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Zhurnal Tekhnicheskoi Fiziki, 2015, Volume 85, Issue 2, Pages 1–7 (Mi jtf7676)  

Theoretical and Mathematical Physics

Isotopic effect at oxygen diffusion in imperfect crystals of cerium oxide

M. A. Kovalenko, A. Ya. Kupryazhkin

Ural Federal University named after the First President of Russia B. N. Yeltsin, Ekaterinburg
Abstract: The surface and volume diffusion of oxygen isotopes in different phase states of Ce$_{1-x}$Gd$_x$O$_{2-x/2}$ crystals are studied with the high-speed molecular dynamics method (using graphics processors). It is shown that the ratio between the oxygen isotope diffusion coefficients (the so-called isotopic effect) in the volume of simulated crystals, $D(\mathrm{O}^{16})/D(\mathrm{O}^{18})$ $\approx$ 1.05, agrees well with the well-known ratio $\sqrt{M(\mathrm{O}^{18})/M(\mathrm{O}^{16})}$ = 1.06 and does not depend on the temperature, phase state, and particle-particle interaction potential. On the surface of nanocrystals, the isotopic effect is a linear function of temperature. The ratio between diffusion coefficients of light and heavy isotopes grows with decreasing temperature and equals $D(\mathrm{O}^{16})/D(\mathrm{O}^{18}$) $\approx$ 1.12 at $T$ = 1000 K.
English version:
Technical Physics, 2015, Volume 60, Issue 1, Pages 155–161
DOI: https://doi.org/10.1134/S1063784215020127
Bibliographic databases:
Document Type: Article
Language: Russian
Citation: M. A. Kovalenko, A. Ya. Kupryazhkin, “Isotopic effect at oxygen diffusion in imperfect crystals of cerium oxide”, Zhurnal Tekhnicheskoi Fiziki, 85:2 (2015), 1–7; Tech. Phys., 60:1 (2015), 155–161
Citation in format AMSBIB
\Bibitem{KovKup15}
\by M.~A.~Kovalenko, A.~Ya.~Kupryazhkin
\paper Isotopic effect at oxygen diffusion in imperfect crystals of cerium oxide
\jour Zhurnal Tekhnicheskoi Fiziki
\yr 2015
\vol 85
\issue 2
\pages 1--7
\mathnet{http://mi.mathnet.ru/jtf7676}
\elib{https://elibrary.ru/item.asp?id=24195982}
\transl
\jour Tech. Phys.
\yr 2015
\vol 60
\issue 1
\pages 155--161
\crossref{https://doi.org/10.1134/S1063784215020127}
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