/*===================================================================*/
 /* NRDF D1426 Data No.16                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,16;
 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                                           */
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 \\EXP,16;
 /* 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=98MO(P,T)96MO;
 PHQ=ANGL-DSTRN;
 INC-ENGY-LAB-RANGE=22.0MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,16;
 INC-ENGY-LAB=22.0MEV;
 EXC-ENGY=0MEV;
 J-PTY=0+;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA
 (DEG) (UB/SR)
 5.134E+00 4.676E+03
 1.039E+01 2.204E+03
 1.299E+01 1.124E+03
 1.515E+01 4.471E+02
 1.785E+01 7.530E+01
 2.023E+01 3.392E+01
 2.152E+01 6.428E+01
 2.282E+01 1.277E+02
 2.556E+01 2.614E+02
 2.827E+01 3.916E+02
 3.095E+01 4.715E+02
 3.589E+01 5.327E+02
 4.080E+01 4.544E+02
 4.587E+01 2.665E+02
 5.089E+01 8.908E+01
 5.331E+01 5.928E+01
 5.598E+01 6.300E+01
 6.098E+01 1.329E+02
 6.635E+01 1.868E+02
 \END;
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