/*===================================================================*/
 /* NRDF D1600 Data No.34                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,34;
 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,34;
 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,34;
 INC-ENGY-LAB=176MEV;
 PRJ=37CL;
 TGT=64NI;
 EMT=X'34';
 /*@34@*/
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC  DELTA-THTC        X'1'   DELTA-X'1'
 (DEG)   (DEG)      (MB/RAD)  (MB/RAD)
  5.168E+01  +1.514E+00-2.724E+00  1.348E+01  +5.142E+00-4.897E+00
  5.747E+01  +1.514E+00-3.633E+00  1.080E+01  +4.654E+00-3.758E+00
  6.386E+01  +3.249E+00-3.638E+00  9.185E+00  +2.931E+00-3.194E+00
  7.177E+01  +2.629E+00-2.927E+00  7.564E+00  +2.650E+00-2.751E+00
  7.996E+01  +2.739E+00-2.926E+00  7.413E+00  +3.188E+00-2.745E+00
  8.615E+01  +1.519E+00-2.627E+00  6.523E+00  +2.917E+00-2.125E+00
  9.151E+01  +1.813E+00-2.127E+00  6.073E+00  +2.618E+00-1.827E+00
  9.686E+01  +1.730E+00-1.917E+00  6.421E+00  +2.256E+00-2.473E+00
  1.018E+02  +3.553E+00-2.222E+00  5.638E+00  +2.249E+00-2.362E+00
  1.080E+02  +3.047E+00-2.935E+00  4.629E+00  +2.068E+00-1.746E+00
  1.151E+02  +3.553E+00-3.837E+00  4.475E+00  +2.875E+00-1.722E+00
  1.216E+02  +1.895E+00-3.849E+00  3.020E+00  +1.499E+00-7.100E-01
 \END;
 /*===================================================================*/