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Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln(2)Zr(2)O(7) (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary
Sm(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0, 0.05, 0.1) and Gd(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1) mixed oxides in a pyrochlore–fluorite morphotropic phase region were prepared via the mechanical activation of oxide mixtures, followed by annealing at 1600 °C. The structure of the solid solutions was studied...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6696096/ https://www.ncbi.nlm.nih.gov/pubmed/31374863 http://dx.doi.org/10.3390/ma12152452 |
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author | Shlyakhtina, A.V. Abrantes, J.C.C. Gomes, E. Lyskov, N.V. Konysheva, E.Yu. Chernyak, S.A. Kharitonova, E.P. Karyagina, O.K. Kolbanev, I.V. Shcherbakova, L.G. |
author_facet | Shlyakhtina, A.V. Abrantes, J.C.C. Gomes, E. Lyskov, N.V. Konysheva, E.Yu. Chernyak, S.A. Kharitonova, E.P. Karyagina, O.K. Kolbanev, I.V. Shcherbakova, L.G. |
author_sort | Shlyakhtina, A.V. |
collection | PubMed |
description | Sm(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0, 0.05, 0.1) and Gd(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1) mixed oxides in a pyrochlore–fluorite morphotropic phase region were prepared via the mechanical activation of oxide mixtures, followed by annealing at 1600 °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 (100–900 °C), and their total conductivity was measured as a function of oxygen partial pressure in the temperature range: 700–950 °C. The Sm(2−x)Ca(x)Zr(2)O(7−x/2) (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 °C, and pure oxygen–ion conductivity above 700 °C. The 500 °C proton conductivity contribution of Sm(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1) is ~ 1 × 10(−4) S/cm. The fluorite-like Gd(2−x)Ca(x)Zr(2)O(7−x/2) (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 °C. As a result, of the morphotropic phase transition from pyrochlore Sm(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1) to fluorite-like Gd(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1), the bulk proton conductivity disappears and oxygen-ion conductivity decreases. The loss of bulk proton conductivity of Gd(2−x)Ca(x)Zr(2)O(7−x/2) (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(2−x)Ca(x))Zr(2)O(7−δ) (Ln = Sm, Gd) is low, x < 0.1. In both series, grain-boundary conductivity usually exceeds bulk conductivity. The high grain-boundary proton conductivity of Ln(2−x)Ca(x)Zr(2)O(7−x/2) (Ln = Sm, Gd; x = 0.1) is attributable to the formation of an intergranular CaZrO(3)-based cubic perovskite phase doped with Sm or Gd in Zr sublattice. |
format | Online Article Text |
id | pubmed-6696096 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-66960962019-09-05 Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln(2)Zr(2)O(7) (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary Shlyakhtina, A.V. Abrantes, J.C.C. Gomes, E. Lyskov, N.V. Konysheva, E.Yu. Chernyak, S.A. Kharitonova, E.P. Karyagina, O.K. Kolbanev, I.V. Shcherbakova, L.G. Materials (Basel) Article Sm(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0, 0.05, 0.1) and Gd(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1) mixed oxides in a pyrochlore–fluorite morphotropic phase region were prepared via the mechanical activation of oxide mixtures, followed by annealing at 1600 °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 (100–900 °C), and their total conductivity was measured as a function of oxygen partial pressure in the temperature range: 700–950 °C. The Sm(2−x)Ca(x)Zr(2)O(7−x/2) (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 °C, and pure oxygen–ion conductivity above 700 °C. The 500 °C proton conductivity contribution of Sm(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1) is ~ 1 × 10(−4) S/cm. The fluorite-like Gd(2−x)Ca(x)Zr(2)O(7−x/2) (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 °C. As a result, of the morphotropic phase transition from pyrochlore Sm(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1) to fluorite-like Gd(2−x)Ca(x)Zr(2)O(7−x/2) (x = 0.05, 0.1), the bulk proton conductivity disappears and oxygen-ion conductivity decreases. The loss of bulk proton conductivity of Gd(2−x)Ca(x)Zr(2)O(7−x/2) (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(2−x)Ca(x))Zr(2)O(7−δ) (Ln = Sm, Gd) is low, x < 0.1. In both series, grain-boundary conductivity usually exceeds bulk conductivity. The high grain-boundary proton conductivity of Ln(2−x)Ca(x)Zr(2)O(7−x/2) (Ln = Sm, Gd; x = 0.1) is attributable to the formation of an intergranular CaZrO(3)-based cubic perovskite phase doped with Sm or Gd in Zr sublattice. MDPI 2019-08-01 /pmc/articles/PMC6696096/ /pubmed/31374863 http://dx.doi.org/10.3390/ma12152452 Text en © 2019 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Shlyakhtina, A.V. Abrantes, J.C.C. Gomes, E. Lyskov, N.V. Konysheva, E.Yu. Chernyak, S.A. Kharitonova, E.P. Karyagina, O.K. Kolbanev, I.V. Shcherbakova, L.G. Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln(2)Zr(2)O(7) (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary |
title | Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln(2)Zr(2)O(7) (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary |
title_full | Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln(2)Zr(2)O(7) (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary |
title_fullStr | Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln(2)Zr(2)O(7) (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary |
title_full_unstemmed | Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln(2)Zr(2)O(7) (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary |
title_short | Evolution of Oxygen–Ion and Proton Conductivity in Ca-Doped Ln(2)Zr(2)O(7) (Ln = Sm, Gd), Located Near Pyrochlore–Fluorite Phase Boundary |
title_sort | evolution of oxygen–ion and proton conductivity in ca-doped ln(2)zr(2)o(7) (ln = sm, gd), located near pyrochlore–fluorite phase boundary |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6696096/ https://www.ncbi.nlm.nih.gov/pubmed/31374863 http://dx.doi.org/10.3390/ma12152452 |
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