DARPE: Search Results
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 /* NRDF D1600 Data No.51                                             */
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 /* Bibliography                                                      */
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 \\BIB,51;
 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,51;
 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=(XSECTN);
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 /* Descriptive Parameters                                            */
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 \\DATA,51;
 INC-ENGY-LAB=176MEV;
 PRJ=28SI;
 TGT=74GE;
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 /* Data Table                                                        */
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 \DATA;
 Z-EMT        XSECTN   DELTA-XSECTN
 (NODIM)      (NODIM)    (NODIM)
  5.924E+00  7.704E+00  +9.829E-01-1.120E+00
  7.047E+00  4.386E+00  +8.219E-01-8.507E-01
  8.108E+00  6.440E+00  +9.290E-01-1.249E+00
  9.081E+00  4.288E+00  +0.000E+00-0.000E+00
  1.024E+01  5.468E+00  +1.010E+00-9.283E-01
  1.113E+01  5.708E+00  +7.193E-01-9.305E-01
  1.217E+01  1.298E+01  +7.171E-01-7.156E-01
  1.311E+01  1.122E+01  +1.009E+00-8.249E-01
  1.397E+01  1.583E+01  +7.163E-01-9.844E-01
  1.490E+01  1.240E+01  +7.680E-01-9.541E-01
  1.592E+01  1.229E+01  +6.632E-01-9.002E-01
  1.684E+01  1.222E+01  +1.118E+00-6.676E-01
  1.799E+01  1.236E+01  +7.459E-01-7.200E-01
  1.904E+01  1.212E+01  +5.051E-01-6.632E-01
  2.011E+01  1.271E+01  +5.066E-01-8.788E-01
  2.109E+01  1.227E+01  +0.000E+00-0.000E+00
  2.207E+01  1.269E+01  +0.000E+00-0.000E+00
  2.279E+01  1.296E+01  +1.038E+00-1.140E+00
  2.373E+01  1.237E+01  +0.000E+00-0.000E+00
  2.461E+01  1.291E+01  +0.000E+00-0.000E+00
  2.556E+01  1.246E+01  +0.000E+00-0.000E+00
  2.668E+01  1.422E+01  +9.837E-01-6.395E-01
  2.789E+01  1.497E+01  +1.114E+00-6.403E-01
  2.885E+01  1.522E+01  +0.000E+00-0.000E+00
  2.988E+01  1.461E+01  +0.000E+00-0.000E+00
 \END;
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