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| /*===================================================================*/
/* NRDF D0021 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
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,2;
/* 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=VCTR-ANALPW;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
INC-ENGY-LAB=22.0MEV;
DELTA-THTL=1.5DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY'7' THTC AY DELTA-AY FLAG'8'
(KEV) (DEG) (NODIM) (NODIM) (NODIM)
0.0 1.517E+01 1.639E-02 +-2.526E-02 3.
0.0 1.992E+01 3.702E-01 +-4.106E-02 3.
0.0 2.500E+01 1.808E-01 +-3.158E-02 3.
0.0 3.009E+01 9.255E-02 +-1.895E-02 3.
0.0 3.532E+01 -1.785E-02 +-2.843E-02 3.
0.0 4.011E+01 -2.641E-01 +-2.838E-02 3.
0.0 4.505E+01 -5.924E-01 +-2.839E-02 3.
0.0 4.993E+01 1.815E-01 +-3.790E-02 3.
0.0 5.469E+01 2.226E-01 +-NEGLIGIBLE 3.
433.938 1.525E+01 2.778E-02 +-1.878E-02 4.
433.938 2.049E+01 1.128E-03 +-2.035E-02 4.
433.938 2.541E+01 -8.030E-02 +-3.600E-02 4.
433.938 3.065E+01 -1.069E-01 +-3.130E-02 4.
433.938 3.574E+01 -4.594E-02 +-2.348E-02 4.
433.938 4.068E+01 4.793E-02 +-1.565E-02 4.
433.938 4.592E+01 8.759E-03 +-2.191E-02 4.
433.938 5.100E+01 -1.024E-01 +-2.348E-02 4.
433.938 5.577E+01 -2.057E-01 +-5.478E-02 4.
\END;
/*===================================================================*/
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