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| /*===================================================================*/
/* NRDF D1600 Data No.50 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,50;
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,50;
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,50;
INC-ENGY-LAB=176MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'50';
/*@50@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
5.054E+01 +3.945E+00-3.156E+00 7.776E+00 +5.193E+00-2.200E+00
5.961E+01 +2.564E+00-3.451E+00 7.099E+00 +3.320E+00-2.262E+00
6.710E+01 +2.366E+00-2.663E+00 6.650E+00 +3.237E+00-2.119E+00
7.312E+01 +2.268E+00-2.169E+00 6.153E+00 +2.879E+00-2.014E+00
7.854E+01 +2.564E+00-2.762E+00 6.069E+00 +2.287E+00-2.288E+00
8.564E+01 +2.761E+00-2.563E+00 4.754E+00 +2.047E+00-1.473E+00
9.323E+01 +3.057E+00-2.268E+00 5.061E+00 +1.997E+00-1.432E+00
1.003E+02 +3.057E+00-2.761E+00 4.865E+00 +3.250E+00-1.834E+00
1.063E+02 +3.057E+00-2.368E+00 4.860E+00 +2.183E+00-1.909E+00
\END;
/*===================================================================*/
|