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| /*===================================================================*/
/* NRDF D1547 Data No.76 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,76;
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,76;
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,76;
INC-ENGY-LAB=25MEV;
RSD=23NA;
EXC-ENGY-INITL=0.0MEV;
J-PTY-INITL=3/2+;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (B/SR) (B/SR)
1.027E+01 3.680E-01 +6.604E-02-5.461E-02
1.200E+01 3.027E-01 +4.857E-02-6.386E-02
1.517E+01 3.915E-01 +4.857E-02-5.694E-02
1.815E+01 4.397E-01 +6.465E-02-5.317E-02
2.235E+01 3.702E-01 +2.952E-02-6.383E-02
2.539E+01 3.266E-01 +3.753E-02-4.063E-02
2.879E+01 2.081E-01 +2.667E-02-2.138E-02
3.177E+01 1.836E-01 +1.941E-02-1.276E-02
3.615E+01 1.497E-01 +1.789E-02-1.594E-02
4.147E+01 1.507E-01 +2.000E-02-1.603E-02
4.718E+01 1.554E-01 +1.377E-02-1.251E-02
5.230E+01 1.093E-01 +1.108E-02-1.312E-02
5.752E+01 1.014E-01 +0.000E+00-0.000E+00
6.214E+01 8.174E-02 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
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