/*===================================================================*/ /* NRDF D1600 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; 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,2; RCT=64NI(37CL,X)X; RTY=(FISSN); ENR=X%; CHM=X; PHYS-FORM=SLD; THK-TGT=280UG/CM**2; BAC=SELF; THK-BAC=XMG/CM**2; POL-TGT=0%; ALGN-TGT=0%; ACC=(LINAC); INST-ACC=2JPNJAE; INC-ENGY-LAB=(186MEV); ERS-PRJ=XKEV; BEAM-INTNSTY=10[100NA; 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,2; INC-ENGY-LAB=186MEV; PRJ=37CL; TGT=64NI; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; Z-EMT ENGY-EMT DELTA-ENGY-EMT (NODIM) (MEV) (MEV) 9.780E+00 5.405E+01 +2.429E+00-2.428E+00 1.071E+01 5.873E+01 +2.840E+00-2.881E+00 1.176E+01 6.127E+01 +2.140E+00-3.045E+00 1.259E+01 6.402E+01 +2.880E+00-2.222E+00 1.358E+01 6.549E+01 +2.512E+00-2.673E+00 1.429E+01 6.791E+01 +3.046E+00-2.799E+00 1.516E+01 6.832E+01 +3.005E+00-2.716E+00 1.624E+01 6.925E+01 +3.293E+00-2.754E+00 1.725E+01 6.895E+01 +2.840E+00-2.880E+00 1.834E+01 7.018E+01 +3.292E+00-3.375E+00 1.942E+01 6.922E+01 +2.963E+00-3.127E+00 2.056E+01 7.073E+01 +2.964E+00-2.839E+00 2.150E+01 6.965E+01 +2.797E+00-3.251E+00 2.241E+01 6.804E+01 +2.922E+00-3.249E+00 2.319E+01 6.540E+01 +3.168E+00-2.635E+00 2.406E+01 6.642E+01 +2.963E+00-2.591E+00 2.497E+01 6.476E+01 +2.798E+00-2.715E+00 2.605E+01 6.339E+01 +2.758E+00-2.385E+00 2.706E+01 6.285E+01 +2.757E+00-2.920E+00 2.821E+01 6.065E+01 +2.386E+00-2.881E+00 2.948E+01 5.673E+01 +2.922E+00-2.469E+00 3.061E+01 5.680E+01 +2.677E+00-2.756E+00 3.142E+01 5.564E+01 +2.592E+00-2.058E+00 3.255E+01 5.291E+01 +2.225E+00-2.302E+00 \END; /*===================================================================*/ |