/*===================================================================*/ /* NRDF D1600 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; 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,3; 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=(170MEV); 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,3; INC-ENGY-LAB=170MEV; PRJ=37CL; TGT=64NI; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; Z-EMT ENGY-EMT DELTA-ENGY-EMT (NODIM) (MEV) (MEV) 5.676E+00 3.566E+01 +1.633E+00-1.530E+00 6.757E+00 4.123E+01 +1.424E+00-1.951E+00 7.840E+00 4.728E+01 +2.003E+00-2.161E+00 8.934E+00 4.937E+01 +1.794E+00-1.948E+00 1.013E+01 5.294E+01 +1.899E+00-2.371E+00 1.116E+01 5.719E+01 +2.373E+00-2.478E+00 1.209E+01 6.050E+01 +2.479E+00-2.581E+00 1.299E+01 6.312E+01 +2.530E+00-2.583E+00 1.380E+01 6.632E+01 +1.529E+00-4.007E+00 1.465E+01 6.642E+01 +2.215E+00-2.476E+00 1.557E+01 6.856E+01 +2.319E+00-2.899E+00 1.668E+01 6.702E+01 +2.213E+00-2.895E+00 1.755E+01 6.869E+01 +2.422E+00-2.741E+00 1.882E+01 7.036E+01 +2.322E+00-2.951E+00 1.995E+01 6.966E+01 +2.478E+00-2.635E+00 2.088E+01 7.117E+01 +3.161E+00-2.898E+00 2.193E+01 6.900E+01 +2.794E+00-2.793E+00 2.285E+01 6.761E+01 +2.478E+00-2.844E+00 2.355E+01 6.655E+01 +2.370E+00-3.109E+00 2.439E+01 6.485E+01 +2.530E+00-3.585E+00 2.533E+01 6.331E+01 +2.425E+00-3.532E+00 2.644E+01 6.277E+01 +2.846E+00-3.321E+00 2.756E+01 5.748E+01 +2.267E+00-2.900E+00 2.883E+01 5.498E+01 +2.744E+00-2.739E+00 \END; /*===================================================================*/ |