/*===================================================================*/
 /* NRDF D0295 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 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,2;
 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,2;
 /*@8@*/
 CMPD=45SC;
 J-PI=3/2-;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB LEG-2
 (MEV) (NODIM)
 2.5014 0.48
 2.5024 0.31
 2.5107 0.17
 2.5155 0.44
 2.5385 0.326
 2.5473 0.23
 2.5479 0.51
 2.5501 -0.02
 2.5561 0.34
 2.5590 0.04
 2.5748 0.25
 2.5802 0.02
 2.5841 0.29
 2.5905 0.02
 2.6077 0.03
 2.6132 -0.03
 2.6155 -0.03
 2.6234 -0.02
 2.6240 -0.03
 2.6248 -0.01
 2.6333 0.04
 2.6454 0.07
 2.6775 0.44
 2.7140 0.40
 2.7255 0.36
 2.7347 0.28
 2.7677 0.37
 2.7806 0.27
 2.7864 0.40
 2.7876 0.30
 2.7895 0.43
 \END;
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