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| /*===================================================================*/
/* NRDF D1600 Data No.13 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,13;
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,13;
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=(170MEV);
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,13;
INC-ENGY-LAB=170MEV;
PRJ=37CL;
TGT=64NI;
EMT=X'13';
/*@13@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DELTA-THTC X'1' DELTA-X'1'
(DEG) (DEG) (MB/RAD) (MB/RAD)
2.978E+01 +3.482E+00-3.675E+00 4.017E+00 +1.501E+00-1.115E+00
4.291E+01 +2.487E+00-4.079E+00 3.814E+00 +1.386E+00-9.975E-01
5.123E+01 +2.787E+00-4.174E+00 5.035E+00 +1.400E+00-1.526E+00
7.240E+01 +2.188E+00-2.878E+00 5.704E+00 +1.178E+00-1.641E+00
8.036E+01 +1.389E+00-2.484E+00 5.063E+00 +1.500E+00-1.131E+00
\END;
/*===================================================================*/
|