/*===================================================================*/ /* NRDF D1600 Data No.50 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,50; 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,50; 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,50; INC-ENGY-LAB=176MEV; PRJ=37CL; TGT=64NI; EMT=X'50'; /*@50@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DELTA-THTC X'1' DELTA-X'1' (DEG) (DEG) (MB/RAD) (MB/RAD) 5.054E+01 +3.945E+00-3.156E+00 7.776E+00 +5.193E+00-2.200E+00 5.961E+01 +2.564E+00-3.451E+00 7.099E+00 +3.320E+00-2.262E+00 6.710E+01 +2.366E+00-2.663E+00 6.650E+00 +3.237E+00-2.119E+00 7.312E+01 +2.268E+00-2.169E+00 6.153E+00 +2.879E+00-2.014E+00 7.854E+01 +2.564E+00-2.762E+00 6.069E+00 +2.287E+00-2.288E+00 8.564E+01 +2.761E+00-2.563E+00 4.754E+00 +2.047E+00-1.473E+00 9.323E+01 +3.057E+00-2.268E+00 5.061E+00 +1.997E+00-1.432E+00 1.003E+02 +3.057E+00-2.761E+00 4.865E+00 +3.250E+00-1.834E+00 1.063E+02 +3.057E+00-2.368E+00 4.860E+00 +2.183E+00-1.909E+00 \END; /*===================================================================*/ |