Complex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic Co3TeO6

Abstract Polarized and unpolarized neutron diffractions have been carried out to investigate the nature of the magnetic structures and transitions in monoclinic Co3TeO6. As the temperature is lowered below 26 K long range order develops, which is fully incommensurate (ICM) in all three crystallograp...

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Autores principales: Chi-Hung Lee, Chin-Wei Wang, Yang Zhao, Wen-Hsien Li, Jeffrey W. Lynn, A. Brooks Harris, Kirrily Rule, Hung-Duen Yang, Helmuth Berger
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Publicado: Nature Portfolio 2017
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Acceso en línea:https://doaj.org/article/9fa07b057b2f4cc980468d87109ca191
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spelling oai:doaj.org-article:9fa07b057b2f4cc980468d87109ca1912021-12-02T16:06:58ZComplex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic Co3TeO610.1038/s41598-017-06651-92045-2322https://doaj.org/article/9fa07b057b2f4cc980468d87109ca1912017-07-01T00:00:00Zhttps://doi.org/10.1038/s41598-017-06651-9https://doaj.org/toc/2045-2322Abstract Polarized and unpolarized neutron diffractions have been carried out to investigate the nature of the magnetic structures and transitions in monoclinic Co3TeO6. As the temperature is lowered below 26 K long range order develops, which is fully incommensurate (ICM) in all three crystallographic directions. Below 19.5 K additional commensurate magnetic peaks develop, consistent with the Γ4 irreducible representation, along with a splitting of the ICM peaks along the h direction which indicates that there are two separate sets of magnetic modulation vectors. Below 18 K, this small additional magnetic incommensurability disappears, ferroelectricity develops, an additional commensurate magnetic structure consistent with Γ3 irreducible representation appears, and the k component of the ICM wave vector disappears. Synchrotron x-ray diffraction measurements demonstrate that there is a significant shift of the electronic charge distribution from the Te ions at the crystallographic 8 f sites to the neighboring Co and O ions. These results, together with the unusually small electric polarization, its strong magnetic field dependence, and the negative thermal expansion in all three lattice parameters, suggest this material is an antiferroelectric. Below15 K the k component of the ICM structure reappears, along with second-order ICM Bragg peaks, which polarized neutron data demonstrate are magnetic in origin.Chi-Hung LeeChin-Wei WangYang ZhaoWen-Hsien LiJeffrey W. LynnA. Brooks HarrisKirrily RuleHung-Duen YangHelmuth BergerNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 7, Iss 1, Pp 1-16 (2017)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Chi-Hung Lee
Chin-Wei Wang
Yang Zhao
Wen-Hsien Li
Jeffrey W. Lynn
A. Brooks Harris
Kirrily Rule
Hung-Duen Yang
Helmuth Berger
Complex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic Co3TeO6
description Abstract Polarized and unpolarized neutron diffractions have been carried out to investigate the nature of the magnetic structures and transitions in monoclinic Co3TeO6. As the temperature is lowered below 26 K long range order develops, which is fully incommensurate (ICM) in all three crystallographic directions. Below 19.5 K additional commensurate magnetic peaks develop, consistent with the Γ4 irreducible representation, along with a splitting of the ICM peaks along the h direction which indicates that there are two separate sets of magnetic modulation vectors. Below 18 K, this small additional magnetic incommensurability disappears, ferroelectricity develops, an additional commensurate magnetic structure consistent with Γ3 irreducible representation appears, and the k component of the ICM wave vector disappears. Synchrotron x-ray diffraction measurements demonstrate that there is a significant shift of the electronic charge distribution from the Te ions at the crystallographic 8 f sites to the neighboring Co and O ions. These results, together with the unusually small electric polarization, its strong magnetic field dependence, and the negative thermal expansion in all three lattice parameters, suggest this material is an antiferroelectric. Below15 K the k component of the ICM structure reappears, along with second-order ICM Bragg peaks, which polarized neutron data demonstrate are magnetic in origin.
format article
author Chi-Hung Lee
Chin-Wei Wang
Yang Zhao
Wen-Hsien Li
Jeffrey W. Lynn
A. Brooks Harris
Kirrily Rule
Hung-Duen Yang
Helmuth Berger
author_facet Chi-Hung Lee
Chin-Wei Wang
Yang Zhao
Wen-Hsien Li
Jeffrey W. Lynn
A. Brooks Harris
Kirrily Rule
Hung-Duen Yang
Helmuth Berger
author_sort Chi-Hung Lee
title Complex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic Co3TeO6
title_short Complex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic Co3TeO6
title_full Complex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic Co3TeO6
title_fullStr Complex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic Co3TeO6
title_full_unstemmed Complex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic Co3TeO6
title_sort complex magnetic incommensurability and electronic charge transfer through the ferroelectric transition in multiferroic co3teo6
publisher Nature Portfolio
publishDate 2017
url https://doaj.org/article/9fa07b057b2f4cc980468d87109ca191
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