/*===================================================================*/ /* NRDF D1600 Data No.43 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,43; 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,43; 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,43; INC-ENGY-LAB=176MEV; PRJ=37CL; TGT=64NI; EMT=X'43'; /*@43@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DELTA-THTC X'1' DELTA-X'1' (DEG) (DEG) (MB/RAD) (MB/RAD) 6.153E+01 +3.732E+00-3.925E+00 3.619E+00 +1.655E+00-1.839E+00 6.958E+01 +1.374E+00-2.651E+00 3.136E+00 +1.500E+00-1.045E+00 7.625E+01 +2.258E+00-2.258E+00 3.577E+00 +1.867E+00-1.359E+00 8.401E+01 +3.535E+00-2.649E+00 3.381E+00 +1.201E+00-1.315E+00 9.294E+01 +3.535E+00-2.257E+00 3.105E+00 +1.291E+00-1.065E+00 1.058E+02 +2.158E+00-3.534E+00 2.938E+00 +1.869E+00-1.116E+00 1.134E+02 +2.847E+00-3.240E+00 3.818E+00 +1.909E+00-1.616E+00 \END; /*===================================================================*/ |