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| /*===================================================================*/
/* NRDF D1600 Data No.51 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,51;
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,51;
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=(XSECTN);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,51;
INC-ENGY-LAB=176MEV;
PRJ=28SI;
TGT=74GE;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
Z-EMT XSECTN DELTA-XSECTN
(NODIM) (NODIM) (NODIM)
5.924E+00 7.704E+00 +9.829E-01-1.120E+00
7.047E+00 4.386E+00 +8.219E-01-8.507E-01
8.108E+00 6.440E+00 +9.290E-01-1.249E+00
9.081E+00 4.288E+00 +0.000E+00-0.000E+00
1.024E+01 5.468E+00 +1.010E+00-9.283E-01
1.113E+01 5.708E+00 +7.193E-01-9.305E-01
1.217E+01 1.298E+01 +7.171E-01-7.156E-01
1.311E+01 1.122E+01 +1.009E+00-8.249E-01
1.397E+01 1.583E+01 +7.163E-01-9.844E-01
1.490E+01 1.240E+01 +7.680E-01-9.541E-01
1.592E+01 1.229E+01 +6.632E-01-9.002E-01
1.684E+01 1.222E+01 +1.118E+00-6.676E-01
1.799E+01 1.236E+01 +7.459E-01-7.200E-01
1.904E+01 1.212E+01 +5.051E-01-6.632E-01
2.011E+01 1.271E+01 +5.066E-01-8.788E-01
2.109E+01 1.227E+01 +0.000E+00-0.000E+00
2.207E+01 1.269E+01 +0.000E+00-0.000E+00
2.279E+01 1.296E+01 +1.038E+00-1.140E+00
2.373E+01 1.237E+01 +0.000E+00-0.000E+00
2.461E+01 1.291E+01 +0.000E+00-0.000E+00
2.556E+01 1.246E+01 +0.000E+00-0.000E+00
2.668E+01 1.422E+01 +9.837E-01-6.395E-01
2.789E+01 1.497E+01 +1.114E+00-6.403E-01
2.885E+01 1.522E+01 +0.000E+00-0.000E+00
2.988E+01 1.461E+01 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
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