/*===================================================================*/ /* NRDF D0021 Data No.4 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,4; 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,4; /* 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=110PD(P,T)108PD; PHQ=ANGL-DSTRN; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,4; INC-ENGY-LAB=22.0MEV; EXC-ENGY=433.938KEV; J-PTY=2+; DELTA-THTL=1.5DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (UB/SR) (UB/SR) 5.188E+00 7.792E+01 +-5.658E+00 1.004E+01 2.445E+02 +-2.180E+01 1.533E+01 3.895E+02 +-2.826E+01 2.076E+01 4.077E+02 +-2.757E+01 2.571E+01 2.706E+02 +-2.306E+01 3.064E+01 1.341E+02 +-1.197E+01 3.605E+01 9.775E+01 +-8.326E+00 4.086E+01 1.035E+02 +-1.014E+01 4.644E+01 9.416E+01 +-7.397E+00 5.124E+01 6.943E+01 +-6.193E+00 5.664E+01 4.149E+01 +-5.423E+00 6.237E+01 3.167E+01 +-4.141E+00 \END; /*===================================================================*/ |