/*===================================================================*/ /* NRDF D0021 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; D#=D21; TITLE=/ Difference in analyzing powers for (p,t) reactions due to a phase change of interference between direct and indirect processes in two-nucleon transfer reactions /; ATH=(K.YAGI'1', S.KUNORI'1', Y.AOKI'1', Y.HIGASHI'1', J.SANADA'1', Y.TAGISHI'1'); INST-ATH=(2JPNTSU'1'); /* '1' Institute of Physics and Tandem Accelerator Center */ REF=PRL; VLP=40(1978)161; RCTS=(128TE(P,T)126TE, 110PD(P,T)108PD); PHQS=(VCTR-ANALPW, ANGL-DSTRN); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,3; /* 2009-08-21 : Compiled+Checked, Nh */ /* Related references - R.B.Firestone et al., FIRESTONE, (1996). (Level energies of 1st 2+ states are not given in K.Yagi et al. J.PRL,40,161,1978, and taken from this book by compiler.) ENR=X%'2'; /* '2' Enriched sample */ CHM=ELM; PHYS-FORM=SLD; THK-TGT=0.5MG/CM**2; POL-TGT=0%; ALGN-TGT=0%; ACC=VDG'3'; /* '3' 12UD Pelletron */ INST-ACC=2JPNTSU'4'; /* '4' 12UD Pelletron */ INC-ENGY-LAB-RANGE=22.0MEV; BEAM-INTNSTY=50NA; POL-PRJ=85+-2%; ION-SOURCE=/ Lamb-shift source /; DET-PARTCL=T; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG,SI); ERS-DET=40KEV; ANL=(CCBA,RPA); RCT=128TE(P,T)126TE; PHQ=ANGL-DSTRN; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,3; INC-ENGY-LAB=22.0MEV; EXC-ENGY=666.338KEV; J-PTY=2+; DELTA-THTL=1.5DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA (DEG) (UB/SR) 5.182E+00 6.695E+01 1.000E+01 9.274E+01 1.512E+01 9.936E+01 2.023E+01 8.428E+01 2.564E+01 5.726E+01 3.090E+01 3.845E+01 3.508E+01 3.113E+01 4.098E+01 3.494E+01 4.609E+01 3.254E+01 5.133E+01 1.504E+01 5.645E+01 1.352E+01 6.189E+01 1.940E+01 6.670E+01 2.054E+01 \END; /*===================================================================*/ |