/*===================================================================*/ /* NRDF D1600 Data No.51 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\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); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\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); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,51; INC-ENGY-LAB=176MEV; PRJ=28SI; TGT=74GE; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \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; /*===================================================================*/ |