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| /*===================================================================*/
/* NRDF D1426 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
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,2;
/* 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=94MO(P,T)92MO;
PHQ=VCTR-ANALPW;
INC-ENGY-LAB-RANGE=22.0MEV;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
INC-ENGY-LAB=22.0MEV;
EXC-ENGY=0MEV;
J-PTY=0+;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC AY
(DEG) (NODIM)
4.973E+00 4.120E-02
1.016E+01 9.182E-02
1.531E+01 2.019E-01
1.890E+01 5.717E-01
1.913E+01 3.025E-01
2.048E+01 2.015E-01
2.298E+01 7.403E-02
2.516E+01 7.955E-02
3.062E+01 1.132E-01
3.607E+01 5.622E-02
4.055E+01 -1.250E-01
4.582E+01 -4.142E-01
5.097E+01 -5.900E-01
5.572E+01 1.512E-01
6.127E+01 2.382E-01
6.605E+01 -3.623E-02
7.120E+01 -2.969E-01
\END;
/*===================================================================*/
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