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| /*===================================================================*/
/* NRDF D1600 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
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,3;
RCT=64NI(37CL,X)X;
RTY=(FISSN);
ENR=X%;
CHM=X;
PHYS-FORM=SLD;
THK-TGT=280UG/CM**2;
BAC=SELF;
THK-BAC=XMG/CM**2;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=(LINAC);
INST-ACC=2JPNJAE;
INC-ENGY-LAB=(170MEV);
ERS-PRJ=XKEV;
BEAM-INTNSTY=10[100NA;
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=(ENGY);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,3;
INC-ENGY-LAB=170MEV;
PRJ=37CL;
TGT=64NI;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
Z-EMT ENGY-EMT DELTA-ENGY-EMT
(NODIM) (MEV) (MEV)
5.676E+00 3.566E+01 +1.633E+00-1.530E+00
6.757E+00 4.123E+01 +1.424E+00-1.951E+00
7.840E+00 4.728E+01 +2.003E+00-2.161E+00
8.934E+00 4.937E+01 +1.794E+00-1.948E+00
1.013E+01 5.294E+01 +1.899E+00-2.371E+00
1.116E+01 5.719E+01 +2.373E+00-2.478E+00
1.209E+01 6.050E+01 +2.479E+00-2.581E+00
1.299E+01 6.312E+01 +2.530E+00-2.583E+00
1.380E+01 6.632E+01 +1.529E+00-4.007E+00
1.465E+01 6.642E+01 +2.215E+00-2.476E+00
1.557E+01 6.856E+01 +2.319E+00-2.899E+00
1.668E+01 6.702E+01 +2.213E+00-2.895E+00
1.755E+01 6.869E+01 +2.422E+00-2.741E+00
1.882E+01 7.036E+01 +2.322E+00-2.951E+00
1.995E+01 6.966E+01 +2.478E+00-2.635E+00
2.088E+01 7.117E+01 +3.161E+00-2.898E+00
2.193E+01 6.900E+01 +2.794E+00-2.793E+00
2.285E+01 6.761E+01 +2.478E+00-2.844E+00
2.355E+01 6.655E+01 +2.370E+00-3.109E+00
2.439E+01 6.485E+01 +2.530E+00-3.585E+00
2.533E+01 6.331E+01 +2.425E+00-3.532E+00
2.644E+01 6.277E+01 +2.846E+00-3.321E+00
2.756E+01 5.748E+01 +2.267E+00-2.900E+00
2.883E+01 5.498E+01 +2.744E+00-2.739E+00
\END;
/*===================================================================*/
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