|
| /*===================================================================*/
/* NRDF D0357 Data No.20 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,20;
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,20;
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,20;
INC-ENGY-LAB=5.035MEV;
CMPD=AS;
RSD=GE;
EXC-ENGY-EMT=4.0MEV;
/*FIG.12*/
/* D357 FIG.12 */
/* SER#= 20 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 4.00000000E+00 YMAX= 6.99999988E-01 */
/* XMIN= 0.00000000E+00 YMIN= 0.00000000E+00 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA1'1' DATA2'2' DELTA-DATA2
(ANGSTROM) (NODIM) (NODIM)
0.000 9.256E-02 5.785E-03
0.100 1.041E-01 1.012E-02
0.205 1.374E-01 1.301E-02
0.305 1.909E-01 1.012E-02
0.399 2.473E-01 1.157E-02
0.504 2.893E-01 8.677E-03
0.610 3.225E-01 1.012E-02
0.704 3.500E-01 1.446E-02
0.809 3.775E-01 1.301E-02
0.903 3.992E-01 1.012E-02
1.009 4.107E-01 1.157E-02
1.202 4.324E-01 1.157E-02
1.408 4.483E-01 1.446E-02
1.496 4.585E-01 1.301E-02
1.607 4.599E-01 1.012E-02
1.806 4.715E-01 1.157E-02
2.006 4.874E-01 7.231E-03
2.205 5.062E-01 1.157E-02
2.405 5.207E-01 1.301E-02
2.510 5.264E-01 1.012E-02
2.604 5.351E-01 8.677E-03
2.815 5.467E-01 1.446E-02
2.997 5.554E-01 1.590E-02
3.513 5.756E-01 1.012E-02
4.018 6.060E-01 7.231E-03
4.510 6.277E-01 8.677E-03
4.985 6.446E-01 X
5.455 6.619E-01 X
6.041 6.763E-01 X
7.214 7.137E-01 X
8.446 7.367E-01 X
9.795 7.511E-01 X
11.613 7.712E-01 X
13.372 7.827E-01 X
14.956 7.885E-01 X
16.305 7.914E-01 X
18.592 7.971E-01 X
\END;
/*===================================================================*/
|