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/* NRDF D1305 Data No.27 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,27;
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,27;
/* 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=(237NP(P,FISSN)117CD/237NP(P,FISSN)97NB);
PHQ=EXC-FUNCT;
INC-ENGY-LAB=9[32MEV;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,27;
EMT=GAMMA'44';
/* '44' Decay data not given */
RSD=(117CD,97NB);
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB XSECTN-RATIO DELTA-XSECTN-RATIO
(MEV) (NODIM) (NODIM)
1.156E+01 1.447E-02 +-4.311E-03
1.236E+01 1.424E-02 +-3.682E-03
1.282E+01 1.164E-02 +-2.754E-03
1.326E+01 2.300E-02 +-4.941E-03
1.358E+01 1.540E-02 +-4.144E-03
1.420E+01 1.387E-02 +-4.531E-03
1.421E+01 2.691E-02 +-3.672E-03
1.464E+01 2.624E-02 +-NEGLIGIBLE
1.485E+01 2.780E-02 +-8.283E-03
1.522E+01 2.734E-02 +-4.993E-03
1.615E+01 4.339E-02 +-6.364E-03
1.728E+01 3.279E-02 +-4.980E-03
1.836E+01 5.229E-02 +-7.947E-03
1.966E+01 4.739E-02 +-6.928E-03
2.031E+01 5.614E-02 +-NEGLIGIBLE
2.130E+01 5.529E-02 +-NEGLIGIBLE
2.219E+01 6.027E-02 +-NEGLIGIBLE
2.439E+01 4.199E-02 +-NEGLIGIBLE
2.543E+01 7.250E-02 +-1.475E-02
3.140E+01 8.819E-02 +-2.036E-02
\END;
/*===================================================================*/
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