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| /*===================================================================*/
/* NRDF D1600 Data No.38 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,38;
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,38;
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,38;
INC-ENGY-LAB=176MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'38';
/*@38@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
8.327E+01 +2.621E+00-4.537E+00 3.143E+00 +1.069E+00-8.527E-01
8.941E+01 +2.220E+00-2.920E+00 2.875E+00 +1.134E+00-5.899E-01
9.477E+01 +2.319E+00-3.230E+00 3.207E+00 +9.576E-01-1.098E+00
1.001E+02 +2.219E+00-3.528E+00 2.565E+00 +1.040E+00-6.358E-01
1.046E+02 +2.222E+00-3.326E+00 2.348E+00 +9.253E-01-5.684E-01
1.105E+02 +4.135E+00-3.632E+00 2.381E+00 +7.602E-01-7.001E-01
1.171E+02 +4.138E+00-3.531E+00 1.965E+00 +5.268E-01-6.630E-01
1.258E+02 +2.523E+00-2.825E+00 2.039E+00 +7.811E-01-5.767E-01
\END;
/*===================================================================*/
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