/*===================================================================*/ /* NRDF D1547 Data No.60 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,60; 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,60; RCT=22NE(D,N)23NA; RTY=(INEL-SCATT); ENR=99.9%; CHM=ELM; PHYS-FORM=GAS; THK-TGT=1.1MG/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,60; INC-ENGY-LAB=25MEV; RSD=23NA; EXC-ENGY-INITL=3.91MEV; J-PTY-INITL=5/2+; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC'15' DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (B/SR) (B/SR) 1.004E+01 7.949E-01 +0.000E+00-0.000E+00 1.183E+01 1.090E+00 +0.000E+00-0.000E+00 1.509E+01 8.866E-01 +0.000E+00-0.000E+00 1.811E+01 8.248E-01 +0.000E+00-0.000E+00 2.035E+01 8.172E-01 +0.000E+00-0.000E+00 2.790E+01 4.039E-01 +5.140E-02-2.776E-02 3.154E+01 3.360E-01 +0.000E+00-0.000E+00 3.694E+01 2.502E-01 +2.250E-02-4.428E-02 4.149E+01 9.456E-02 +1.776E-02-2.551E-02 4.663E+01 2.124E-01 +0.000E+00-0.000E+00 5.234E+01 1.002E-01 +9.837E-03-1.615E-02 5.778E+01 1.498E-01 +0.000E+00-0.000E+00 6.201E+01 1.284E-01 +0.000E+00-0.000E+00 \END; /*===================================================================*/ |