Magnetic-anisotropy modulation in multiferroic heterostructures by ferroelectric domains from first principles
First-principles calculations incorporating spin-orbit coupling are presented for a multiferroic material as a ferromagnetic/ferroelectric junction. We simulate the interface effect that cannot be described by the single-phase bulk. The in-plane uniaxial magnetic-anisotropy of Co FeSi is observed wh...
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Published in | Science and technology of advanced materials Vol. 25; no. 1; p. 2391268 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
United States
Taylor & Francis Ltd
2024
Taylor & Francis Taylor & Francis Group |
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Online Access | Get full text |
ISSN | 1468-6996 1878-5514 |
DOI | 10.1080/14686996.2024.2391268 |
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Abstract | First-principles calculations incorporating spin-orbit coupling are presented for a multiferroic material as a ferromagnetic/ferroelectric junction. We simulate the interface effect that cannot be described by the single-phase bulk. The in-plane uniaxial magnetic-anisotropy of Co
FeSi is observed when the ferroelectric domain is polarized parallel to the interface, whereas the magnetic anisotropy is significantly different in the plane for the electrical polarization perpendicular to the interface. While the single-phase effect dominates the main part of the modulation of the magnetic anisotropy, symmetry breaking due to the interfacial effect is observed in the ferromagnetic ultrathin films. The origin of the modulated magnetic-anisotropy can be attributed to the shifting of specific energy bands in Co
FeSi when the ferroelectric domain is modified. |
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AbstractList | IMPACT STATEMENT The origin of strain-induced magnetocrystalline anisotropy in multiferroic Co2FeSi/BaTiO3(001) heterostructures is clarified by first-principles electron theory. The magnetic anisotropy is modified by interface effects for ultrathin Co2FeSi films. First-principles calculations incorporating spin-orbit coupling are presented for a multiferroic material as a ferromagnetic/ferroelectric junction. We simulate the interface effect that cannot be described by the single-phase bulk. The in-plane uniaxial magnetic-anisotropy of Co2FeSi is observed when the ferroelectric domain is polarized parallel to the interface, whereas the magnetic anisotropy is significantly different in the plane for the electrical polarization perpendicular to the interface. While the single-phase effect dominates the main part of the modulation of the magnetic anisotropy, symmetry breaking due to the interfacial effect is observed in the ferromagnetic ultrathin films. The origin of the modulated magnetic-anisotropy can be attributed to the shifting of specific energy bands in Co2FeSi when the ferroelectric domain is modified.First-principles calculations incorporating spin-orbit coupling are presented for a multiferroic material as a ferromagnetic/ferroelectric junction. We simulate the interface effect that cannot be described by the single-phase bulk. The in-plane uniaxial magnetic-anisotropy of Co2FeSi is observed when the ferroelectric domain is polarized parallel to the interface, whereas the magnetic anisotropy is significantly different in the plane for the electrical polarization perpendicular to the interface. While the single-phase effect dominates the main part of the modulation of the magnetic anisotropy, symmetry breaking due to the interfacial effect is observed in the ferromagnetic ultrathin films. The origin of the modulated magnetic-anisotropy can be attributed to the shifting of specific energy bands in Co2FeSi when the ferroelectric domain is modified. First-principles calculations incorporating spin-orbit coupling are presented for a multiferroic material as a ferromagnetic/ferroelectric junction. We simulate the interface effect that cannot be described by the single-phase bulk. The in-plane uniaxial magnetic-anisotropy of Co 2 FeSi is observed when the ferroelectric domain is polarized parallel to the interface, whereas the magnetic anisotropy is significantly different in the plane for the electrical polarization perpendicular to the interface. While the single-phase effect dominates the main part of the modulation of the magnetic anisotropy, symmetry breaking due to the interfacial effect is observed in the ferromagnetic ultrathin films. The origin of the modulated magnetic-anisotropy can be attributed to the shifting of specific energy bands in Co 2 FeSi when the ferroelectric domain is modified. The origin of strain-induced magnetocrystalline anisotropy in multiferroic Co 2 FeSi/BaTiO 3 (001) heterostructures is clarified by first-principles electron theory. The magnetic anisotropy is modified by interface effects for ultrathin Co 2 FeSi films. First-principles calculations incorporating spin-orbit coupling are presented for a multiferroic material as a ferromagnetic/ferroelectric junction. We simulate the interface effect that cannot be described by the single-phase bulk. The in-plane uniaxial magnetic-anisotropy of Co2FeSi is observed when the ferroelectric domain is polarized parallel to the interface, whereas the magnetic anisotropy is significantly different in the plane for the electrical polarization perpendicular to the interface. While the single-phase effect dominates the main part of the modulation of the magnetic anisotropy, symmetry breaking due to the interfacial effect is observed in the ferromagnetic ultrathin films. The origin of the modulated magnetic-anisotropy can be attributed to the shifting of specific energy bands in Co2FeSi when the ferroelectric domain is modified. First-principles calculations incorporating spin-orbit coupling are presented for a multiferroic material as a ferromagnetic/ferroelectric junction. We simulate the interface effect that cannot be described by the single-phase bulk. The in-plane uniaxial magnetic-anisotropy of Co FeSi is observed when the ferroelectric domain is polarized parallel to the interface, whereas the magnetic anisotropy is significantly different in the plane for the electrical polarization perpendicular to the interface. While the single-phase effect dominates the main part of the modulation of the magnetic anisotropy, symmetry breaking due to the interfacial effect is observed in the ferromagnetic ultrathin films. The origin of the modulated magnetic-anisotropy can be attributed to the shifting of specific energy bands in Co FeSi when the ferroelectric domain is modified. |
Author | Yatmeidhy, Amran Mahfudh Gohda, Yoshihiro |
Author_xml | – sequence: 1 givenname: Amran Mahfudh orcidid: 0000-0003-0057-7590 surname: Yatmeidhy fullname: Yatmeidhy, Amran Mahfudh – sequence: 2 givenname: Yoshihiro orcidid: 0000-0002-6047-027X surname: Gohda fullname: Gohda, Yoshihiro |
BackLink | https://www.ncbi.nlm.nih.gov/pubmed/39188550$$D View this record in MEDLINE/PubMed |
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Keywords | First-principles calculations magnetic anisotropy spin-orbit coupling multiferroic heterostructure ferroelectric domains |
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Snippet | First-principles calculations incorporating spin-orbit coupling are presented for a multiferroic material as a ferromagnetic/ferroelectric junction. We... IMPACT STATEMENT The origin of strain-induced magnetocrystalline anisotropy in multiferroic Co2FeSi/BaTiO3(001) heterostructures is clarified by... |
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StartPage | 2391268 |
SubjectTerms | Anisotropy Broken symmetry Electric fields Energy Energy bands Ferroelectric domains Ferroelectric materials Ferroelectricity Ferromagnetic materials First principles First-principles calculations Focus on New Methodology for Developing Innovative Materials Heterostructures Interfaces Magnetic anisotropy Materials science Modulation multiferroic heterostructure Multiferroic materials Orbit calculation Specific energy spin-orbit coupling Spin-orbit interactions Thin films |
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Title | Magnetic-anisotropy modulation in multiferroic heterostructures by ferroelectric domains from first principles |
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