/*===================================================================*/
 /* NRDF D0295 Data No.9                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,9;
 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,9;
 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,9;
 CMPD=45SC;
 EXC-ENGY=XMEV;
 J-PI=3/2-;
 /*@19@*/
 /*FIG.3-(A)*/
 /* D295                           FIG 3-(A)                       */
 /* SER#=    6            */
 /* XSCALE=LINEAR     YSCALE=LINEAR     */
 /* XMAX= 2.80000000E+03   YMAX= 1.00000000E+01 */
 /* XMIN= 2.50000000E+03   YMIN= 0.00000000E+00 */
 /* FOLLOWING DATA ARE TAKEN FROM GRAPH */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
       INC-ENGY-LAB  SQ-REDUCED-WDTH
           (KEV)         (KEV)
         2500.85       1.69E-01
         2501.70       2.54E-01
         2510.18       3.81E-01
         2515.27       1.69E-01
         2537.34       2.54E-01
         2547.10       3.81E-01
         2550.07       1.19E+00
         2556.01       3.81E-01
         2558.56       1.95E+00
         2575.10       2.97E-01
         2581.05       1.82E+00
         2584.44       2.97E-01
         2590.81       2.25E+00
         2608.63       5.59E+00
         2614.14       6.36E-01
         2616.26       3.52E+00
         2624.75       9.49E+00
         2624.75       3.56E+00
         2626.45       2.80E+00
         2634.09       4.07E+00
         2646.39       8.47E-01
         2678.64       2.97E-01
         2714.71       2.12E-01
         2725.74       2.12E-01
         2735.93       2.12E-01
         2767.75       1.69E-01
         2780.48       2.97E-01
         2786.00       3.81E-01
         2788.12       1.69E-01
         2789.81       1.69E-01
 \END;
 /*===================================================================*/