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| /*===================================================================*/
/* NRDF D0357 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
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,1;
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@*/
RCT=72GE(P,P)72GE;
PHQ=(EXC-FUNCT,EXC-ENGY,SPIN,PTY);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-ENGY-LAB=4.9[5.2MEV;
CMPD=73AS;
RSD=72GE;
EXC-ENGY=0MEV;
THTL=90DEG;
/*FIG.1-(A)*/
/* D357 FIG.1-(A) */
/* SER#= 1 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 5.19999981E+00 YMAX= 2.00000000E+02 */
/* XMIN= 4.89999962E+00 YMIN= 1.50000000E+02 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE
(MEV) (MB/SR/MEV) (MB/SR/MEV)
4.901 2.076E+02 4.822E+00
4.904 2.109E+02 XXXXXXXXX
4.906 2.066E+02 XXXXXXXXX
4.909 2.036E+02 XXXXXXXXX
4.912 2.048E+02 XXXXXXXXX
4.915 2.036E+02 XXXXXXXXX
4.919 2.041E+02 XXXXXXXXX
4.923 2.018E+02 XXXXXXXXX
4.926 1.980E+02 XXXXXXXXX
4.928 2.000E+02 XXXXXXXXX
4.931 2.018E+02 XXXXXXXXX
4.935 1.995E+02 XXXXXXXXX
4.937 2.018E+02 XXXXXXXXX
4.938 1.985E+02 XXXXXXXXX
4.943 1.985E+02 XXXXXXXXX
4.945 2.013E+02 XXXXXXXXX
4.950 1.995E+02 XXXXXXXXX
4.951 1.934E+02 5.837E+00
4.954 1.919E+02 XXXXXXXXX
4.957 1.914E+02 XXXXXXXXX
4.960 1.962E+02 XXXXXXXXX
4.964 1.934E+02 XXXXXXXXX
4.967 1.886E+02 XXXXXXXXX
4.970 1.871E+02 XXXXXXXXX
4.973 1.881E+02 XXXXXXXXX
4.976 1.863E+02 XXXXXXXXX
4.977 1.843E+02 XXXXXXXXX
4.981 1.843E+02 XXXXXXXXX
4.983 1.794E+02 XXXXXXXXX
4.986 1.772E+02 XXXXXXXXX
4.990 1.728E+02 XXXXXXXXX
4.992 1.706E+02 XXXXXXXXX
4.995 1.650E+02 XXXXXXXXX
4.998 1.594E+02 XXXXXXXXX
5.001 1.581E+02 3.299E+00
5.004 1.607E+02 XXXXXXXXX
5.006 1.670E+02 XXXXXXXXX
5.011 1.708E+02 XXXXXXXXX
5.014 1.734E+02 XXXXXXXXX
5.017 1.751E+02 XXXXXXXXX
5.019 1.787E+02 XXXXXXXXX
5.022 1.812E+02 XXXXXXXXX
5.026 1.901E+02 XXXXXXXXX
5.028 1.977E+02 XXXXXXXXX
5.032 1.972E+02 XXXXXXXXX
5.035 2.003E+02 XXXXXXXXX
5.038 2.036E+02 XXXXXXXXX
5.040 2.036E+02 4.822E+00
5.044 2.028E+02 XXXXXXXXX
5.046 1.980E+02 XXXXXXXXX
5.050 1.972E+02 XXXXXXXXX
5.054 1.954E+02 XXXXXXXXX
5.056 1.898E+02 XXXXXXXXX
5.062 1.904E+02 XXXXXXXXX
5.065 1.850E+02 XXXXXXXXX
5.067 1.838E+02 XXXXXXXXX
5.070 1.802E+02 XXXXXXXXX
5.073 1.716E+02 XXXXXXXXX
5.075 1.645E+02 XXXXXXXXX
5.079 1.617E+02 XXXXXXXXX
5.083 1.561E+02 XXXXXXXXX
5.086 1.561E+02 XXXXXXXXX
5.089 1.482E+02 XXXXXXXXX
5.091 1.467E+02 XXXXXXXXX
5.094 1.454E+02 XXXXXXXXX
5.097 1.437E+02 XXXXXXXXX
5.100 1.437E+02 3.553E+00
5.103 1.434E+02 XXXXXXXXX
5.106 1.482E+02 XXXXXXXXX
5.108 1.510E+02 XXXXXXXXX
5.111 1.561E+02 XXXXXXXXX
5.116 1.589E+02 XXXXXXXXX
5.118 1.642E+02 XXXXXXXXX
5.121 1.703E+02 XXXXXXXXX
5.124 1.718E+02 XXXXXXXXX
5.127 1.741E+02 XXXXXXXXX
5.130 1.754E+02 XXXXXXXXX
5.134 1.751E+02 XXXXXXXXX
5.138 1.756E+02 XXXXXXXXX
5.140 1.766E+02 XXXXXXXXX
5.143 1.777E+02 XXXXXXXXX
5.146 1.797E+02 XXXXXXXXX
5.149 1.794E+02 XXXXXXXXX
5.153 1.799E+02 4.060E+00
5.155 1.817E+02 XXXXXXXXX
5.159 1.792E+02 XXXXXXXXX
5.162 1.815E+02 XXXXXXXXX
5.164 1.777E+02 XXXXXXXXX
5.167 1.772E+02 XXXXXXXXX
5.170 1.772E+02 XXXXXXXXX
5.173 1.789E+02 XXXXXXXXX
5.177 1.820E+02 XXXXXXXXX
5.181 1.830E+02 XXXXXXXXX
5.182 1.766E+02 XXXXXXXXX
5.187 1.766E+02 XXXXXXXXX
5.189 1.772E+02 XXXXXXXXX
5.191 1.751E+02 XXXXXXXXX
5.195 1.756E+02 XXXXXXXXX
5.198 1.764E+02 4.568E+00
\END;
/*===================================================================*/
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