/*===================================================================*/ /* NRDF D1600 Data No.1 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,1; 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,1; 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=(ENGY); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,1; INC-ENGY-LAB=176MEV; PRJ=28SI; TGT=74GE; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; Z-EMT ENGY-EMT DELTA-ENGY-EMT (NODIM) (MEV) (MEV) 7.117E+00 4.574E+01 +1.628E+00-1.997E+00 8.181E+00 4.922E+01 +2.146E+00-1.997E+00 9.198E+00 5.395E+01 +1.850E+00-3.033E+00 1.014E+01 5.713E+01 +2.590E+00-1.997E+00 1.108E+01 6.001E+01 +2.738E+00-2.663E+00 1.181E+01 6.200E+01 +3.107E+00-2.515E+00 1.266E+01 6.511E+01 +3.107E+00-3.255E+00 1.357E+01 6.533E+01 +2.959E+00-3.625E+00 1.464E+01 6.747E+01 +2.441E+00-3.552E+00 1.580E+01 6.798E+01 +2.959E+00-3.847E+00 1.669E+01 6.768E+01 +3.403E+00-3.182E+00 1.790E+01 6.871E+01 +2.441E+00-3.477E+00 1.891E+01 6.730E+01 +2.146E+00-2.812E+00 1.993E+01 6.952E+01 +2.442E+00-2.664E+00 2.085E+01 7.040E+01 +2.590E+00-3.107E+00 2.169E+01 6.818E+01 +3.033E+00-2.441E+00 2.256E+01 6.936E+01 +2.441E+00-2.885E+00 2.345E+01 6.773E+01 +3.403E+00-3.033E+00 2.449E+01 6.477E+01 +2.664E+00-3.551E+00 2.546E+01 6.469E+01 +2.367E+00-3.847E+00 2.671E+01 6.106E+01 +2.812E+00-3.107E+00 \END; /*===================================================================*/ |