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The intrinsic origin of the grain-boundary resistance in Sr-doped LaGaO(3)
ABSTRACT: In this paper I summarize our recent investigations (Park and Kim, Phys Chem C 111:14903, 2007; Solid State Ionics 179:1329, 2008) on the origin of the grain-boundary resistance in a doped LaGaO(3), a perovskite-structured solid electrolyte. The partial electronic and ionic resistances of...
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Springer Vienna
2009
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4494845/ https://www.ncbi.nlm.nih.gov/pubmed/26166849 http://dx.doi.org/10.1007/s00706-009-0136-4 |
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author | Kim, Sangtae |
author_facet | Kim, Sangtae |
author_sort | Kim, Sangtae |
collection | PubMed |
description | ABSTRACT: In this paper I summarize our recent investigations (Park and Kim, Phys Chem C 111:14903, 2007; Solid State Ionics 179:1329, 2008) on the origin of the grain-boundary resistance in a doped LaGaO(3), a perovskite-structured solid electrolyte. The partial electronic and ionic resistances of the bulk and the grain boundaries, as well as the total resistance, in 1 mol% Sr-doped LaGaO(3) were measured separately by means of a dc-polarization method and ac-impedance spectroscopy. Both of the partial resistances at the grain boundaries were greater than the bulk counterparts, indicating that the grain boundaries impede the ionic as well as the electronic transport in this material. The transference number of the partial electronic conductivity at the grain boundary was however greater than that in the bulk. This fact strongly suggests that both electronic and ionic charge carriers deplete at the grain boundaries to form the space-charge zones and that the grain-boundary cores in this material are positively charged. In light of the fact that the effective charge of the oxygen vacancy (+2) is greater than that of the electron hole (+1), the oxygen vacancies deplete more sharply in the space-charge zones compared to the electron holes such that the grain boundaries become more mixed conducting relative to the bulk. These observations verify that the electrical conduction across the grain-boundaries in 1 mol% Sr-doped LaGaO(3) is governed by the space charge. GRAPHICAL ABSTRACT: [Image: see text] |
format | Online Article Text |
id | pubmed-4494845 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2009 |
publisher | Springer Vienna |
record_format | MEDLINE/PubMed |
spelling | pubmed-44948452015-07-09 The intrinsic origin of the grain-boundary resistance in Sr-doped LaGaO(3) Kim, Sangtae Monatsh Chem Original Paper ABSTRACT: In this paper I summarize our recent investigations (Park and Kim, Phys Chem C 111:14903, 2007; Solid State Ionics 179:1329, 2008) on the origin of the grain-boundary resistance in a doped LaGaO(3), a perovskite-structured solid electrolyte. The partial electronic and ionic resistances of the bulk and the grain boundaries, as well as the total resistance, in 1 mol% Sr-doped LaGaO(3) were measured separately by means of a dc-polarization method and ac-impedance spectroscopy. Both of the partial resistances at the grain boundaries were greater than the bulk counterparts, indicating that the grain boundaries impede the ionic as well as the electronic transport in this material. The transference number of the partial electronic conductivity at the grain boundary was however greater than that in the bulk. This fact strongly suggests that both electronic and ionic charge carriers deplete at the grain boundaries to form the space-charge zones and that the grain-boundary cores in this material are positively charged. In light of the fact that the effective charge of the oxygen vacancy (+2) is greater than that of the electron hole (+1), the oxygen vacancies deplete more sharply in the space-charge zones compared to the electron holes such that the grain boundaries become more mixed conducting relative to the bulk. These observations verify that the electrical conduction across the grain-boundaries in 1 mol% Sr-doped LaGaO(3) is governed by the space charge. GRAPHICAL ABSTRACT: [Image: see text] Springer Vienna 2009-03-27 2009 /pmc/articles/PMC4494845/ /pubmed/26166849 http://dx.doi.org/10.1007/s00706-009-0136-4 Text en © The Author(s) 2009 https://creativecommons.org/licenses/by-nc/4.0/ This article is distributed under the terms of the Creative Commons Attribution Noncommercial License which permits any noncommercial use, distribution, and reproduction in any medium, provided the original author(s) and source are credited. |
spellingShingle | Original Paper Kim, Sangtae The intrinsic origin of the grain-boundary resistance in Sr-doped LaGaO(3) |
title | The intrinsic origin of the grain-boundary resistance in Sr-doped LaGaO(3) |
title_full | The intrinsic origin of the grain-boundary resistance in Sr-doped LaGaO(3) |
title_fullStr | The intrinsic origin of the grain-boundary resistance in Sr-doped LaGaO(3) |
title_full_unstemmed | The intrinsic origin of the grain-boundary resistance in Sr-doped LaGaO(3) |
title_short | The intrinsic origin of the grain-boundary resistance in Sr-doped LaGaO(3) |
title_sort | intrinsic origin of the grain-boundary resistance in sr-doped lagao(3) |
topic | Original Paper |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4494845/ https://www.ncbi.nlm.nih.gov/pubmed/26166849 http://dx.doi.org/10.1007/s00706-009-0136-4 |
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