/*===================================================================*/ /* NRDF D1600 Data No.30 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,30; 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,30; 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=(ANGL-DSTRN); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,30; INC-ENGY-LAB=186MEV; PRJ=37CL; TGT=64NI; EMT=X'30'; /*@30@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DELTA-THTC X'1' DELTA-X'1' (DEG) (DEG) (MB/RAD) (MB/RAD) 4.830E+01 +4.353E+00-2.919E+00 1.564E+01 +7.472E+00-4.536E+00 6.623E+01 +1.600E+00-2.923E+00 1.252E+01 +4.777E+00-3.877E+00 7.350E+01 +3.629E+00-3.135E+00 1.364E+01 +4.518E+00-4.227E+00 9.161E+01 +4.534E+00-3.136E+00 9.645E+00 +3.303E+00-3.480E+00 1.006E+02 +2.926E+00-2.733E+00 9.007E+00 +3.568E+00-2.489E+00 \END; /*===================================================================*/ |