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/* NRDF D1305 Data No.10 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,10;
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,10;
/* 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=(P,FISSN);
PHQ=DATA'21';
/* '21' Weighted mean peak positions of heavy asymmetric peak */
INC-ENGY-LAB=12MEV;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,10;
INC-ENGY-LAB=12MEV;
EMT=GAMMA'22';
/* '22' Decay data not given */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
A-CMPD DATA1'23' DELTA-DATA1'23'
(NODIM) (NODIM) (NODIM)
233 1.391E+02 +-2.040E+00
234 1.339E+02 +-1.966E+00
236 1.363E+02 +-2.662E+00
238 1.350E+02 +-1.573E+00
239 1.352E+02 +-1.526E+00
240 1.342E+02 +-1.829E+00
242 1.361E+02 +-1.620E+00
243 1.362E+02 +-2.756E+00
244 1.382E+02 +-1.806E+00
245 1.355E+02 +-2.175E+00
\END;
/*===================================================================*/
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