|
| /*===================================================================*/
/* NRDF D0295 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
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,4;
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,4;
CMPD=45SC;
J-PI=3/2-;
/*@11@*/
/*FIG.1*/
/* D295 FIG 1 */
/* SER#= 1 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 2.80000000E+03 YMAX= 9.00000000E+01 */
/* XMIN= 2.50000000E+03 YMIN= 0.00000000E+00 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB DATA1'1' DELTA-DATA1
(KEV) (DEG) (DEG)
2501.25 6.25E+00 7.08E+00
2502.09 -3.75E+01 6.66E+00
2509.60 -5.29E+01 4.58E+00
2514.60 1.50E+01 6.66E+00
2537.55 2.92E+01 4.58E+00
2550.07 8.62E+01 1.08E+01
2547.98 -8.33E-01 5.83E+00
2547.15 -4.71E+01 5.41E+00
2555.91 -3.38E+01 6.66E+00
2558.41 -7.29E+01 6.66E+00
2574.27 -5.00E+01 4.58E+00
2580.53 -7.50E+01 8.75E+00
2583.87 -4.50E+01 4.58E+00
2590.12 -7.58E+01 6.66E+00
2606.40 -7.33E+01 6.66E+00
2612.66 -8.58E+01 6.25E+00
2615.16 -9.04E+01 7.91E+00
2621.00 -8.54E+01 6.25E+00
2623.09 -8.67E+01 6.25E+00
2624.34 -9.04E+01 5.83E+00
2633.10 -7.17E+01 6.25E+00
2644.78 -6.75E+01 6.66E+00
2676.91 1.92E+01 6.25E+00
2713.63 2.79E+01 7.91E+00
2724.48 -3.71E+01 6.66E+00
2733.66 3.79E+01 5.41E+00
2767.04 2.50E+01 7.08E+00
2780.39 3.83E+01 5.00E+00
2786.23 2.54E+01 5.41E+00
2787.48 3.58E+01 5.00E+00
2789.57 1.58E+01 6.66E+00
\END;
/*===================================================================*/
|