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/* NRDF D1547 Data No.63 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,63;
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,63;
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,63;
INC-ENGY-LAB=25MEV;
RSD=23NA;
EXC-ENGY-INITL=8.42MEV;
J-PTY-INITL=3/2+;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC'15' DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (B/SR) (B/SR)
1.345E+01 2.454E+00 +0.000E+00-0.000E+00
1.496E+01 2.792E+00 +0.000E+00-0.000E+00
1.778E+01 2.260E+00 +0.000E+00-0.000E+00
2.152E+01 1.656E+00 +0.000E+00-0.000E+00
2.494E+01 1.412E+00 +0.000E+00-0.000E+00
2.874E+01 1.315E+00 +0.000E+00-0.000E+00
3.156E+01 8.791E-01 +0.000E+00-0.000E+00
3.432E+01 5.642E-01 +0.000E+00-0.000E+00
3.895E+01 3.387E-01 +4.105E-02-4.323E-02
4.441E+01 2.983E-01 +0.000E+00-0.000E+00
5.094E+01 2.422E-01 +2.540E-02-2.935E-02
5.575E+01 2.012E-01 +2.522E-02-1.841E-02
6.024E+01 1.734E-01 +0.000E+00-0.000E+00
6.555E+01 7.466E-02 +2.826E-02-1.371E-02
\END;
/*===================================================================*/
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