/*===================================================================*/
 /* NRDF D1537 Data No.1                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D1537;
 TITLE=/SPIN-FLIP PROBABILITIES VIA ISOBARIC ANALOGUE RESONANCES IN
        50TI(P,P')50TI* INELASTIC SCATTERING/;
 PURPOSE=/STUDY OF S(THETA) THROUGH IAR, IN WICH RESONANCE PROCESS IS
          CONSIDERED DOMINANT, AND OF THE STRUCTURE OF PARENT STATE./;
 ATH=(T.NOJIRI'1',H.TOYAMA'2');
 INST-ATH=(2JPNJPN'1',2JPNTIT'2');
 REF=JPJ;
 VLP=37(1974)1479;
 RCTS=50TI(P,P)50TI;
 PHQS=(EXC-FUNCT,SIGMA,SFLP,ANGL-DSTRN);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 RCT=50TI(P,P)50TI;
 RTY=(INEL-SCATT);
 ENR=NAT;
 CHM=TI.O2;
 PHYS-FORM=SLD;
 THK-TGT=10MUG/CM**2;
 BAC=C;
 THK-BAC=XMG/CM**2;
 ACC=(VDG);
 INST-ACC=2JPNINS;
 ERS-PRJ=XKEV'21';
 /*@31@*/
 INC-ENGY-LAB-RANGE=(3.580MEV(XMEV)3.625MEV);
 DET-PARTCL=(P,GAMMA);
 COINC=GAMMA;
 ANT-COINC=NO;
 DET-SYS=(SSD,NAI(TL));
 SOLID-ANGL=1.29MSR'22';
 /*@32@*/
 PHQ=(EXC-FUNCT);
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 EMT-1=P;
 RSD=50TI;
 THTL-1=90DEG;
 EXC-ENGY=1.55MEV;
 J-PTY=2+;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY  COUNTS
 (MEV)   (NODIM)
  3.580E+00  5.567E+01
  3.583E+00  1.206E+02
  3.587E+00  4.639E+02
  3.588E+00  8.320E+02
  3.588E+00  8.876E+02
  3.589E+00  6.588E+02
  3.590E+00  4.191E+02
  3.591E+00  3.418E+02
  3.592E+00  3.541E+02
  3.593E+00  5.289E+02
  3.594E+00  6.541E+02
  3.595E+00  4.918E+02
  3.596E+00  3.758E+02
  3.597E+00  2.861E+02
  3.598E+00  2.366E+02
  3.599E+00  2.660E+02
  3.600E+00  3.186E+02
  3.601E+00  4.222E+02
  3.602E+00  4.655E+02
  3.604E+00  7.763E+02
  3.605E+00  1.212E+03
  3.606E+00  1.421E+03
  3.607E+00  1.265E+03
  3.608E+00  1.018E+03
  3.610E+00  5.861E+02
  3.612E+00  3.433E+02
  3.613E+00  2.242E+02
  3.617E+00  2.567E+02
  3.620E+00  1.515E+02
 \END;
 /*===================================================================*/