Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln<sub>2</sub>Zr<sub>2</sub>O<sub>7</sub> (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary

Sm<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0, 0.05, 0.1) and Gd<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0.05, 0.1) m...

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Main Authors: A.V. Shlyakhtina, J.C.C. Abrantes, E. Gomes, N.V. Lyskov, E.Yu. Konysheva, S.A. Chernyak, E.P. Kharitonova, O.K. Karyagina, I.V. Kolbanev, L.G. Shcherbakova
Format: Article
Language:English
Published: MDPI AG 2019-08-01
Series:Materials
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Online Access:https://www.mdpi.com/1996-1944/12/15/2452
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Summary:Sm<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0, 0.05, 0.1) and Gd<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0.05, 0.1) mixed oxides in a pyrochlore&#8722;fluorite morphotropic phase region were prepared via the mechanical activation of oxide mixtures, followed by annealing at 1600 &#176;C. The structure of the solid solutions was studied by X-ray diffraction and refined by the Rietveld method, water content was determined by thermogravimetry (TG), their bulk and grain-boundary conductivity was determined by impedance spectroscopy in dry and wet air (100&#8722;900 &#176;C), and their total conductivity was measured as a function of oxygen partial pressure in the temperature range: 700&#8722;950 &#176;C. The Sm<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0.05, 0.1) pyrochlore solid solutions, lying near the morphotropic phase boundary, have proton conductivity contribution both in the grain bulk and on grain boundaries below 600 &#176;C, and pure oxygen&#8722;ion conductivity above 700 &#176;C. The 500 &#176;C proton conductivity contribution of Sm<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0.05, 0.1) is ~ 1 &#215; 10<sup>&#8722;4</sup> S/cm. The fluorite-like Gd<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0.1) solid solution has oxygen-ion bulk conductivity in entire temperature range studied, whereas proton transport contributes to its grain-boundary conductivity below 700 &#176;C. As a result, of the morphotropic phase transition from pyrochlore Sm<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0.05, 0.1) to fluorite-like Gd<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0.05, 0.1), the bulk proton conductivity disappears and oxygen-ion conductivity decreases. The loss of bulk proton conductivity of Gd<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (x = 0.05, 0.1) can be associated with the fluorite structure formation. It is important to note that the degree of Ca substitution in such solid solutions (Ln<sub>2&#8722;x</sub>Ca<sub>x</sub>)Zr<sub>2</sub>O<sub>7&#8722;&#948;</sub> (Ln = Sm, Gd) is low, x &lt; 0.1. In both series, grain-boundary conductivity usually exceeds bulk conductivity. The high grain-boundary proton conductivity of Ln<sub>2&#8722;x</sub>Ca<sub>x</sub>Zr<sub>2</sub>O<sub>7&#8722;x/2</sub> (Ln = Sm, Gd; x = 0.1) is attributable to the formation of an intergranular CaZrO<sub>3</sub>-based cubic perovskite phase doped with Sm or Gd in Zr sublattice.
ISSN:1996-1944