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| /*===================================================================*/
/* NRDF D0021 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
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,1;
/* 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=128TE(P,T)126TE;
PHQ=VCTR-ANALPW;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-ENGY-LAB=22.0MEV;
DELTA-THTL=1.5DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY'5' THTC AY DELTA-AY FLAG'6'
(KEV) (DEG) (NODIM) (NODIM) (NODIM)
0.0 1.502E+01 -5.719E-03 +-3.158E-02 1.
0.0 2.024E+01 4.494E-02 +-5.369E-02 1.
0.0 2.501E+01 1.619E-01 +-3.158E-02 1.
0.0 3.008E+01 1.336E-01 +-3.158E-02 1.
0.0 3.517E+01 2.004E-02 +-3.158E-02 1.
0.0 4.025E+01 -1.567E-01 +-3.474E-02 1.
0.0 4.519E+01 -4.250E-01 +-4.105E-02 1.
0.0 5.011E+01 -3.554E-01 +-4.736E-02 1.
666.338 1.525E+01 7.317E-02 +-3.913E-02 2.
666.338 2.049E+01 9.973E-02 +-4.226E-02 2.
666.338 2.527E+01 1.200E-01 +-4.696E-02 2.
666.338 2.989E+01 4.175E-02 +-3.443E-02 2.
666.338 3.544E+01 3.701E-02 +-4.852E-02 2.
666.338 4.068E+01 1.506E-02 +-4.539E-02 2.
666.338 4.576E+01 -8.045E-02 +-5.635E-02 2.
666.338 5.069E+01 -5.858E-02 +-4.383E-02 2.
\END;
/*===================================================================*/
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