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| /*===================================================================*/
/* NRDF D1547 Data No.75 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,75;
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,75;
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. */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,75;
INC-ENGY-LAB=25MEV;
RSD=21NA;
EXC-ENGY-INITL=1.72MEV;
J-PTY-INITL=7/2+;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (B/SR) (B/SR)
1.614E+01 2.434E-01 +1.094E-01-1.426E-01
2.311E+01 3.018E-01 +7.244E-02-9.776E-02
2.983E+01 3.223E-01 +4.159E-02-7.734E-02
3.256E+01 2.237E-01 +3.795E-02-4.337E-02
3.733E+01 2.213E-01 +3.855E-02-2.763E-02
4.304E+01 1.647E-01 +3.247E-02-2.763E-02
4.867E+01 1.750E-01 +3.126E-02-3.164E-02
5.376E+01 1.171E-01 +1.662E-02-2.118E-02
5.785E+01 1.180E-01 +1.419E-02-1.789E-02
6.293E+01 8.439E-02 +0.000E+00-0.000E+00
6.905E+01 7.701E-02 +0.000E+00-0.000E+00
7.411E+01 7.803E-02 +0.000E+00-0.000E+00
7.895E+01 9.613E-02 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
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