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Diffusion of oxygen in amorphous Al2O3, Ta2O5, and Nb2O5.

Authors :
Nakamura, R.
Toda, T.
Tsukui, S.
Tane, M.
Ishimaru, M.
Suzuki, T.
Nakajima, H.
Source :
Journal of Applied Physics; 2014, Vol. 116 Issue 3, p033504-1-033504-8, 8p, 1 Diagram, 3 Charts, 8 Graphs
Publication Year :
2014

Abstract

The self-diffusivity of oxygen in amorphous Al<subscript>2</subscript>O<subscript>3</subscript> (a-Al<subscript>2</subscript>O<subscript>3</subscript>), a-Ta<subscript>2</subscript>O<subscript>5</subscript>, and a-Nb<subscript>2</subscript>O<subscript>5</subscript> was investigated along with structural analysis in terms of pair distribution function (PDF). The low activation energy, ~1.2 eV, for diffusion in the oxides suggests a single atomic jump of oxygen ions mediated via vacancy-like defects. However, the pre-exponential factor for a-Ta<subscript>2</subscript>O<subscript>5</subscript> and a-Nb<subscript>2</subscript>O<subscript>5</subscript> with lower bond energy was two orders of magnitude larger than that for a-Al<subscript>2</subscript>O<subscript>3</subscript> with higher bond energy. PDF analyses revealed that the short-range configuration in a-Ta<subscript>2</subscript>O<subscript>5</subscript> and a-Nb<subscript>2</subscript>O<subscript>5</subscript> was more broadly distributed than that in a-Al<subscript>2</subscript>O<subscript>3</subscript>. Due to the larger variety of atomic configurations of a-Ta<subscript>2</subscript>O<subscript>5</subscript> and a-Nb<subscript>2</subscript>O<subscript>5</subscript>, these oxides have a higher activation entropy for diffusion than a-Al<subscript>2</subscript>O<subscript>3</subscript>. The entropy term for diffusion associated with short-range structures was shown to be a dominant factor for diffusion in amorphous oxides. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00218979
Volume :
116
Issue :
3
Database :
Complementary Index
Journal :
Journal of Applied Physics
Publication Type :
Academic Journal
Accession number :
97191852
Full Text :
https://doi.org/10.1063/1.4889800