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| /*===================================================================*/
/* NRDF D1305 Data No.38 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,38;
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,38;
/* 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)140LA/237NP(P,FISSN)97NB);
PHQ=EXC-FUNCT;
INC-ENGY-LAB=9[32MEV;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,38;
EMT=GAMMA'55';
/* '55' Decay data not given */
RSD=(140LA,97NB);
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-LAB XSECTN-RATIO DELTA-XSECTN-RATIO
(MEV) (NODIM) (NODIM)
9.907E+00 7.131E-01 +-2.164E-01
1.084E+01 8.508E-01 +-1.548E-01
1.194E+01 6.301E-01 +-7.608E-02
1.278E+01 7.217E-01 +-1.143E-01
1.355E+01 6.013E-01 +-1.271E-01
1.409E+01 9.084E-01 +-2.284E-01
1.478E+01 8.622E-01 +-1.443E-01
1.499E+01 6.644E-01 +-1.273E-01
1.533E+01 8.420E-01 +-1.696E-01
1.565E+01 9.875E-01 +-NEGLIGIBLE
1.653E+01 7.741E-01 +-NEGLIGIBLE
1.770E+01 5.371E-01 +-NEGLIGIBLE
1.865E+01 6.203E-01 +-NEGLIGIBLE
2.018E+01 7.684E-01 +-NEGLIGIBLE
2.085E+01 7.913E-01 +-NEGLIGIBLE
2.185E+01 7.393E-01 +-NEGLIGIBLE
2.272E+01 8.162E-01 +-NEGLIGIBLE
2.384E+01 7.058E-01 +-NEGLIGIBLE
2.486E+01 6.028E-01 +-NEGLIGIBLE
2.587E+01 7.836E-01 +-NEGLIGIBLE
2.704E+01 7.945E-01 +-NEGLIGIBLE
2.790E+01 8.019E-01 +-NEGLIGIBLE
2.882E+01 7.996E-01 +-NEGLIGIBLE
3.184E+01 7.045E-01 +-NEGLIGIBLE
\END;
/*===================================================================*/
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