/*===================================================================*/ /* NRDF D1600 Data No.36 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,36; 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,36; 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,36; INC-ENGY-LAB=176MEV; PRJ=37CL; TGT=64NI; EMT=X'36'; /*@36@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DELTA-THTC X'1' DELTA-X'1' (DEG) (DEG) (MB/RAD) (MB/RAD) 5.789E+01 +2.714E+00-3.816E+00 5.471E+00 +2.738E+00-1.898E+00 6.401E+01 +3.015E+00-2.009E+00 4.739E+00 +2.158E+00-1.314E+00 7.104E+01 +3.115E+00-3.214E+00 3.941E+00 +1.971E+00-1.470E+00 7.998E+01 +2.514E+00-5.323E+00 3.737E+00 +2.468E+00-1.369E+00 8.590E+01 +2.714E+00-3.715E+00 3.108E+00 +1.650E+00-8.841E-01 9.203E+01 +2.510E+00-2.915E+00 3.167E+00 +1.259E+00-9.686E-01 9.736E+01 +2.008E+00-2.511E+00 3.130E+00 +1.334E+00-1.226E+00 1.024E+02 +2.110E+00-3.011E+00 2.578E+00 +1.099E+00-8.422E-01 1.076E+02 +4.217E+00-2.512E+00 2.350E+00 +7.717E-01-9.349E-01 1.142E+02 +3.214E+00-4.524E+00 2.468E+00 +8.778E-01-9.664E-01 1.201E+02 +3.718E+00-4.021E+00 1.727E+00 +6.869E-01-5.876E-01 1.285E+02 +2.411E+00-2.514E+00 1.605E+00 +3.811E-01-5.781E-01 \END; /*===================================================================*/ |