|
| /*===================================================================*/
/* NRDF D0295 Data No.13 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,13;
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,13;
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,13;
CMPD=45SC;
J-PI=3/2-;
/*@31@*/
/*FIG.4-(A)*/
/* D295 FIG 4-(A) */
/* SER#= 8 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 2.80000000E+03 YMAX= 8.00000000E+00 */
/* XMIN= 2.50000000E+03 YMIN= 0.00000000E+00 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB DATA6'6'
(KEV) (KEV)
2502.30 -2.57E-02
2502.30 1.80E-01
2514.39 2.06E-01
2514.97 4.63E-01
2537.43 4.63E-01
2537.43 5.66E-01
2546.06 5.14E-01
2546.64 1.34E+00
2547.21 1.31E+00
2547.79 1.41E+00
2554.70 1.41E+00
2555.28 1.57E+00
2557.58 1.59E+00
2558.15 1.93E+00
2580.04 1.95E+00
2580.04 2.34E+00
2583.49 2.37E+00
2583.49 2.47E+00
2589.25 2.47E+00
2589.25 2.60E+00
2607.68 2.60E+00
2607.10 3.60E+00
2612.86 3.63E+00
2613.43 4.12E+00
2615.74 4.12E+00
2616.31 4.96E+00
2623.80 4.96E+00
2623.22 5.86E+00
2624.95 5.92E+00
2624.37 6.64E+00
2625.53 6.66E+00
2624.95 7.00E+00
2633.59 7.00E+00
2633.59 7.54E+00
2645.68 7.51E+00
2646.25 7.85E+00
2678.50 7.85E+00
2679.08 7.95E+00
2713.63 7.95E+00
2713.63 8.03E+00
2726.87 8.00E+00
2727.44 8.15E+00
2734.35 8.13E+00
2735.51 8.18E+00
2767.75 8.18E+00
2768.33 8.46E+00
2779.84 8.46E+00
2780.42 8.54E+00
2785.60 8.54E+00
\END;
/*===================================================================*/
|