Cargando…
Electric-field-induced non-ergodic relaxor to ferroelectric transition in BiFeO(3)–xSrTiO(3) ceramics
While BiFeO(3)-based solid solutions show great promise for applications in energy conversion and storage, realizing this promise necessitates understanding the structure–property relationship in particular pertaining to the relaxor-like characteristics often exhibited by solid solutions with polar-...
Autores principales: | , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2023
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10273322/ https://www.ncbi.nlm.nih.gov/pubmed/37332483 http://dx.doi.org/10.1039/d2tc05100a |
_version_ | 1785059662226259968 |
---|---|
author | Oliveira, Leonardo Ormstrup, Jeppe Majkut, Marta Makarovic, Maja Rojac, Tadej Walker, Julian Simons, Hugh |
author_facet | Oliveira, Leonardo Ormstrup, Jeppe Majkut, Marta Makarovic, Maja Rojac, Tadej Walker, Julian Simons, Hugh |
author_sort | Oliveira, Leonardo |
collection | PubMed |
description | While BiFeO(3)-based solid solutions show great promise for applications in energy conversion and storage, realizing this promise necessitates understanding the structure–property relationship in particular pertaining to the relaxor-like characteristics often exhibited by solid solutions with polar-to-non-polar morphotropic phase boundaries. To this end, we investigated the role of the compositionally-driven relaxor state in (100 − x)BiFeO(3)–xSrTiO(3) [BFO–xSTO], via in situ synchrotron X-ray diffraction under bipolar electric-field cycling. The electric-field induced changes to the crystal structure, phase fraction and domain textures were monitored via the {111}(pc), {200}(pc), and 1/2{311}(pc) Bragg peaks. The dynamics of the intensities and positions of the (111) and (111̄) reflections reveal an initial non-ergodic regime followed by long-range ferroelectric ordering after extended poling cycles. The increased degree of random multi-site occupation in BFO–42STO compared to BFO–35STO is correlated with an increase of the critical electric field needed to induce the non-ergodic-to-ferroelectric transition, and a decrease in the degree of domain reorientation. Although both compositions show an irreversible transition to a long-range ferroelectric state, our results suggest that the weaker ferroelectric response in BFO–42STO is related to an increase in ergodicity. This, in turn, serves to guide the development of BFO-based systems into promising platform for further property engineering towards specific capacitor applications. |
format | Online Article Text |
id | pubmed-10273322 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | The Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-102733222023-06-17 Electric-field-induced non-ergodic relaxor to ferroelectric transition in BiFeO(3)–xSrTiO(3) ceramics Oliveira, Leonardo Ormstrup, Jeppe Majkut, Marta Makarovic, Maja Rojac, Tadej Walker, Julian Simons, Hugh J Mater Chem C Mater Chemistry While BiFeO(3)-based solid solutions show great promise for applications in energy conversion and storage, realizing this promise necessitates understanding the structure–property relationship in particular pertaining to the relaxor-like characteristics often exhibited by solid solutions with polar-to-non-polar morphotropic phase boundaries. To this end, we investigated the role of the compositionally-driven relaxor state in (100 − x)BiFeO(3)–xSrTiO(3) [BFO–xSTO], via in situ synchrotron X-ray diffraction under bipolar electric-field cycling. The electric-field induced changes to the crystal structure, phase fraction and domain textures were monitored via the {111}(pc), {200}(pc), and 1/2{311}(pc) Bragg peaks. The dynamics of the intensities and positions of the (111) and (111̄) reflections reveal an initial non-ergodic regime followed by long-range ferroelectric ordering after extended poling cycles. The increased degree of random multi-site occupation in BFO–42STO compared to BFO–35STO is correlated with an increase of the critical electric field needed to induce the non-ergodic-to-ferroelectric transition, and a decrease in the degree of domain reorientation. Although both compositions show an irreversible transition to a long-range ferroelectric state, our results suggest that the weaker ferroelectric response in BFO–42STO is related to an increase in ergodicity. This, in turn, serves to guide the development of BFO-based systems into promising platform for further property engineering towards specific capacitor applications. The Royal Society of Chemistry 2023-04-14 /pmc/articles/PMC10273322/ /pubmed/37332483 http://dx.doi.org/10.1039/d2tc05100a Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by/3.0/ |
spellingShingle | Chemistry Oliveira, Leonardo Ormstrup, Jeppe Majkut, Marta Makarovic, Maja Rojac, Tadej Walker, Julian Simons, Hugh Electric-field-induced non-ergodic relaxor to ferroelectric transition in BiFeO(3)–xSrTiO(3) ceramics |
title | Electric-field-induced non-ergodic relaxor to ferroelectric transition in BiFeO(3)–xSrTiO(3) ceramics |
title_full | Electric-field-induced non-ergodic relaxor to ferroelectric transition in BiFeO(3)–xSrTiO(3) ceramics |
title_fullStr | Electric-field-induced non-ergodic relaxor to ferroelectric transition in BiFeO(3)–xSrTiO(3) ceramics |
title_full_unstemmed | Electric-field-induced non-ergodic relaxor to ferroelectric transition in BiFeO(3)–xSrTiO(3) ceramics |
title_short | Electric-field-induced non-ergodic relaxor to ferroelectric transition in BiFeO(3)–xSrTiO(3) ceramics |
title_sort | electric-field-induced non-ergodic relaxor to ferroelectric transition in bifeo(3)–xsrtio(3) ceramics |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10273322/ https://www.ncbi.nlm.nih.gov/pubmed/37332483 http://dx.doi.org/10.1039/d2tc05100a |
work_keys_str_mv | AT oliveiraleonardo electricfieldinducednonergodicrelaxortoferroelectrictransitioninbifeo3xsrtio3ceramics AT ormstrupjeppe electricfieldinducednonergodicrelaxortoferroelectrictransitioninbifeo3xsrtio3ceramics AT majkutmarta electricfieldinducednonergodicrelaxortoferroelectrictransitioninbifeo3xsrtio3ceramics AT makarovicmaja electricfieldinducednonergodicrelaxortoferroelectrictransitioninbifeo3xsrtio3ceramics AT rojactadej electricfieldinducednonergodicrelaxortoferroelectrictransitioninbifeo3xsrtio3ceramics AT walkerjulian electricfieldinducednonergodicrelaxortoferroelectrictransitioninbifeo3xsrtio3ceramics AT simonshugh electricfieldinducednonergodicrelaxortoferroelectrictransitioninbifeo3xsrtio3ceramics |