/*===================================================================*/
 /* NRDF D1600 Data No.35                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,35;
 D#=D1600;
 TITLE=/THE COMPETITION BETWEEN FUSION-FISSION AND DEEPLY INELASTIC
        REACTIONS IN THE MEDIUM MASS SYSTEMS/;
 PURPOSE=/WE EXPECT TO UNDERSTAND THE DRASTICAL CHANGE OF MASS
          DISTRIBUTIONS IN THE 32S/;
 ATH=(Y.H.PU'1',S.M.LEE'1',S.C.JEONG'2',H.FUJIWARA'1',T.MIZOTA'1',
      Y.FUTAMI'1',T.NAKAGAWA'3',H.IKEZOE'4',Y.NAGAME'4');
 INST-ATH=(2JPNTSU'1',2JPNINS'2',2JPNIPC'3',2JPNJAE'4');
 REF=ZP/A;
 VLP=353(1996)387;
 RCTS=(64NI(37CL,X)X,74GE(28SI,X)X);
 PHQS=(ENGY,ANGL-DSTRN,XSECTN);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,35;
 RCT=74GE(28SI,X)X;
 RTY=(FISSN);
 ENR=97%;
 CHM=GE.O2;
 PHYS-FORM=SLD;
 THK-TGT=370UG/CM**2;
 BAC=SELF;
 THK-BAC=XMG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(LINAC);
 INST-ACC=2JPNJAE;
 INC-ENGY-LAB=(176MEV);
 ERS-PRJ=XKEV;
 BEAM-INTNSTY=XA;
 CHRG-INC-ION=X;
 POL-PRJ=0%;
 DET-PARTCL=(X);
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(CNTR-TLSCP);
 SOLID-ANGL=2.1MSR;
 ERS-DET=XKEV;
 ANL=(X);
 PHQ=(ANGL-DSTRN);
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,35;
 INC-ENGY-LAB=176MEV;
 PRJ=37CL;
 TGT=64NI;
 EMT=X'35';
 /*@35@*/
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC  DELTA-THTC        X'1'   DELTA-X'1'
 (DEG)   (DEG)      (MB/RAD)  (MB/RAD)
  5.042E+01  +1.506E+00-2.513E+00  8.290E+00  +3.764E+00-2.715E+00
  5.545E+01  +1.911E+00-2.313E+00  6.882E+00  +2.908E+00-2.644E+00
  6.138E+01  +4.023E+00-2.312E+00  5.841E+00  +2.653E+00-1.998E+00
  6.913E+01  +1.911E+00-2.714E+00  4.443E+00  +1.606E+00-1.676E+00
  7.657E+01  +2.917E+00-2.312E+00  4.305E+00  +1.820E+00-1.683E+00
  8.431E+01  +1.911E+00-2.815E+00  3.820E+00  +1.438E+00-1.389E+00
  8.984E+01  +1.910E+00-2.112E+00  3.580E+00  +1.802E+00-1.276E+00
  9.497E+01  +1.912E+00-2.513E+00  3.585E+00  +1.572E+00-1.120E+00
  1.000E+02  +2.716E+00-2.213E+00  2.911E+00  +1.185E+00-9.530E-01
  1.063E+02  +1.510E+00-3.118E+00  2.526E+00  +7.642E-01-7.699E-01
  1.129E+02  +3.517E+00-2.916E+00  2.368E+00  +1.114E+00-6.851E-01
  1.183E+02  +3.718E+00-2.413E+00  1.780E+00  +8.960E-01-5.959E-01
 \END;
 /*===================================================================*/