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| /*===================================================================*/
/* NRDF D1600 Data No.30 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,30;
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,30;
RCT=64NI(37CL,X)X;
RTY=(FISSN);
ENR=X%;
CHM=X;
PHYS-FORM=SLD;
THK-TGT=280UG/CM**2;
BAC=SELF;
THK-BAC=XMG/CM**2;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=(LINAC);
INST-ACC=2JPNJAE;
INC-ENGY-LAB=(186MEV);
ERS-PRJ=XKEV;
BEAM-INTNSTY=10[100NA;
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,30;
INC-ENGY-LAB=186MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'30';
/*@30@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
4.830E+01 +4.353E+00-2.919E+00 1.564E+01 +7.472E+00-4.536E+00
6.623E+01 +1.600E+00-2.923E+00 1.252E+01 +4.777E+00-3.877E+00
7.350E+01 +3.629E+00-3.135E+00 1.364E+01 +4.518E+00-4.227E+00
9.161E+01 +4.534E+00-3.136E+00 9.645E+00 +3.303E+00-3.480E+00
1.006E+02 +2.926E+00-2.733E+00 9.007E+00 +3.568E+00-2.489E+00
\END;
/*===================================================================*/
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