/*===================================================================*/ /* NRDF D1600 Data No.33 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\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); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\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); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,33; INC-ENGY-LAB=176MEV; PRJ=37CL; TGT=64NI; EMT=X'33'; /*@33@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \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; /*===================================================================*/ |