/*===================================================================*/ /* 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; /*===================================================================*/ |