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| /*===================================================================*/
/* NRDF D1547 Data No.74 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,74;
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,74;
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,74;
INC-ENGY-LAB=25MEV;
RSD=21NA;
EXC-ENGY-INITL=0.0MEV;
J-PTY-INITL=3/2+;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (B/SR) (B/SR)
1.091E+01 8.997E-01 +1.713E-01-1.679E-01
1.270E+01 1.054E+00 +1.328E-01-1.435E-01
1.620E+01 4.356E-01 +1.306E-01-1.057E-01
1.998E+01 6.521E-01 +1.087E-01-8.898E-02
2.351E+01 4.644E-01 +6.914E-02-6.512E-02
2.689E+01 5.881E-01 +6.943E-02-6.838E-02
2.960E+01 4.335E-01 +5.490E-02-4.547E-02
3.261E+01 3.659E-01 +3.964E-02-2.798E-02
3.783E+01 2.522E-01 +3.861E-02-2.764E-02
4.355E+01 2.156E-01 +2.916E-02-1.254E-02
4.932E+01 1.579E-01 +2.938E-02-2.043E-02
5.404E+01 1.210E-01 +1.858E-02-2.176E-02
5.840E+01 1.309E-01 +1.893E-02-1.143E-02
6.414E+01 9.178E-02 +0.000E+00-0.000E+00
6.959E+01 8.557E-02 +0.000E+00-0.000E+00
7.487E+01 8.169E-02 +0.000E+00-0.000E+00
7.885E+01 8.257E-02 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
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