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Group Theory Analysis to Study Phase Transitions of Quasi-2D Sr(3)Hf(2)O(7)

We present an ab-initio study performed in the framework of density functional theory, group-subgroup symmetry analysis and lattice dynamics, to probe the octahedral distortions, which occur during the structural phase transitions of the quasi-2D layered perovskite Sr(3)Hf(2)O(7) compound. Such a sy...

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Autores principales: da Silva, Estelina Lora, Gerami, Adeleh Mokhles, Lekshmi, P. Neenu, Marcondes, Michel L., Assali, Lucy V. C., Petrilli, Helena M., Correia, Joao Guilherme, Lopes, Armandina M. L., Araújo, João P.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8066622/
https://www.ncbi.nlm.nih.gov/pubmed/33807471
http://dx.doi.org/10.3390/nano11040897
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author da Silva, Estelina Lora
Gerami, Adeleh Mokhles
Lekshmi, P. Neenu
Marcondes, Michel L.
Assali, Lucy V. C.
Petrilli, Helena M.
Correia, Joao Guilherme
Lopes, Armandina M. L.
Araújo, João P.
author_facet da Silva, Estelina Lora
Gerami, Adeleh Mokhles
Lekshmi, P. Neenu
Marcondes, Michel L.
Assali, Lucy V. C.
Petrilli, Helena M.
Correia, Joao Guilherme
Lopes, Armandina M. L.
Araújo, João P.
author_sort da Silva, Estelina Lora
collection PubMed
description We present an ab-initio study performed in the framework of density functional theory, group-subgroup symmetry analysis and lattice dynamics, to probe the octahedral distortions, which occur during the structural phase transitions of the quasi-2D layered perovskite Sr(3)Hf(2)O(7) compound. Such a system is characterized by a high-temperature I4/mmm centrosymmetric structure and a ground-state Cmc2(1) ferroelectric phase. We have probed potential candidate polymorphs that may form the I4/mmm → Cmc2(1) transition pathways, namely Fmm2, Ccce, Cmca and Cmcm. We found that the band gap widths increase as the symmetry decreases, with the ground-state structure presenting the largest gap width (∼5.95 eV). By probing the Partial Density of States, we observe a direct relation regarding the tilts and rotations of the oxygen perovskite cages as the transition occurs; these show large variations mostly of the O p-states which contribute mostly to the valence band maximum. Moreover, by analyzing the hyperfine parameters, namely the Electric Field Gradients and asymmetric parameters, we observe variations as the transition occurs, from which it is possible to identify the most plausible intermediate phases. We have also computed the macroscopic polarization and confirm that the Cmc2(1) phase is ferroelectric with a value of spontaneous polarization of 0.0478 C/m(2). The ferroelectricity of the ground-state Cmc2(1) system arises due to a second order parameter related to the coupling of the rotation and tilts of the O perovskite cages together with the Sr displacements.
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spelling pubmed-80666222021-04-25 Group Theory Analysis to Study Phase Transitions of Quasi-2D Sr(3)Hf(2)O(7) da Silva, Estelina Lora Gerami, Adeleh Mokhles Lekshmi, P. Neenu Marcondes, Michel L. Assali, Lucy V. C. Petrilli, Helena M. Correia, Joao Guilherme Lopes, Armandina M. L. Araújo, João P. Nanomaterials (Basel) Article We present an ab-initio study performed in the framework of density functional theory, group-subgroup symmetry analysis and lattice dynamics, to probe the octahedral distortions, which occur during the structural phase transitions of the quasi-2D layered perovskite Sr(3)Hf(2)O(7) compound. Such a system is characterized by a high-temperature I4/mmm centrosymmetric structure and a ground-state Cmc2(1) ferroelectric phase. We have probed potential candidate polymorphs that may form the I4/mmm → Cmc2(1) transition pathways, namely Fmm2, Ccce, Cmca and Cmcm. We found that the band gap widths increase as the symmetry decreases, with the ground-state structure presenting the largest gap width (∼5.95 eV). By probing the Partial Density of States, we observe a direct relation regarding the tilts and rotations of the oxygen perovskite cages as the transition occurs; these show large variations mostly of the O p-states which contribute mostly to the valence band maximum. Moreover, by analyzing the hyperfine parameters, namely the Electric Field Gradients and asymmetric parameters, we observe variations as the transition occurs, from which it is possible to identify the most plausible intermediate phases. We have also computed the macroscopic polarization and confirm that the Cmc2(1) phase is ferroelectric with a value of spontaneous polarization of 0.0478 C/m(2). The ferroelectricity of the ground-state Cmc2(1) system arises due to a second order parameter related to the coupling of the rotation and tilts of the O perovskite cages together with the Sr displacements. MDPI 2021-03-31 /pmc/articles/PMC8066622/ /pubmed/33807471 http://dx.doi.org/10.3390/nano11040897 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/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 (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
da Silva, Estelina Lora
Gerami, Adeleh Mokhles
Lekshmi, P. Neenu
Marcondes, Michel L.
Assali, Lucy V. C.
Petrilli, Helena M.
Correia, Joao Guilherme
Lopes, Armandina M. L.
Araújo, João P.
Group Theory Analysis to Study Phase Transitions of Quasi-2D Sr(3)Hf(2)O(7)
title Group Theory Analysis to Study Phase Transitions of Quasi-2D Sr(3)Hf(2)O(7)
title_full Group Theory Analysis to Study Phase Transitions of Quasi-2D Sr(3)Hf(2)O(7)
title_fullStr Group Theory Analysis to Study Phase Transitions of Quasi-2D Sr(3)Hf(2)O(7)
title_full_unstemmed Group Theory Analysis to Study Phase Transitions of Quasi-2D Sr(3)Hf(2)O(7)
title_short Group Theory Analysis to Study Phase Transitions of Quasi-2D Sr(3)Hf(2)O(7)
title_sort group theory analysis to study phase transitions of quasi-2d sr(3)hf(2)o(7)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8066622/
https://www.ncbi.nlm.nih.gov/pubmed/33807471
http://dx.doi.org/10.3390/nano11040897
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