/*===================================================================*/ /* NRDF D1551 Data No.5 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,5; D#=D1551; TITLE=/SYMMETRIC MASS-DIVISION PROCESS IN NUCLEI WITH MASS NUMBERS AROUND A(CN)=100/; PURPOSE=/TO ELUCIDATE THE PRESENCE OF THE SYMMETRIC MASS-DIVISION PROCESS IN LIGHT NUCLEI WITH MASS NUMBERS OF THE COMPOUND NUCLEUS A(CN)=100 AND TO STUDY THE ROLE OF ANGULAR MOMENTUM./; ATH=(Y.NAGAME'1',H.IKEZOE'1',T.OHTSUKI'1,2'); INST-ATH=(2JPNJAE'1'); /*@2@*/ REF=PR/C; VLP=47(1993)1586; RCTS=(68ZN(37CL,X)X,89Y(16O,X)X); PHQS=(A-DSTRN,ANGL-DSTRN,TOT-KIN-ENGY)'15'; /*@15@*/ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,5; RCT=89Y(16O,X)X; RTY=(CMPD-RCT,FISSN); ENR=NAT; CHM=ELM; PHYS-FORM=SLD; THK-TGT=433E-3MG/CM**2; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=(VDGT); INST-ACC=2JPNJAE; INC-ENGY-LAB=(140MEV); ERS-PRJ=XKEV; BEAM-INTNSTY=XA; CHRG-INC-ION=+8; POL-PRJ=0%; DET-PARTCL=(X'20'); /*@20@*/ COINC=NO; ANT-COINC=NO; DET-SYS=(SBD,TOF); SOLID-ANGL=XMSR; ERS-DET=XKEV; CALB-DET=/@THE ENERGY CALIBRATION WAS PERFORMED BY USING THE ELASTICALLY SCATTERD PROJECTILES FRON A 100-MICROGRAM/CM**2-THICK 197AU TARGET AT HIGH ENERGIES AND ALPHA PARTICLES FROM AN 241AM SOURCE AT LOW ENERGY.@/; ANL=(STATIST-MODEL); PHQ=(DSIGMA/DOMEGA); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,5; INC-ENGY-LAB=140MEV; CMPD=105AG; EMT=X'20'; RSD=X'20'; /*@20@*/ THTL=35DEG; NORM=X'30'; /*@30@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; MASS DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (NODIM) (MB/SR) (MB/SR) 3.300E+01 3.867E-01 +2.663E-02-2.663E-02 3.500E+01 3.292E-01 +3.031E-02-3.031E-02 3.600E+01 3.392E-01 +3.258E-02-3.258E-02 3.800E+01 3.163E-01 +4.221E-02-4.221E-02 4.000E+01 3.382E-01 +5.285E-02-5.285E-02 4.300E+01 3.096E-01 +4.362E-02-4.362E-02 4.500E+01 3.779E-01 +4.287E-02-4.287E-02 4.600E+01 3.644E-01 +3.540E-02-3.540E-02 4.800E+01 3.948E-01 +3.852E-02-3.852E-02 5.100E+01 3.568E-01 +4.886E-02-4.886E-02 5.300E+01 4.302E-01 +3.345E-02-3.345E-02 5.400E+01 4.182E-01 +2.926E-02-2.926E-02 5.600E+01 3.769E-01 +3.457E-02-3.457E-02 5.800E+01 3.064E-01 +5.780E-02-5.780E-02 6.000E+01 3.464E-01 +4.373E-02-4.373E-02 6.200E+01 2.821E-01 +5.100E-02-5.100E-02 6.400E+01 3.253E-01 +3.796E-02-3.796E-02 6.600E+01 3.007E-01 +3.835E-02-3.835E-02 6.800E+01 3.293E-01 +3.088E-02-3.088E-02 7.000E+01 3.597E-01 +3.740E-02-3.740E-02 7.200E+01 3.572E-01 +2.691E-02-2.691E-02 7.400E+01 4.092E-01 +2.409E-02-2.409E-02 \END; /*===================================================================*/ |