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/* NRDF D1600 Data No.49 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,49;
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,49;
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,49;
INC-ENGY-LAB=176MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'49';
/*@49@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
5.135E+01 +4.014E+00-1.670E+00 5.701E+00 +3.631E+00-2.305E+00
6.037E+01 +2.840E+00-2.841E+00 4.837E+00 +2.872E+00-1.719E+00
6.772E+01 +2.738E+00-2.843E+00 4.937E+00 +2.722E+00-1.755E+00
7.379E+01 +1.858E+00-2.449E+00 4.836E+00 +2.566E+00-1.881E+00
7.978E+01 +2.932E+00-2.945E+00 4.315E+00 +2.745E+00-1.222E+00
8.674E+01 +5.097E+00-1.963E+00 4.011E+00 +2.213E+00-1.320E+00
9.408E+01 +3.920E+00-3.229E+00 4.094E+00 +2.011E+00-1.690E+00
1.018E+02 +2.055E+00-3.631E+00 3.860E+00 +2.544E+00-1.372E+00
\END;
/*===================================================================*/
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