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| /*===================================================================*/
/* NRDF D0295 Data No.16 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,16;
D#=D295;
TITLE=/STUDY OF INELASTIC PROTON AMPLITUDES FOR A FRAGMENTED ANALOGUE
STATE IN 45SC/;
PURPOSE=/RECENTLY WE DEVELOPED A SIMPLE TECHNIQUE WHICH ENABLE ONE TO
MEASURE THE MAGNITUDES AND THE RELATIVE SGIN OF INELASTIC
PROTON-CHANNEL AMPLITUDES FOR ISOLATED RESONANCES COMBINENED
WITH OUR HIGH RESOLUTION SYSTEM, THIS NEW TECHNIQUE MAKES
POSSIBLE NEW TYPES OF STUDIES OF ASPECTS OF LINE-BROADENING
(E.G.,FRAGMENTED ANALOGUE STATES) AND OF STATISTICAL PROPERTIES
OF COMPOUND NUCLEAR STATES. A FRAGMENTED ANALOGUE STATE IN
45SC PROVIDES AN EXCELLENT EXAMPLE OF ANALOGUE FINE STRUCTURE
IN THREE CHANNELS, WITH THE ROBSON ASYMMETRY CLEARLY
DEMONSTRATED FOR A NON-ELASTIC CHANNEL. THE CORRELATION
BETWEEN AMPLITUDES (RATHER THAN WIDTHS) IN DIFFERENT CHANNELS
IS PRESENTED. THESE NEW EXPERIMENTAL DATA MAY BE VIEWED AS AN
'OFF-DIAGONAL STRENGTH FUNCTION'. THE ANALOGUE RESULTLS FOR
THE TOW INELASTIC CHANNELS (DIAGONAL STRENGTH FUNCTIONS) ARE
USED TO PREDICT THE OFF-DIAGONAL STRENGTH FUNCTION AND THE
PREDICTIONS ARE COMPARED WITH THE THEORY OF ANALOGUE STATE
BROADENING./;
/*@41@*/
ATH=(G.E.MITCHELL'1,2',T.R.DITTRICH'1,2',E.G.BILPUCH'2,3');
INST-ATH=(1USANCS'1',1USATNL'2',1USADKE'3');
REF=ZP/A;
VLP=289(1979)211;
RCTS=44CA(P,P,GAMMA);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,16;
RCT=44CA(P,P,GAMMA);
ENR=98.6%;
CHM=CACO3'1';
/*@3@*/
THK-TGT=1[2MG/CM**2;
BAC=CARBON-FOIL;
THK-BAC=5[10MUG/CM**2;
POL-TGT=NO;
ALGN-TGT=NO;
ACC=(VDG);
INST-ACC=1USATNL;
INC-ENGY-LAB-RANGE=2.5MEV(XMEV)2.8MEV;
DELTA-INC-ENGY=XKEV;
ERS-PRJ=XKEV;
BEAM-INTNSTY=XUA;
POL-PRJ=NO;
ANL=RMTRX-THEORY;
PHQ=(EXC-FUNCT,ANGL-DSTRN,ENGY-SPEC,SPIN-CORRL-PARA'1',PART-WDTH'2',SPE
C-FCTR,TRANSN-STRGTH'3');
/*@5@*/
/*@6@*/
/*@17@*/
/*@38@*/
DET-PARTCL=(GAMMA);
DET-SYS=(NAI'1');
/*4@*/
DET-PARTCL=P;
DET-SYS=(SI);
ERS-DET=0.35KEV;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,16;
CMPD=45SC;
J-PI=3/2-;
/*@34@*/
/*FIG.4-(D)*/
/* D295 FIG 4-(D) */
/* SER#= 11 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 2.80000000E+03 YMAX= 2.50000000E+01 */
/* XMIN= 2.50000000E+03 YMIN= 0.00000000E+00 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB DATA6'6'
(KEV) (KEV)
2501.72 -1.81E-05
2501.14 1.78E+00
2502.29 1.78E+00
2502.29 2.37E+00
2509.75 2.37E+00
2510.32 2.67E+00
2514.91 2.67E+00
2515.49 3.04E+00
2536.14 2.97E+00
2536.71 3.19E+00
2545.31 3.26E+00
2545.89 4.08E+00
2546.46 4.01E+00
2547.03 4.30E+00
2549.33 4.30E+00
2549.33 4.45E+00
2555.64 4.53E+00
2556.21 5.79E+00
2558.51 5.71E+00
2559.08 7.05E+00
2573.99 7.05E+00
2574.57 7.34E+00
2579.16 7.42E+00
2579.73 8.53E+00
2583.75 8.61E+00
2584.32 8.98E+00
2590.63 8.98E+00
2591.20 1.02E+01
2607.84 1.04E+01
2607.84 1.39E+01
2612.43 1.39E+01
2612.43 1.41E+01
2615.87 1.41E+01
2616.44 1.50E+01
2623.32 1.50E+01
2623.90 1.94E+01
2625.05 1.94E+01
2625.62 2.02E+01
2634.80 2.02E+01
2634.80 2.31E+01
2646.84 2.31E+01
2647.42 2.37E+01
2679.54 2.36E+01
2680.11 2.41E+01
2716.25 2.41E+01
2716.82 2.43E+01
2727.15 2.42E+01
2727.72 2.47E+01
2736.90 2.46E+01
2737.47 2.48E+01
2770.74 2.47E+01
2770.74 2.49E+01
2788.53 2.48E+01
2788.53 2.52E+01
\END;
/*===================================================================*/
|