|
| /*===================================================================*/
/* 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;
/*===================================================================*/
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