DARPE: Search Results
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 /* NRDF D1600 Data No.33                                             */
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 /* Bibliography                                                      */
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 \\BIB,33;
 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);
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 /* Experimental Conditions                                           */
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 \\EXP,33;
 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);
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 /* Descriptive Parameters                                            */
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 \\DATA,33;
 INC-ENGY-LAB=176MEV;
 PRJ=37CL;
 TGT=64NI;
 EMT=X'33';
 /*@33@*/
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 /* Data Table                                                        */
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 \DATA;
 THTC  DELTA-THTC        X'1'   DELTA-X'1'
 (DEG)   (DEG)      (MB/RAD)  (MB/RAD)
  5.141E+01  +1.743E+00-2.749E+00  9.315E+00  +2.516E+00-3.128E+00
  5.799E+01  +2.666E+00-3.784E+00  7.481E+00  +2.107E+00-2.898E+00
  6.446E+01  +2.460E+00-2.658E+00  6.976E+00  +2.157E+00-2.343E+00
  7.297E+01  +3.077E+00-3.688E+00  6.397E+00  +1.976E+00-2.589E+00
  8.106E+01  +2.882E+00-2.652E+00  6.161E+00  +2.566E+00-2.418E+00
  8.763E+01  +2.881E+00-2.052E+00  5.746E+00  +1.627E+00-2.040E+00
  9.236E+01  +1.930E+00-1.342E+00  5.135E+00  +1.720E+00-1.476E+00
  9.838E+01  +1.959E+00-2.447E+00  5.502E+00  +1.414E+00-2.059E+00
  1.111E+02  +2.665E+00-3.287E+00  3.442E+00  +1.587E+00-9.169E-01
  1.178E+02  +2.756E+00-4.008E+00  3.276E+00  +2.165E+00-1.010E+00
 \END;
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