/*===================================================================*/ /* NRDF D1547 Data No.64 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,64; 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,64; 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,64; INC-ENGY-LAB=25MEV; RSD=23NA; EXC-ENGY-INITL=9.70MEV; J-PTY-INITL=3/2+; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC'15' DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (B/SR) (B/SR) 1.116E+01 2.077E+00 +0.000E+00-0.000E+00 1.315E+01 1.913E+00 +0.000E+00-0.000E+00 1.607E+01 1.549E+00 +0.000E+00-0.000E+00 1.922E+01 9.457E-01 +0.000E+00-0.000E+00 2.290E+01 5.253E-01 +9.725E-02-1.096E-01 2.982E+01 3.079E-01 +5.979E-02-5.581E-02 3.293E+01 3.556E-01 +7.067E-02-4.519E-02 3.703E+01 2.860E-01 +4.535E-02-5.007E-02 4.220E+01 2.519E-01 +4.554E-02-4.251E-02 4.861E+01 1.952E-01 +3.355E-02-3.477E-02 5.417E+01 1.600E-01 +2.123E-02-1.713E-02 5.833E+01 1.026E-01 +1.899E-02-1.796E-02 6.302E+01 8.899E-02 +1.181E-02-1.558E-02 \END; /*===================================================================*/ |