/*===================================================================*/
 /* NRDF D0295 Data No.5                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,5;
 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,5;
 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,5;
 CMPD=45SC;
 EXC-ENGY=0.0MEV;
 J-PI=3/2-;
 /*@12@*/
 /*FIG.2-(A)*/
 /* D295                           FIG 2-(A)                       */
 /* SER#=    2            */
 /* XSCALE=LINEAR     YSCALE=LINEAR     */
 /* XMAX= 2.80000000E+03   YMAX= 2.00000000E+00 */
 /* 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)
         2500.88       1.69E-01
         2501.76       4.49E-02
         2511.01       4.49E-02
         2515.42       3.03E-01
         2538.77       7.87E-02
         2546.69       8.31E-01
         2548.02       6.74E-02
         2549.78       3.37E-02
         2555.06       1.46E-01
         2558.59       3.26E-01
         2574.01       3.37E-02
         2579.29       3.93E-01
         2582.82       8.99E-02
         2589.43       1.24E-01
         2606.17       1.01E+00
         2611.45       4.61E-01
         2613.66       8.54E-01
         2621.14       9.66E-01
         2622.47       7.53E-01
         2623.79       3.48E-01
         2632.16       4.72E-01
         2643.61       3.48E-01
         2675.77       1.12E-01
         2713.21       4.49E-02
         2724.23       1.57E-01
         2734.36       1.01E-01
         2766.96       3.26E-01
         2780.18       1.12E-01
         2785.46       6.74E-02
         2787.22       1.12E-01
         2789.43       5.62E-02
 \END;
 /*===================================================================*/