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Strong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferrite

Isolated nonmagnetic substitutional defect ions experience huge coupled electric magnetic interaction in the single-phase multiferroic BiFeO$_{3}$. In the ferroelectric state above the magnetic Néel temperature $T$$_{N}$, the electric environment generates a single symmetric electric field gradient...

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Autores principales: Schell, Juliana, Schmuck, Merlin, Efe, İpek, Dang, Thien Thanh, Gonçalves, João Nuno, Lewin, Daniil, Castillo, Marianela Escobar, Shvartsman, Vladimir V, Costa, Ângelo Rafael Granadeiro, Köster, Ulli, Vianden, Reiner, Noll, Cornelia, Lupascu, Doru C
Lenguaje:eng
Publicado: 2022
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevB.105.094102
http://cds.cern.ch/record/2803754
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author Schell, Juliana
Schmuck, Merlin
Efe, İpek
Dang, Thien Thanh
Gonçalves, João Nuno
Lewin, Daniil
Castillo, Marianela Escobar
Shvartsman, Vladimir V
Costa, Ângelo Rafael Granadeiro
Köster, Ulli
Vianden, Reiner
Noll, Cornelia
Lupascu, Doru C
author_facet Schell, Juliana
Schmuck, Merlin
Efe, İpek
Dang, Thien Thanh
Gonçalves, João Nuno
Lewin, Daniil
Castillo, Marianela Escobar
Shvartsman, Vladimir V
Costa, Ângelo Rafael Granadeiro
Köster, Ulli
Vianden, Reiner
Noll, Cornelia
Lupascu, Doru C
author_sort Schell, Juliana
collection CERN
description Isolated nonmagnetic substitutional defect ions experience huge coupled electric magnetic interaction in the single-phase multiferroic BiFeO$_{3}$. In the ferroelectric state above the magnetic Néel temperature $T$$_{N}$, the electric environment generates a single symmetric electric field gradient (EFG) parallel to the electric polarization direction. Below $T$$_{N}$, a distinct magnetic interaction arises, monitored by the probe nuclei via their magnetic moment. Two magnetic environments arise, given by the relative angle of the local magnetic moment within its easy magnetic plane with respect to the EFG orientation. The angle between field gradient orientation and magnetic field direction is the most stable fitting parameter. The magnetic interaction concomitantly increases the EFG dramatically which reflects an outstandingly large local magnetoelectric coupling. In the set of best fits, two different electric environments form concurrently with two distinctly different local magnetic fields. The magnetic ordering in BiFeO$_{3}$ thus completely distorts the electric environment of the nonmagnetic probe nucleus. The implications for the local effect of dopants in BiFeO$_{3}$ are discussed. A third probe environment arising independent of temperature is identified and associated with an iron vacancy.
id cern-2803754
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2022
record_format invenio
spelling cern-28037542023-03-22T15:46:15Zdoi:10.1103/PhysRevB.105.094102http://cds.cern.ch/record/2803754engSchell, JulianaSchmuck, MerlinEfe, İpekDang, Thien ThanhGonçalves, João NunoLewin, DaniilCastillo, Marianela EscobarShvartsman, Vladimir VCosta, Ângelo Rafael GranadeiroKöster, UlliVianden, ReinerNoll, CorneliaLupascu, Doru CStrong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferriteCondensed MatterIsolated nonmagnetic substitutional defect ions experience huge coupled electric magnetic interaction in the single-phase multiferroic BiFeO$_{3}$. In the ferroelectric state above the magnetic Néel temperature $T$$_{N}$, the electric environment generates a single symmetric electric field gradient (EFG) parallel to the electric polarization direction. Below $T$$_{N}$, a distinct magnetic interaction arises, monitored by the probe nuclei via their magnetic moment. Two magnetic environments arise, given by the relative angle of the local magnetic moment within its easy magnetic plane with respect to the EFG orientation. The angle between field gradient orientation and magnetic field direction is the most stable fitting parameter. The magnetic interaction concomitantly increases the EFG dramatically which reflects an outstandingly large local magnetoelectric coupling. In the set of best fits, two different electric environments form concurrently with two distinctly different local magnetic fields. The magnetic ordering in BiFeO$_{3}$ thus completely distorts the electric environment of the nonmagnetic probe nucleus. The implications for the local effect of dopants in BiFeO$_{3}$ are discussed. A third probe environment arising independent of temperature is identified and associated with an iron vacancy.oai:cds.cern.ch:28037542022
spellingShingle Condensed Matter
Schell, Juliana
Schmuck, Merlin
Efe, İpek
Dang, Thien Thanh
Gonçalves, João Nuno
Lewin, Daniil
Castillo, Marianela Escobar
Shvartsman, Vladimir V
Costa, Ângelo Rafael Granadeiro
Köster, Ulli
Vianden, Reiner
Noll, Cornelia
Lupascu, Doru C
Strong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferrite
title Strong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferrite
title_full Strong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferrite
title_fullStr Strong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferrite
title_full_unstemmed Strong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferrite
title_short Strong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferrite
title_sort strong magnetoelectric coupling at an atomic nonmagnetic electromagnetic probe in bismuth ferrite
topic Condensed Matter
url https://dx.doi.org/10.1103/PhysRevB.105.094102
http://cds.cern.ch/record/2803754
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