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| /*===================================================================*/
/* NRDF D0295 Data No.19 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,19;
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,19;
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,19;
CMPD=45SC;
RSD=44CA;
EXC-ENGY=XMEV;
J-PI=3/2-;
/*@40@*/
/*FIG.5*/
/* D295 FIG 5 */
/* SER#= 12 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 2.80000000E+03 YMAX= 2.99999952E-01 */
/* XMIN= 2.50000000E+03 YMIN= 0.00000000E+00 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB DATA1'1,3'
(KEV) (NODIM)
2500.85 -2.23E-02
2505.94 -1.91E-02
2511.03 -1.17E-02
2515.27 -6.38E-03
2520.37 -2.60E-07
2525.88 1.06E-03
2530.97 4.26E-03
2536.49 7.45E-03
2541.16 1.38E-02
2545.83 2.66E-02
2550.92 4.26E-02
2555.59 5.85E-02
2560.25 6.38E-02
2565.35 5.96E-02
2570.44 6.17E-02
2575.10 7.45E-02
2580.62 8.94E-02
2586.14 9.89E-02
2590.38 1.09E-01
2595.05 1.17E-01
2599.72 1.43E-01
2605.23 1.88E-01
2609.90 2.30E-01
2614.99 2.62E-01
2619.66 3.05E-01
2624.33 3.12E-01
2629.42 2.57E-01
2634.94 1.95E-01
2640.03 1.36E-01
2645.12 9.26E-02
2649.36 6.28E-02
2654.45 4.36E-02
2659.55 3.19E-02
2665.06 1.49E-02
2669.31 1.17E-02
2674.82 5.32E-03
2679.07 3.19E-03
2684.58 3.19E-03
2689.67 3.19E-03
2694.34 2.13E-03
2699.01 5.32E-03
2704.53 3.19E-03
2709.19 1.06E-03
2713.86 -2.60E-07
2719.38 -2.60E-07
2724.47 -1.06E-03
2729.14 -1.06E-03
2733.80 -2.60E-07
2738.90 -2.60E-07
2745.26 -1.06E-03
2749.93 -1.06E-03
2755.02 1.06E-03
2759.26 -2.60E-07
2764.36 -5.32E-03
2769.45 -7.45E-03
2774.54 -9.57E-03
2780.06 -1.70E-02
2785.15 -2.23E-02
2789.39 -1.81E-02
2794.91 -1.28E-02
\END;
/*===================================================================*/
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