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| /*===================================================================*/
/* NRDF D1600 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
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,1;
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=(ENGY);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-ENGY-LAB=176MEV;
PRJ=28SI;
TGT=74GE;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
Z-EMT ENGY-EMT DELTA-ENGY-EMT
(NODIM) (MEV) (MEV)
7.117E+00 4.574E+01 +1.628E+00-1.997E+00
8.181E+00 4.922E+01 +2.146E+00-1.997E+00
9.198E+00 5.395E+01 +1.850E+00-3.033E+00
1.014E+01 5.713E+01 +2.590E+00-1.997E+00
1.108E+01 6.001E+01 +2.738E+00-2.663E+00
1.181E+01 6.200E+01 +3.107E+00-2.515E+00
1.266E+01 6.511E+01 +3.107E+00-3.255E+00
1.357E+01 6.533E+01 +2.959E+00-3.625E+00
1.464E+01 6.747E+01 +2.441E+00-3.552E+00
1.580E+01 6.798E+01 +2.959E+00-3.847E+00
1.669E+01 6.768E+01 +3.403E+00-3.182E+00
1.790E+01 6.871E+01 +2.441E+00-3.477E+00
1.891E+01 6.730E+01 +2.146E+00-2.812E+00
1.993E+01 6.952E+01 +2.442E+00-2.664E+00
2.085E+01 7.040E+01 +2.590E+00-3.107E+00
2.169E+01 6.818E+01 +3.033E+00-2.441E+00
2.256E+01 6.936E+01 +2.441E+00-2.885E+00
2.345E+01 6.773E+01 +3.403E+00-3.033E+00
2.449E+01 6.477E+01 +2.664E+00-3.551E+00
2.546E+01 6.469E+01 +2.367E+00-3.847E+00
2.671E+01 6.106E+01 +2.812E+00-3.107E+00
\END;
/*===================================================================*/
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