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| /*===================================================================*/
/* NRDF D1600 Data No.43 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,43;
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,43;
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,43;
INC-ENGY-LAB=176MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'43';
/*@43@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
6.153E+01 +3.732E+00-3.925E+00 3.619E+00 +1.655E+00-1.839E+00
6.958E+01 +1.374E+00-2.651E+00 3.136E+00 +1.500E+00-1.045E+00
7.625E+01 +2.258E+00-2.258E+00 3.577E+00 +1.867E+00-1.359E+00
8.401E+01 +3.535E+00-2.649E+00 3.381E+00 +1.201E+00-1.315E+00
9.294E+01 +3.535E+00-2.257E+00 3.105E+00 +1.291E+00-1.065E+00
1.058E+02 +2.158E+00-3.534E+00 2.938E+00 +1.869E+00-1.116E+00
1.134E+02 +2.847E+00-3.240E+00 3.818E+00 +1.909E+00-1.616E+00
\END;
/*===================================================================*/
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