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| /*===================================================================*/
/* NRDF D0021 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
D#=D21;
TITLE=/ Difference in analyzing powers for (p,t) reactions due to a
phase change of interference between direct and indirect
processes in two-nucleon transfer reactions /;
ATH=(K.YAGI'1', S.KUNORI'1', Y.AOKI'1', Y.HIGASHI'1', J.SANADA'1',
Y.TAGISHI'1');
INST-ATH=(2JPNTSU'1');
/* '1' Institute of Physics and Tandem Accelerator Center */
REF=PRL;
VLP=40(1978)161;
RCTS=(128TE(P,T)126TE, 110PD(P,T)108PD);
PHQS=(VCTR-ANALPW, ANGL-DSTRN);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,4;
/* 2009-08-21 : Compiled+Checked, Nh */
/* Related references
- R.B.Firestone et al., FIRESTONE, (1996).
(Level energies of 1st 2+ states are not given in K.Yagi et al.
J.PRL,40,161,1978, and taken from this book by compiler.)
ENR=X%'2';
/* '2' Enriched sample */
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=0.5MG/CM**2;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=VDG'3';
/* '3' 12UD Pelletron */
INST-ACC=2JPNTSU'4';
/* '4' 12UD Pelletron */
INC-ENGY-LAB-RANGE=22.0MEV;
BEAM-INTNSTY=50NA;
POL-PRJ=85+-2%;
ION-SOURCE=/ Lamb-shift source /;
DET-PARTCL=T;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG,SI);
ERS-DET=40KEV;
ANL=(CCBA,RPA);
RCT=110PD(P,T)108PD;
PHQ=ANGL-DSTRN;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,4;
INC-ENGY-LAB=22.0MEV;
EXC-ENGY=433.938KEV;
J-PTY=2+;
DELTA-THTL=1.5DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (UB/SR) (UB/SR)
5.188E+00 7.792E+01 +-5.658E+00
1.004E+01 2.445E+02 +-2.180E+01
1.533E+01 3.895E+02 +-2.826E+01
2.076E+01 4.077E+02 +-2.757E+01
2.571E+01 2.706E+02 +-2.306E+01
3.064E+01 1.341E+02 +-1.197E+01
3.605E+01 9.775E+01 +-8.326E+00
4.086E+01 1.035E+02 +-1.014E+01
4.644E+01 9.416E+01 +-7.397E+00
5.124E+01 6.943E+01 +-6.193E+00
5.664E+01 4.149E+01 +-5.423E+00
6.237E+01 3.167E+01 +-4.141E+00
\END;
/*===================================================================*/
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