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Effects of poling and crystallinity on the dielectric properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) at cryogenic temperatures

The mechanisms underlying the anomalously large, room temperature piezoelectric activity of relaxor-PbTiO(3) type single crystals have previously been linked to low temperature relaxations in the piezoelectric and dielectric properties. We investigate the properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1...

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Autores principales: Shepley, Philippa M., Stoica, Laura A., Li, Yang, Burnell, Gavin, Bell, Andrew J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6385292/
https://www.ncbi.nlm.nih.gov/pubmed/30792435
http://dx.doi.org/10.1038/s41598-019-38995-9
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author Shepley, Philippa M.
Stoica, Laura A.
Li, Yang
Burnell, Gavin
Bell, Andrew J.
author_facet Shepley, Philippa M.
Stoica, Laura A.
Li, Yang
Burnell, Gavin
Bell, Andrew J.
author_sort Shepley, Philippa M.
collection PubMed
description The mechanisms underlying the anomalously large, room temperature piezoelectric activity of relaxor-PbTiO(3) type single crystals have previously been linked to low temperature relaxations in the piezoelectric and dielectric properties. We investigate the properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) between 10 and 300 K using dielectric permittivity measurements. We compare results on single crystal plates measured in the [001] and [111] directions with a polycrystalline ceramic of the same composition. Poled crystals have very different behaviour to unpoled crystals, whereas the dielectric spectrum of the polycrystalline ceramic changes very little on poling. A large, frequency dependent dielectric relaxation is seen in the poled [001] crystal around 100 K. The relaxation is much less prominent in the [111] cut crystal, and is not present in the polycrystalline ceramic. The unique presence of the large relaxation in poled, [001] oriented crystals indicates that the phenomenon is not due their relaxor nature alone. We propose that heterophase dynamics such as the motion of phase domain boundaries are responsible for both the anomalous electromechanical and dielectric behaviour.
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spelling pubmed-63852922019-02-26 Effects of poling and crystallinity on the dielectric properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) at cryogenic temperatures Shepley, Philippa M. Stoica, Laura A. Li, Yang Burnell, Gavin Bell, Andrew J. Sci Rep Article The mechanisms underlying the anomalously large, room temperature piezoelectric activity of relaxor-PbTiO(3) type single crystals have previously been linked to low temperature relaxations in the piezoelectric and dielectric properties. We investigate the properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) between 10 and 300 K using dielectric permittivity measurements. We compare results on single crystal plates measured in the [001] and [111] directions with a polycrystalline ceramic of the same composition. Poled crystals have very different behaviour to unpoled crystals, whereas the dielectric spectrum of the polycrystalline ceramic changes very little on poling. A large, frequency dependent dielectric relaxation is seen in the poled [001] crystal around 100 K. The relaxation is much less prominent in the [111] cut crystal, and is not present in the polycrystalline ceramic. The unique presence of the large relaxation in poled, [001] oriented crystals indicates that the phenomenon is not due their relaxor nature alone. We propose that heterophase dynamics such as the motion of phase domain boundaries are responsible for both the anomalous electromechanical and dielectric behaviour. Nature Publishing Group UK 2019-02-21 /pmc/articles/PMC6385292/ /pubmed/30792435 http://dx.doi.org/10.1038/s41598-019-38995-9 Text en © The Author(s) 2019 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Shepley, Philippa M.
Stoica, Laura A.
Li, Yang
Burnell, Gavin
Bell, Andrew J.
Effects of poling and crystallinity on the dielectric properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) at cryogenic temperatures
title Effects of poling and crystallinity on the dielectric properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) at cryogenic temperatures
title_full Effects of poling and crystallinity on the dielectric properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) at cryogenic temperatures
title_fullStr Effects of poling and crystallinity on the dielectric properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) at cryogenic temperatures
title_full_unstemmed Effects of poling and crystallinity on the dielectric properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) at cryogenic temperatures
title_short Effects of poling and crystallinity on the dielectric properties of Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) at cryogenic temperatures
title_sort effects of poling and crystallinity on the dielectric properties of pb(in(1/2)nb(1/2))o(3)-pb(mg(1/3)nb(2/3))o(3)-pbtio(3) at cryogenic temperatures
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6385292/
https://www.ncbi.nlm.nih.gov/pubmed/30792435
http://dx.doi.org/10.1038/s41598-019-38995-9
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