/*===================================================================*/ /* NRDF D1600 Data No.49 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,49; 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,49; 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,49; INC-ENGY-LAB=176MEV; PRJ=37CL; TGT=64NI; EMT=X'49'; /*@49@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DELTA-THTC X'1' DELTA-X'1' (DEG) (DEG) (MB/RAD) (MB/RAD) 5.135E+01 +4.014E+00-1.670E+00 5.701E+00 +3.631E+00-2.305E+00 6.037E+01 +2.840E+00-2.841E+00 4.837E+00 +2.872E+00-1.719E+00 6.772E+01 +2.738E+00-2.843E+00 4.937E+00 +2.722E+00-1.755E+00 7.379E+01 +1.858E+00-2.449E+00 4.836E+00 +2.566E+00-1.881E+00 7.978E+01 +2.932E+00-2.945E+00 4.315E+00 +2.745E+00-1.222E+00 8.674E+01 +5.097E+00-1.963E+00 4.011E+00 +2.213E+00-1.320E+00 9.408E+01 +3.920E+00-3.229E+00 4.094E+00 +2.011E+00-1.690E+00 1.018E+02 +2.055E+00-3.631E+00 3.860E+00 +2.544E+00-1.372E+00 \END; /*===================================================================*/ |