Abstract
Propagation of an ion in a solid involves the penetration of a rather large species through a structure, which, from the point of view of the ion, is densely populated. One would, therefore, expect small ion (cation) motion to be more likely than large ion (anion) motion. While this is indeed the trend, fast anionic conduction in crystalline solids can be observed at elevated temperatures where conductivities of the order of 1 ohm- 1 -cm- 1 are measured.
The most intensively investigated anionic conductors are those conducting oxygen and fluorine ions. However, conduction of other anions, in particular halogen ions, has been observed.
We discuss the following topics: The various conduction mechanisms, crystalline structures and defect structures that enable the conduction of anions. Special emphasis will be on the fluorite structure. Typical examples of fast O2 — and F−conductors will be discussed in detail.
Data collected from a range of different experimental methods for the same material or group of materials will be presented. This will constitute the main part of the lecture.
We shall close the presentation with short references to a) application of fast anion conductors, and b) “high temperature” superconductor oxides, the crystalline and defect structure of which are rather close to some of the oxide fast ionic conductors that will be discussed.
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© 1989 Plenum Press, New York
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Riess, I. (1989). Crystalline Anionic Fast Ion Conduction. In: Tuller, H.L., Balkanski, M. (eds) Science and Technology of Fast Ion Conductors. NATO ASI Series, vol 199. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-0509-5_2
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DOI: https://doi.org/10.1007/978-1-4613-0509-5_2
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