/*===================================================================*/ /* NRDF D1600 Data No.48 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,48; 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,48; 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,48; INC-ENGY-LAB=176MEV; PRJ=37CL; TGT=64NI; EMT=X'48'; /*@48@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DELTA-THTC X'1' DELTA-X'1' (DEG) (DEG) (MB/RAD) (MB/RAD) 5.353E+01 +4.545E+00-3.263E+00 4.390E+00 +3.317E+00-1.754E+00 6.233E+01 +2.373E+00-2.570E+00 4.577E+00 +2.470E+00-1.935E+00 6.974E+01 +2.767E+00-2.967E+00 4.526E+00 +2.915E+00-1.548E+00 7.578E+01 +1.582E+00-2.671E+00 4.302E+00 +2.323E+00-1.651E+00 8.260E+01 +2.769E+00-2.867E+00 4.424E+00 +2.212E+00-1.903E+00 9.071E+01 +3.065E+00-4.450E+00 3.890E+00 +2.022E+00-1.524E+00 9.753E+01 +3.066E+00-3.263E+00 3.948E+00 +2.375E+00-1.417E+00 1.044E+02 +2.966E+00-2.373E+00 3.853E+00 +2.003E+00-1.599E+00 \END; /*===================================================================*/ |