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| /*===================================================================*/
/* NRDF D1600 Data No.36 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,36;
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,36;
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,36;
INC-ENGY-LAB=176MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'36';
/*@36@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
5.789E+01 +2.714E+00-3.816E+00 5.471E+00 +2.738E+00-1.898E+00
6.401E+01 +3.015E+00-2.009E+00 4.739E+00 +2.158E+00-1.314E+00
7.104E+01 +3.115E+00-3.214E+00 3.941E+00 +1.971E+00-1.470E+00
7.998E+01 +2.514E+00-5.323E+00 3.737E+00 +2.468E+00-1.369E+00
8.590E+01 +2.714E+00-3.715E+00 3.108E+00 +1.650E+00-8.841E-01
9.203E+01 +2.510E+00-2.915E+00 3.167E+00 +1.259E+00-9.686E-01
9.736E+01 +2.008E+00-2.511E+00 3.130E+00 +1.334E+00-1.226E+00
1.024E+02 +2.110E+00-3.011E+00 2.578E+00 +1.099E+00-8.422E-01
1.076E+02 +4.217E+00-2.512E+00 2.350E+00 +7.717E-01-9.349E-01
1.142E+02 +3.214E+00-4.524E+00 2.468E+00 +8.778E-01-9.664E-01
1.201E+02 +3.718E+00-4.021E+00 1.727E+00 +6.869E-01-5.876E-01
1.285E+02 +2.411E+00-2.514E+00 1.605E+00 +3.811E-01-5.781E-01
\END;
/*===================================================================*/
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