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| /*===================================================================*/
/* NRDF D0357 Data No.10 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,10;
D#=D357;
TITLE=/APPLICATION OF THE CRYSTAL BLOCKING TECHNIQUE TO THE STUDY OF
THE HIGHLY EXCITED NUCLEAR CONTINUUM/;
PURPOSE=/TO EXAMINE CHANGES OF THE REACTION TIMES DUE TO ENHANCEMENT OF
CERTAIN STATES AMONG THE MANY COMPOUND NUCLEAR FINE-STRUCTURE
RESONANCES BY AN ISOBARIC ANALOGUE RESONANCE./;
ATH=(W.M.GIBSON'1,2',M.MARUYAMA'3',Y.HASHIMOTO'3',E.P.KANTER'3',
G.M.TEMMER'3',R.J.KEDDY'4',D.W.MINGAY'4',J.P.F.SELLSCHOP'4');
INST-ATH=(1USABEL'1',1USAALB'2',1USARUT'3',3SAFWIT'4');
/*@7@*/
REF=NP/A;
VLP=317(1979)313;
RCTS=(70GE(P,P)70GE,72GE(P,P)72GE,74GE(P,P)74GE);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,10;
ENR=NAT;
CHM=ELN;
THK-TGT=X'1';
/*@8@*/
BAC=C'2';
/*@11@*/
POL-TGT=NO;
ACC=(VDG);
INST-ACC=1USARUT;
INC-ENGY-LAB-RANGE=(5.035MEV,5.110MEV,4.200MEV,3.708MEV,4.358MEV,
5.210MEV);
POL-PRJ=NO;
DET-PARTCL=(P);
DET-SYS=(PS-SI);
ERS-DET=58KEV;
ANL=(DWBA,STATIST-MODEL,X'1');
/*@9@*/
PHQ=(X'1');
/*@14@*/
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,10;
INC-ENGY-LAB=5.110MEV;
CMPD=73AS;
RSD=72GE;
/*FIG.7-(3)*/
/* D357 FIG.7-(3) */
/* SER#= 10 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 3.00000000E+04 YMAX= 9.99999642E-02 */
/* XMIN= 0.00000000E+00 YMIN= 0.00000000E+00 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA1'1' DELTA-DATA1 DATA2'2' DELTA-DATA2
(UCOULOMB) (UCOULOMB) (NODIM) (NODIM)
2788.595 1.034E+03 9.260E-02 1.793E-03
5397.289 1.574E+03 8.700E-02 2.242E-03
10434.770 1.529E+03 8.161E-02 1.793E-03
14842.566 7.196E+02 8.004E-02 2.242E-03
17001.488 7.646E+02 8.856E-02 1.793E-03
21364.309 1.529E+03 9.305E-02 1.793E-03
24737.621 8.545E+02 9.462E-02 1.793E-03
\END;
/*===================================================================*/
|