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| /*===================================================================*/
/* NRDF D1600 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
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,2;
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=(186MEV);
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,2;
INC-ENGY-LAB=186MEV;
PRJ=37CL;
TGT=64NI;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
Z-EMT ENGY-EMT DELTA-ENGY-EMT
(NODIM) (MEV) (MEV)
9.780E+00 5.405E+01 +2.429E+00-2.428E+00
1.071E+01 5.873E+01 +2.840E+00-2.881E+00
1.176E+01 6.127E+01 +2.140E+00-3.045E+00
1.259E+01 6.402E+01 +2.880E+00-2.222E+00
1.358E+01 6.549E+01 +2.512E+00-2.673E+00
1.429E+01 6.791E+01 +3.046E+00-2.799E+00
1.516E+01 6.832E+01 +3.005E+00-2.716E+00
1.624E+01 6.925E+01 +3.293E+00-2.754E+00
1.725E+01 6.895E+01 +2.840E+00-2.880E+00
1.834E+01 7.018E+01 +3.292E+00-3.375E+00
1.942E+01 6.922E+01 +2.963E+00-3.127E+00
2.056E+01 7.073E+01 +2.964E+00-2.839E+00
2.150E+01 6.965E+01 +2.797E+00-3.251E+00
2.241E+01 6.804E+01 +2.922E+00-3.249E+00
2.319E+01 6.540E+01 +3.168E+00-2.635E+00
2.406E+01 6.642E+01 +2.963E+00-2.591E+00
2.497E+01 6.476E+01 +2.798E+00-2.715E+00
2.605E+01 6.339E+01 +2.758E+00-2.385E+00
2.706E+01 6.285E+01 +2.757E+00-2.920E+00
2.821E+01 6.065E+01 +2.386E+00-2.881E+00
2.948E+01 5.673E+01 +2.922E+00-2.469E+00
3.061E+01 5.680E+01 +2.677E+00-2.756E+00
3.142E+01 5.564E+01 +2.592E+00-2.058E+00
3.255E+01 5.291E+01 +2.225E+00-2.302E+00
\END;
/*===================================================================*/
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