|
| /*===================================================================*/
/* NRDF D1305 Data No.7 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,7;
D#=D1305;
TITLE=/Systematic analysis of mass yield curves in low-energy fission
of actinides/;
ATH=(T.OHTSUKI'1', Y.HAMAJIMA'1', K.SUEKI'1', H.NAKAHARA'1',
Y.NAGAME'2', N.SHINOHARA'2', H.IKEZOE'2');
INST-ATH=(2JPNTMU'1', 2JPNJAE'2');
/* '1' Department of Chemistry, Faculty of Science */
REF=PR/C;
VLP=40(1989)2144;
RCTS=(233U(P,FISSN), 235U(P,FISSN), 237NP(P,FISSN), 238U(P,FISSN),
239PU(P,FISSN), 242PU(P,FISSN), 244PU(P,FISSN), 241AM(P,FISSN),
243AM(P,FISSN), (P,FISSN), 237NP(P,FISSN)85KR,
237NP(P,FISSN)97NB, 237NP(P,FISSN)87KR, 237NP(P,FISSN)88KR,
237NP(P,FISSN)91SR, 237NP(P,FISSN)92SR, 237NP(P,FISSN)93Y,
237NP(P,FISSN)95ZR, 237NP(P,FISSN)99MO, 237NP(P,FISSN)103RU,
237NP(P,FISSN)105RH, 237NP(P,FISSN)111AG, 237NP(P,FISSN)112PD,
237NP(P,FISSN)113AG, 237NP(P,FISSN)115CD, 237NP(P,FISSN)117CD,
237NP(P,FISSN)126SB);
PHQS=(A-DSTRN, DATA'3', DATA'4', DATA'5', EXC-FUNCT);
/* '3' Weighted mean peak positions of heavy asymmetric peak */
/* '4' Weighted mean peak positions of light asymmetric peak */
/* '5' Full width at half maximum of asymnetric peak */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,7;
/* 2004-03-25 : Converted, Data converted to EXFOR E1305 */
RTY=(FISSN,FISSN,FISSN);
ENR=>99%;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=0.100[0.300MG/CM**2'6';
/* '6' Thickness was determined by alpha spectrometry */
BAC=AL'7';
/* '7' Electrodeposited on Al foil and wrapped with a sheet of Al
foil */
THK-BAC=6MG/CM**2;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=(VDGT'8',CYC'9');
/* '9' Isochronous cyclotron */
INST-ACC=(2JPNJAE'8',2JPNINS'9');
BEAM-INTNSTY=[1UA;
POL-PRJ=0%;
DET-PARTCL=GAMMA'10';
/* '10' . Decay data not given */
COINC=NO;
ANT-COINC=NO;
DET-SYS=GE(LI)'11';
/* '11' To detect decay gamma */
/* Experimental Method:
- Activation
/* Analysis:
- Mass yield curves were constructed from the observed cross
section of each fission product to which a correction was
applied, when necessary, for the charge distribution by assuming
a Gaussian charge distribution with the most probable charge Zp
of unchanged-charge division. The Gaussian width parameter of
0.95 was used as suggested by McHugh et al. [J.A. Mchugh and M.C.
Michel, Phys. ReV. 172(1968)1160].
RCT=244PU(P,FISSN);
PHQ=A-DSTRN;
INC-ENGY-LAB=12MEV;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,7;
INC-ENGY-LAB=12MEV;
TOT-ERR=[10%;
EMT=GAMMA'18';
/* '18' Decay data not given */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
A YLD
(NODIM) (%)
8.453E+01 4.431E-01
8.897E+01 8.225E-01
9.215E+01 1.390E+00
9.313E+01 1.310E+00
9.818E+01 2.630E+00
9.972E+01 4.054E+00
1.028E+02 4.844E+00
1.045E+02 6.068E+00
1.112E+02 3.793E+00
1.126E+02 2.285E+00
1.137E+02 1.575E+00
1.151E+02 9.930E-01
1.170E+02 6.683E-01
1.264E+02 1.397E+00
1.287E+02 1.795E+00
1.310E+02 4.117E+00
1.323E+02 5.941E+00
1.353E+02 5.940E+00
1.387E+02 4.956E+00
1.395E+02 4.118E+00
1.404E+02 3.568E+00
1.422E+02 2.763E+00
1.475E+02 1.397E+00
1.507E+02 1.415E+00
1.532E+02 6.807E-01
\END;
/*===================================================================*/
|