/*===================================================================*/ /* NRDF D1600 Data No.52 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,52; 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,52; RCT=64NI(37CL,X)X; RTY=(FISSN); ENR=X%; CHM=X; PHYS-FORM=SLD; THK-TGT=280UG/CM**2; BAC=SELF; THK-BAC=XMG/CM**2; POL-TGT=0%; ALGN-TGT=0%; ACC=(LINAC); INST-ACC=2JPNJAE; INC-ENGY-LAB=(186MEV); ERS-PRJ=XKEV; BEAM-INTNSTY=10[100NA; 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,52; INC-ENGY-LAB=186MEV; PRJ=37CL; TGT=64NI; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; Z-EMT XSECTN DELTA-XSECTN (NODIM) (NODIM) (NODIM) 5.778E+00 6.763E+00 +0.000E+00-0.000E+00 6.704E+00 2.482E+00 +0.000E+00-0.000E+00 7.729E+00 5.113E+00 +0.000E+00-0.000E+00 8.846E+00 2.731E+00 +0.000E+00-0.000E+00 1.008E+01 5.903E+00 +0.000E+00-0.000E+00 1.104E+01 6.557E+00 +0.000E+00-0.000E+00 1.195E+01 1.243E+01 +9.871E-01-1.071E+00 1.285E+01 1.502E+01 +1.110E+00-9.805E-01 1.377E+01 1.999E+01 +1.805E+00-1.484E+00 1.461E+01 2.240E+01 +1.397E+00-1.768E+00 1.554E+01 2.121E+01 +1.479E+00-1.189E+00 1.668E+01 2.244E+01 +1.313E+00-1.687E+00 1.768E+01 2.343E+01 +8.134E-01-1.730E+00 1.871E+01 2.417E+01 +1.356E+00-1.896E+00 1.985E+01 2.372E+01 +1.483E+00-1.150E+00 2.069E+01 2.387E+01 +1.278E+00-1.148E+00 2.174E+01 2.478E+01 +1.151E+00-1.066E+00 2.265E+01 2.485E+01 +1.194E+00-1.023E+00 2.353E+01 2.415E+01 +1.276E+00-1.149E+00 2.438E+01 2.385E+01 +1.069E+00-1.352E+00 2.544E+01 2.377E+01 +1.353E+00-1.232E+00 2.626E+01 2.360E+01 +1.317E+00-1.764E+00 2.739E+01 2.233E+01 +1.559E+00-1.848E+00 2.863E+01 2.122E+01 +1.231E+00-1.689E+00 2.971E+01 2.040E+01 +1.396E+00-1.482E+00 3.057E+01 1.908E+01 +1.520E+00-1.803E+00 \END; /*===================================================================*/ |