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Pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites Hg(3)Te(2)X(2) (X = Cl, Br)

Ferroelectricity is typically suppressed under hydrostatic compression because the short-range repulsions, which favor the nonpolar phase, increase more rapidly than the long-range interactions, which prefer the ferroelectric phase. Here, based on single-crystal X-ray diffraction and density-functio...

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Autores principales: Cai, Weizhao, He, Jiangang, Li, Hao, Zhang, Rong, Zhang, Dongzhou, Chung, Duck Young, Bhowmick, Tushar, Wolverton, Christopher, Kanatzidis, Mercouri G., Deemyad, Shanti
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7940478/
https://www.ncbi.nlm.nih.gov/pubmed/33686062
http://dx.doi.org/10.1038/s41467-021-21836-7
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author Cai, Weizhao
He, Jiangang
Li, Hao
Zhang, Rong
Zhang, Dongzhou
Chung, Duck Young
Bhowmick, Tushar
Wolverton, Christopher
Kanatzidis, Mercouri G.
Deemyad, Shanti
author_facet Cai, Weizhao
He, Jiangang
Li, Hao
Zhang, Rong
Zhang, Dongzhou
Chung, Duck Young
Bhowmick, Tushar
Wolverton, Christopher
Kanatzidis, Mercouri G.
Deemyad, Shanti
author_sort Cai, Weizhao
collection PubMed
description Ferroelectricity is typically suppressed under hydrostatic compression because the short-range repulsions, which favor the nonpolar phase, increase more rapidly than the long-range interactions, which prefer the ferroelectric phase. Here, based on single-crystal X-ray diffraction and density-functional theory, we provide evidence of a ferroelectric-like transition from phase I2(1)3 to R3 induced by pressure in two isostructural defect antiperovskites Hg(3)Te(2)Cl(2) (15.5 GPa) and Hg(3)Te(2)Br(2) (17.5 GPa). First-principles calculations show that this transition is attributed to pressure-induced softening of the infrared phonon mode Γ(4), similar to the archetypal ferroelectric material BaTiO(3) at ambient pressure. Additionally, we observe a gradual band-gap closing from ~2.5 eV to metallic-like state of Hg(3)Te(2)Br(2) with an unexpectedly stable R3 phase even after semiconductor-to-metal transition. This study demonstrates the possibility of emergence of polar metal under pressure in this class of materials and establishes the possibility of pressure-induced ferroelectric-like transition in perovskite-related systems.
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spelling pubmed-79404782021-03-28 Pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites Hg(3)Te(2)X(2) (X = Cl, Br) Cai, Weizhao He, Jiangang Li, Hao Zhang, Rong Zhang, Dongzhou Chung, Duck Young Bhowmick, Tushar Wolverton, Christopher Kanatzidis, Mercouri G. Deemyad, Shanti Nat Commun Article Ferroelectricity is typically suppressed under hydrostatic compression because the short-range repulsions, which favor the nonpolar phase, increase more rapidly than the long-range interactions, which prefer the ferroelectric phase. Here, based on single-crystal X-ray diffraction and density-functional theory, we provide evidence of a ferroelectric-like transition from phase I2(1)3 to R3 induced by pressure in two isostructural defect antiperovskites Hg(3)Te(2)Cl(2) (15.5 GPa) and Hg(3)Te(2)Br(2) (17.5 GPa). First-principles calculations show that this transition is attributed to pressure-induced softening of the infrared phonon mode Γ(4), similar to the archetypal ferroelectric material BaTiO(3) at ambient pressure. Additionally, we observe a gradual band-gap closing from ~2.5 eV to metallic-like state of Hg(3)Te(2)Br(2) with an unexpectedly stable R3 phase even after semiconductor-to-metal transition. This study demonstrates the possibility of emergence of polar metal under pressure in this class of materials and establishes the possibility of pressure-induced ferroelectric-like transition in perovskite-related systems. Nature Publishing Group UK 2021-03-08 /pmc/articles/PMC7940478/ /pubmed/33686062 http://dx.doi.org/10.1038/s41467-021-21836-7 Text en © The Author(s) 2021 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
Cai, Weizhao
He, Jiangang
Li, Hao
Zhang, Rong
Zhang, Dongzhou
Chung, Duck Young
Bhowmick, Tushar
Wolverton, Christopher
Kanatzidis, Mercouri G.
Deemyad, Shanti
Pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites Hg(3)Te(2)X(2) (X = Cl, Br)
title Pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites Hg(3)Te(2)X(2) (X = Cl, Br)
title_full Pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites Hg(3)Te(2)X(2) (X = Cl, Br)
title_fullStr Pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites Hg(3)Te(2)X(2) (X = Cl, Br)
title_full_unstemmed Pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites Hg(3)Te(2)X(2) (X = Cl, Br)
title_short Pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites Hg(3)Te(2)X(2) (X = Cl, Br)
title_sort pressure-induced ferroelectric-like transition creates a polar metal in defect antiperovskites hg(3)te(2)x(2) (x = cl, br)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7940478/
https://www.ncbi.nlm.nih.gov/pubmed/33686062
http://dx.doi.org/10.1038/s41467-021-21836-7
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