/*===================================================================*/ /* NRDF D1426 Data No.1 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,1; 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,1; /* 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=92ZR(P,T)90ZR; PHQ=VCTR-ANALPW; INC-ENGY-LAB-RANGE=22.0MEV; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,1; INC-ENGY-LAB=22.0MEV; EXC-ENGY=0MEV; J-PTY=0+; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC AY (DEG) (NODIM) 4.909E+00 4.444E-02 9.545E+00 9.444E-02 1.261E+01 1.205E-01 1.520E+01 1.261E-01 1.831E+01 -1.167E-02 2.018E+01 -4.889E-01 2.155E+01 -5.056E-01 2.260E+01 -1.019E-01 2.536E+01 1.278E-01 2.759E+01 1.840E-01 3.075E+01 1.775E-01 3.533E+01 8.728E-02 4.064E+01 -10.000E-02 4.609E+01 -5.000E-01 5.127E+01 -5.278E-01 5.645E+01 1.667E-02 6.109E+01 2.389E-01 6.627E+01 3.333E-02 \END; /*===================================================================*/ |