|
| /*===================================================================*/
/* NRDF D0295 Data No.14 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,14;
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,14;
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,14;
CMPD=45SC;
J-PI=3/2-;
/*@32@*/
/*FIG.4-(B)*/
/* D295 FIG 4-(B) */
/* SER#= 9 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 2.80000000E+03 YMAX= 4.00000000E+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)
2502.88 -1.13E-01
2502.88 3.40E-01
2516.15 2.27E-01
2516.15 4.53E-01
2537.50 3.40E-01
2538.07 6.80E-01
2546.73 5.67E-01
2547.31 1.02E+00
2549.61 1.02E+00
2549.61 1.93E+00
2554.81 1.93E+00
2555.38 2.15E+00
2558.27 2.15E+00
2558.84 4.08E+00
2573.84 3.97E+00
2574.42 4.31E+00
2580.19 4.31E+00
2580.77 6.12E+00
2583.65 6.12E+00
2584.23 6.23E+00
2590.00 6.23E+00
2590.57 8.61E+00
2607.88 8.61E+00
2609.04 1.42E+01
2614.81 1.42E+01
2614.81 1.45E+01
2617.11 1.45E+01
2617.11 1.80E+01
2624.61 1.80E+01
2625.19 2.75E+01
2626.34 2.75E+01
2626.34 3.10E+01
2627.50 3.10E+01
2626.92 3.34E+01
2635.00 3.34E+01
2635.57 3.74E+01
2648.27 3.74E+01
2648.27 3.80E+01
2680.00 3.80E+01
2680.00 3.82E+01
2716.92 3.81E+01
2716.92 3.84E+01
2727.31 3.83E+01
2728.46 3.85E+01
2738.27 3.84E+01
2738.84 3.86E+01
2782.11 3.85E+01
2782.11 3.86E+01
2788.46 3.86E+01
2789.61 3.90E+01
2801.15 3.89E+01
\END;
/*===================================================================*/
|