/*===================================================================*/ /* NRDF D0021 Data No.1 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,1; 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,1; /* 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=VCTR-ANALPW; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,1; INC-ENGY-LAB=22.0MEV; DELTA-THTL=1.5DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY'5' THTC AY DELTA-AY FLAG'6' (KEV) (DEG) (NODIM) (NODIM) (NODIM) 0.0 1.502E+01 -5.719E-03 +-3.158E-02 1. 0.0 2.024E+01 4.494E-02 +-5.369E-02 1. 0.0 2.501E+01 1.619E-01 +-3.158E-02 1. 0.0 3.008E+01 1.336E-01 +-3.158E-02 1. 0.0 3.517E+01 2.004E-02 +-3.158E-02 1. 0.0 4.025E+01 -1.567E-01 +-3.474E-02 1. 0.0 4.519E+01 -4.250E-01 +-4.105E-02 1. 0.0 5.011E+01 -3.554E-01 +-4.736E-02 1. 666.338 1.525E+01 7.317E-02 +-3.913E-02 2. 666.338 2.049E+01 9.973E-02 +-4.226E-02 2. 666.338 2.527E+01 1.200E-01 +-4.696E-02 2. 666.338 2.989E+01 4.175E-02 +-3.443E-02 2. 666.338 3.544E+01 3.701E-02 +-4.852E-02 2. 666.338 4.068E+01 1.506E-02 +-4.539E-02 2. 666.338 4.576E+01 -8.045E-02 +-5.635E-02 2. 666.338 5.069E+01 -5.858E-02 +-4.383E-02 2. \END; /*===================================================================*/ |