/*===================================================================*/
 /* NRDF D1600 Data No.37                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,37;
 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,37;
 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,37;
 INC-ENGY-LAB=176MEV;
 PRJ=37CL;
 TGT=64NI;
 EMT=X'37';
 /*@37@*/
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC  DELTA-THTC        X'1'   DELTA-X'1'
 (DEG)   (DEG)      (MB/RAD)  (MB/RAD)
  6.105E+01  +4.120E+00-3.114E+00  2.118E+00  +8.279E-01-4.464E-01
  6.858E+01  +4.321E+00-3.918E+00  1.834E+00  +6.626E-01-3.445E-01
  7.612E+01  +3.416E+00-4.220E+00  1.998E+00  +3.925E-01-5.198E-01
  8.275E+01  +3.818E+00-3.718E+00  1.634E+00  +4.814E-01-4.337E-01
  8.837E+01  +2.511E+00-3.215E+00  1.488E+00  +3.180E-01-3.387E-01
  9.360E+01  +3.516E+00-2.713E+00  1.633E+00  +3.490E-01-3.985E-01
  9.922E+01  +2.812E+00-2.512E+00  1.435E+00  +4.095E-01-3.106E-01
  1.048E+02  +3.014E+00-3.415E+00  1.335E+00  +3.445E-01-2.739E-01
  1.106E+02  +2.311E+00-3.014E+00  1.354E+00  +3.617E-01-3.378E-01
  1.100E+02  +3.215E+00-2.311E+00  1.148E+00  +3.598E-01-2.157E-01
  1.157E+02  +3.316E+00-5.124E+00  9.125E-01  +1.792E-01-1.607E-01
  1.258E+02  +3.315E+00-3.919E+00  1.076E+00  +2.113E-01-2.507E-01
 \END;
 /*===================================================================*/