/*===================================================================*/ /* NRDF D1600 Data No.53 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,53; 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,53; 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=(170MEV); 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,53; INC-ENGY-LAB=170MEV; PRJ=37CL; TGT=64NI; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; Z-EMT XSECTN DELTA-XSECTN (NODIM) (NODIM) (NODIM) 5.494E+00 4.459E+00 +8.037E-01-8.037E-01 6.416E+00 1.699E+00 +0.000E+00-0.000E+00 7.500E+00 2.627E+00 +0.000E+00-0.000E+00 8.573E+00 1.141E+00 +0.000E+00-0.000E+00 9.686E+00 3.237E+00 +0.000E+00-0.000E+00 1.091E+01 3.260E+00 +0.000E+00-0.000E+00 1.184E+01 8.804E+00 +1.091E+00-1.325E+00 1.271E+01 7.756E+00 +1.064E+00-8.301E-01 1.367E+01 1.231E+01 +8.816E-01-8.561E-01 1.463E+01 1.277E+01 +7.774E-01-1.065E+00 1.551E+01 1.614E+01 +1.141E+00-1.274E+00 1.763E+01 1.441E+01 +2.128E+00-2.183E+00 1.861E+01 1.575E+01 +1.556E+00-1.636E+00 1.963E+01 1.489E+01 +1.271E+00-1.219E+00 2.087E+01 1.338E+01 +9.589E-01-1.094E+00 2.174E+01 1.547E+01 +1.087E+00-1.192E+00 2.267E+01 1.570E+01 +8.829E-01-8.802E-01 2.364E+01 1.592E+01 +6.995E-01-7.000E-01 2.432E+01 1.598E+01 +7.272E-01-8.310E-01 2.531E+01 1.520E+01 +6.995E-01-8.561E-01 2.646E+01 1.322E+01 +2.671E+00-2.440E+00 2.742E+01 1.264E+01 +2.440E+00-2.543E+00 2.862E+01 9.524E+00 +2.672E+00-2.883E+00 2.985E+01 1.056E+01 +2.514E+00-2.652E+00 \END; /*===================================================================*/ |