/*===================================================================*/ /* NRDF D1600 Data No.39 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,39; 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,39; 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,39; INC-ENGY-LAB=176MEV; PRJ=37CL; TGT=64NI; EMT=X'39'; /*@39@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DELTA-THTC X'1' DELTA-X'1' (DEG) (DEG) (MB/RAD) (MB/RAD) 8.034E+01 +3.011E+00-3.718E+00 1.652E+00 +6.432E-01-5.226E-01 8.676E+01 +2.211E+00-2.412E+00 1.501E+00 +5.426E-01-4.853E-01 9.188E+01 +2.013E+00-2.005E+00 1.528E+00 +7.071E-01-3.583E-01 9.670E+01 +2.010E+00-2.303E+00 1.508E+00 +6.306E-01-4.878E-01 1.019E+02 +2.108E+00-2.306E+00 1.385E+00 +6.614E-01-3.141E-01 1.078E+02 +3.214E+00-3.514E+00 1.395E+00 +7.098E-01-4.705E-01 1.136E+02 +2.614E+00-4.013E+00 1.179E+00 +5.109E-01-3.043E-01 1.234E+02 +3.312E+00-3.117E+00 1.080E+00 +3.903E-01-4.003E-01 \END; /*===================================================================*/ |