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/* NRDF D0357 Data No.13 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,13;
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,13;
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=(EXC-ENGY,SPIN,PTY,X'1');
/*@15@*/
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,13;
INC-ENGY-LAB=5.110MEV;
CMPD=73AS;
RSD=72GE;
EXC-ENGY=0.835MEV;
J-PI=2+'1';
/*@5@*/
DATA=0.430+-0.021'1';
WDTH=21.4MIN'2';
DELTA-WDTH=1.2MIN;
/*@3@*/
/*@4@*/
/*FIG.9-(C)*/
/* D357 FIG.9-(C) */
/* SER#= 12 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 4.00000000E+01 YMAX= 3.00000000E+02 */
/* XMIN=-4.00000000E+01 YMIN= 0.00000000E+00 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
ANGL COUNTS/CHNL
(MINUTES) (NODIM)
-47.640 3.255E+02
-44.944 3.382E+02
-41.798 3.227E+02
-40.899 3.109E+02
-38.652 3.264E+02
-36.854 3.109E+02
-34.157 3.036E+02
-31.461 3.264E+02
-29.214 3.245E+02
-27.416 3.764E+02
-24.719 3.245E+02
-24.719 3.200E+02
-22.921 3.164E+02
-20.674 3.500E+02
-18.427 3.109E+02
-16.180 2.909E+02
-13.483 2.627E+02
-12.135 2.755E+02
-9.438 2.145E+02
-8.090 1.936E+02
-6.742 1.745E+02
-3.596 1.327E+02
-0.449 1.200E+02
1.798 1.382E+02
3.146 1.600E+02
5.393 1.673E+02
7.191 2.000E+02
9.888 2.364E+02
12.135 2.455E+02
13.933 2.291E+02
19.775 2.409E+02
15.730 2.727E+02
18.876 2.709E+02
22.022 2.973E+02
24.270 3.091E+02
27.416 3.318E+02
29.213 3.073E+02
30.562 3.318E+02
32.809 3.627E+02
35.056 3.273E+02
35.056 2.864E+02
38.652 2.809E+02
41.348 2.964E+02
45.393 2.836E+02
43.146 3.445E+02
47.191 3.309E+02
49.888 3.309E+02
51.236 3.136E+02
\END;
/*===================================================================*/
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