Measurement of 89Y(n,2n) spectral averaged cross section in LR-0 special core reactor spectrum

The present paper describes reaction rate measurement of 89Y(n,2n)88Y in a well-defined reactor spectrum of a special core assembled in the LR-0 reactor and compares this value with results of simulation. The reaction rate is derived from the measurement of activity of 88Y using gamma-ray spectromet...

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Veröffentlicht in:Radiation physics and chemistry (Oxford, England : 1993) England : 1993), 2017-12, Vol.141, p.22-28
Hauptverfasser: Košťál, Michal, Losa, Evžen, Baroň, Petr, Šolc, Jaroslav, Švadlenková, Marie, Koleška, Michal, Mareček, Martin, Uhlíř, Jan
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Sprache:eng
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Zusammenfassung:The present paper describes reaction rate measurement of 89Y(n,2n)88Y in a well-defined reactor spectrum of a special core assembled in the LR-0 reactor and compares this value with results of simulation. The reaction rate is derived from the measurement of activity of 88Y using gamma-ray spectrometry of irradiated Y2O3 sample. The resulting cross section value averaged in spectrum is 43.9 ± 1.5 µb, averaged in the 235U spectrum is 0.172 ± 0.006mb. This cross-section is important as it is used as high energy neutron monitor and is therefore included in the International Reactor Dosimetry and Fusion File. Calculations of reaction rates were performed with the MCNP6 code using ENDF/B-VII.0, JEFF-3.1, JEFF-3.2, JENDL-3.3, JENDL-4, ROSFOND-2010, CENDL-3.1 and IRDFF nuclear data libraries. The agreement with uranium description by CIELO library is very good, while in ENDF/B-VII.0 description of uranium, underprediction about 10% in average can be observed. •Determination of 89Y reaction rate in irradiated Y2O3 sample.•Experimental spectral average cross section of 89Y(n,2n) reaction.•Calculation of reaction rate 89Y(n,2n) reaction.•Discrepancies between calculation and experiment.
ISSN:0969-806X
1879-0895
DOI:10.1016/j.radphyschem.2017.05.027