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| /*===================================================================*/
/* NRDF D1600 Data No.33 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,33;
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,33;
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,33;
INC-ENGY-LAB=176MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'33';
/*@33@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
5.141E+01 +1.743E+00-2.749E+00 9.315E+00 +2.516E+00-3.128E+00
5.799E+01 +2.666E+00-3.784E+00 7.481E+00 +2.107E+00-2.898E+00
6.446E+01 +2.460E+00-2.658E+00 6.976E+00 +2.157E+00-2.343E+00
7.297E+01 +3.077E+00-3.688E+00 6.397E+00 +1.976E+00-2.589E+00
8.106E+01 +2.882E+00-2.652E+00 6.161E+00 +2.566E+00-2.418E+00
8.763E+01 +2.881E+00-2.052E+00 5.746E+00 +1.627E+00-2.040E+00
9.236E+01 +1.930E+00-1.342E+00 5.135E+00 +1.720E+00-1.476E+00
9.838E+01 +1.959E+00-2.447E+00 5.502E+00 +1.414E+00-2.059E+00
1.111E+02 +2.665E+00-3.287E+00 3.442E+00 +1.587E+00-9.169E-01
1.178E+02 +2.756E+00-4.008E+00 3.276E+00 +2.165E+00-1.010E+00
\END;
/*===================================================================*/
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