/*===================================================================*/ /* NRDF D1547 Data No.20 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,20; D#=D1547; TITLE=/PROTON SINGLE-PARTICLE STATES IN 21,23NA THROUGH THE (D,N) REACTION/; PURPOSE=/TO SEE THE SINGLE-PARTICLE OR SINGLE-HOLE STATES IN RESIDUAL NUCLEI AND GROUND-STATE PROPERTIES OF THE TARGET NUCLEUS./; ATH=(A.TERAKAWA'1',T.TOHEI'1',T.NAKAGAWA'1',A.SATO'1',J.TAKAMATSU'1', M.MORI'1',A.NARITA'1',H.ORIHARA'2',K.ISHII'2',T.NIIZEKI'2', M.OURA'2',S.HIRASAKI'2',M.HOSAKA'2',G.C.JON'2',K.MIURA'3', H.OHNUMA'4'); INST-ATH=(2JPNTOH'1',2JPNTOH'2',2JPNTOI'3',2JPNTIT'4'); /*@1@*/ /*@2@*/ REF=PR/C; VLP=48(1993)2775; RCTS=(20NE(D,N)21NA,22NE(D,N)23NA); PHQS=(ANGL-DSTRN,SPEC-STR'21'); /*@22@*/ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,20; RCT=20NE(D,N)21NA; RTY=(INEL-SCATT); ENR=99.9%; CHM=ELM; PHYS-FORM=GAS; THK-TGT=1.0MG/CM**2; BAC=SELF; ACC=(CYC); INST-ACC=2JPNTOH; INC-ENGY-LAB=(25MEV); CHRG-INC-ION=1; DET-PARTCL=(N); COINC=NO; ANT-COINC=NO; DET-SYS=(TOF)'1'; /*@12@*/ SOLID-ANGL=0.23MSR; /* EFCN-DET=DETECTOR EFFICIENCY WAS 3% WHICH WAS DETERMINED BY THE 7LI(P,N)7BE REACTION THROUGH ACTIVATION ANALYSIS. */ ANL=(OPT-MODEL,ADBA'2',DWBA); /*@13@*/ PHQ=(ANGL-DSTRN,SPEC-STR'21'); /*@22@*/ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,20; INC-ENGY-LAB=25MEV; RSD=21NA; EXC-ENGY-INITL=4.17MEV; J-PTY-INITL=3/2-; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC'7' DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (B/SR) (B/SR) 2.236E+00 9.621E+00 +0.000E+00-0.000E+00 4.436E+00 1.084E+01 +0.000E+00-0.000E+00 1.292E+01 5.211E+00 +0.000E+00-0.000E+00 1.495E+01 3.286E+00 +0.000E+00-0.000E+00 1.778E+01 2.302E+00 +0.000E+00-0.000E+00 2.033E+01 1.551E+00 +0.000E+00-0.000E+00 2.334E+01 1.218E+00 +0.000E+00-0.000E+00 2.595E+01 9.605E-01 +0.000E+00-0.000E+00 2.918E+01 6.697E-01 +0.000E+00-0.000E+00 3.312E+01 6.134E-01 +0.000E+00-0.000E+00 3.903E+01 4.747E-01 +0.000E+00-0.000E+00 4.484E+01 2.756E-01 +2.662E-02-2.021E-02 4.991E+01 1.741E-01 +2.416E-02-2.283E-02 5.371E+01 2.113E-01 +0.000E+00-0.000E+00 5.876E+01 1.185E-01 +1.871E-02-1.105E-02 6.434E+01 1.096E-01 +0.000E+00-0.000E+00 7.004E+01 9.245E-02 +0.000E+00-0.000E+00 7.607E+01 6.527E-02 +0.000E+00-0.000E+00 8.068E+01 4.097E-02 +6.964E-03-3.019E-03 \END; /*===================================================================*/ |