Cargando…

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...

Descripción completa

Detalles Bibliográficos
Autores principales: 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.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2019
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
_version_ 1783444190136369152
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
work_keys_str_mv AT shlyakhtinaav evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT abrantesjcc evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT gomese evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT lyskovnv evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT konyshevaeyu evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT chernyaksa evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT kharitonovaep evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT karyaginaok evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT kolbaneviv evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary
AT shcherbakovalg evolutionofoxygenionandprotonconductivityincadopedln2zr2o7lnsmgdlocatednearpyrochlorefluoritephaseboundary