048E+00 1.716E+00
5.197E+00 1.518E+00
5.511E+00 1.451E+00
5.610E+00 1.402E+00
5.925E+00 1.286E+00
6.024E+00 1.285E+00
6.355E+00 1.186E+00
6.438E+00 1.120E+00
6.753E+00 1.086E+00
6.852E+00 1.069E+00
7.167E+00 1.003E+00
7.266E+00 1.003E+00
7.597E+00 9.854E-01
7.697E+00 9.687E-01
7.978E+00 8.927E-01
8.082E+00 8.770E-01
8.406E+00 8.748E-01
8.495E+00 8.592E-01
8.840E+00 9.002E-01
8.893E+00 8.415E-01
9.204E+00 8.336E-01
9.287E+00 8.004E-01
9.616E+00 7.320E-01
9.734E+00 7.829E-01
1.004E+01 7.887E-01
1.013E+01 7.656E-01
1.046E+01 6.989E-01
1.050E+01 7.318E-01
1.083E+01 6.981E-01
1.124E+01 6.972E-01
1.162E+01 7.292E-01
1.202E+01 7.283E-01
1.242E+01 6.780E-01
1.280E+01 7.594E-01
1.318E+01 6.927E-01
\END;
/*===================================================================*/
|