/*===================================================================*/ /* NRDF D1551 Data No.4 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,4; 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,4; 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,4; INC-ENGY-LAB=140MEV; CMPD=105AG; EMT=X'20'; RSD=X'20'; /*@20@*/ THTL=15DEG; NORM=X'30'; /*@30@*/ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; MASS DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (NODIM) (MB/SR) (MB/SR) 3.600E+01 5.324E-01 +3.145E-02-3.145E-02 3.800E+01 4.687E-01 +3.259E-02-3.259E-02 4.100E+01 3.976E-01 +2.126E-02-2.126E-02 4.300E+01 4.164E-01 +2.777E-02-2.777E-02 4.500E+01 4.153E-01 +2.976E-02-2.976E-02 4.600E+01 4.451E-01 +3.968E-02-3.968E-02 4.800E+01 4.596E-01 +2.778E-02-2.778E-02 5.100E+01 4.489E-01 +3.740E-02-3.740E-02 5.300E+01 3.954E-01 +5.082E-02-5.082E-02 5.400E+01 4.615E-01 +3.881E-02-3.881E-02 5.600E+01 4.367E-01 +3.314E-02-3.314E-02 5.800E+01 4.075E-01 +2.666E-02-2.666E-02 6.100E+01 3.982E-01 +1.927E-02-1.927E-02 6.200E+01 4.102E-01 +3.796E-02-3.796E-02 6.400E+01 4.256E-01 +3.825E-02-3.825E-02 6.800E+01 4.608E-01 +2.693E-02-2.693E-02 7.000E+01 5.226E-01 +2.551E-02-2.551E-02 \END; /*===================================================================*/ |