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/* NRDF D1426 Data No.23 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,23;
D#=D1426;
TITLE=/ Marked changes in (p,t) analyzing powers for isotopes of Zr,
Mo, Ru, and Pd and strong, sequential, two-step transfer
processes in both (p,t) and (t,p) reactions /;
PURPOSE=/ To investigate whether or not storong sequential
two-steptransfer processes exist in allowed (p,t) and/or
(t,p) reactions and how storong they are when they exist /;
ATH=(Y.AOKI'1', H.IIDA'1', S.KUNORI'1', K.NAGANO'1', Y.TOBA'1',
K.YAGI'1');
INST-ATH=(2JPNTSU'1');
/* '1' Institute of Physics and Tandem Accelerator Center */
REF=PR/C;
VLP=25(1982)1050;
RCTS=(92ZR(P,T)90ZR, 94MO(P,T)92MO, 96MO(P,T)94MO, 98MO(P,T)96MO,
100RU(P,T)98RU, 102RU(P,T)100RU, 104RU(P,T)102RU,
104PD(P,T)102PD, 106PD(P,T)104PD, 108PD(P,T)106PD,
110PD(P,T)108PD, 138BA(P,T)136BA);
PHQS=(VCTR-ANALPW, ANGL-DSTRN);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,23;
/* 2006-04-05 : Converted, N.Otuka. Converted to EXFOR E1426 */
CHM=ELM;
PHYS-FORM=SLD;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=VDGT;
INST-ACC=2JPNTSU;
POL-PRJ=X%;
ION-SOURCE=/ Polarized ion source /;
DET-PARTCL=T;
COINC=NO;
ANT-COINC=NO;
ANL=DWBA;
/* 2006-04-13 : Altered, At. Re-digitized */
RCT=138BA(P,T)136BA;
PHQ=VCTR-ANALPW;
INC-ENGY-LAB-RANGE=18.5MEV;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,23;
INC-ENGY-LAB=18.5MEV;
EXC-ENGY=0MEV;
J-PTY=0+;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC AY DELTA-AY
(DEG) (NODIM) (NODIM)
5.022E+00 -2.494E-02 +-2.604E-02
1.037E+01 -9.629E-02 +-2.604E-02
1.150E+01 -1.538E-01 +-3.125E-02
1.292E+01 -3.989E-01 +-5.729E-02
1.402E+01 2.279E-02 +-5.471E-02
1.549E+01 1.553E-01 +-4.947E-02
1.826E+01 4.279E-02 +-NEGLIGIBLE
2.043E+01 2.935E-02 +-NEGLIGIBLE
2.555E+01 2.306E-03 +-NEGLIGIBLE
3.052E+01 -5.335E-02 +-NEGLIGIBLE
3.574E+01 -1.325E-01 +-NEGLIGIBLE
4.053E+01 -3.053E-01 +-NEGLIGIBLE
\END;
/*===================================================================*/
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