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| /*===================================================================*/
/* NRDF D1600 Data No.39 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,39;
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,39;
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,39;
INC-ENGY-LAB=176MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'39';
/*@39@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
8.034E+01 +3.011E+00-3.718E+00 1.652E+00 +6.432E-01-5.226E-01
8.676E+01 +2.211E+00-2.412E+00 1.501E+00 +5.426E-01-4.853E-01
9.188E+01 +2.013E+00-2.005E+00 1.528E+00 +7.071E-01-3.583E-01
9.670E+01 +2.010E+00-2.303E+00 1.508E+00 +6.306E-01-4.878E-01
1.019E+02 +2.108E+00-2.306E+00 1.385E+00 +6.614E-01-3.141E-01
1.078E+02 +3.214E+00-3.514E+00 1.395E+00 +7.098E-01-4.705E-01
1.136E+02 +2.614E+00-4.013E+00 1.179E+00 +5.109E-01-3.043E-01
1.234E+02 +3.312E+00-3.117E+00 1.080E+00 +3.903E-01-4.003E-01
\END;
/*===================================================================*/
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