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Features of structure, magnetic state and electrodynamic performance of SrFe(12−x)In(x)O(19)
Indium-substituted strontium hexaferrites were prepared by the conventional solid-phase reaction method. Neutron diffraction patterns were obtained at room temperature and analyzed using the Rietveld methods. A linear dependence of the unit cell parameters is found. In(3+) cations are located mainly...
Autores principales: | , , , , , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8443609/ https://www.ncbi.nlm.nih.gov/pubmed/34526572 http://dx.doi.org/10.1038/s41598-021-97684-8 |
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author | Turchenko, V. A. Trukhanov, S. V. Kostishin, V. G. Damay, F. Porcher, F. Klygach, D. S. Vakhitov, M. G. Lyakhov, D. Michels, D. Bozzo, B. Fina, I. Almessiere, M. A. Slimani, Y. Baykal, A. Zhou, D. Trukhanov, A. V. |
author_facet | Turchenko, V. A. Trukhanov, S. V. Kostishin, V. G. Damay, F. Porcher, F. Klygach, D. S. Vakhitov, M. G. Lyakhov, D. Michels, D. Bozzo, B. Fina, I. Almessiere, M. A. Slimani, Y. Baykal, A. Zhou, D. Trukhanov, A. V. |
author_sort | Turchenko, V. A. |
collection | PubMed |
description | Indium-substituted strontium hexaferrites were prepared by the conventional solid-phase reaction method. Neutron diffraction patterns were obtained at room temperature and analyzed using the Rietveld methods. A linear dependence of the unit cell parameters is found. In(3+) cations are located mainly in octahedral positions of 4f(VI) and 12 k. The average crystallite size varies within 0.84–0.65 μm. With increasing substitution, the T(C) Curie temperature decreases monotonically down to ~ 520 K. ZFC and FC measurements showed a frustrated state. Upon substitution, the average and maximum sizes of ferrimagnetic clusters change in the opposite direction. The M(r) remanent magnetization decreases down to ~ 20.2 emu/g at room temperature. The M(s) spontaneous magnetization and the k(eff) effective magnetocrystalline anisotropy constant are determined. With increasing substitution, the maximum of the ε(/) real part of permittivity decreases in magnitude from ~ 3.3 to ~ 1.9 and shifts towards low frequencies from ~ 45.5 GHz to ~ 37.4 GHz. The maximum of the tg(α) dielectric loss tangent decreases from ~ 1.0 to ~ 0.7 and shifts towards low frequencies from ~ 40.6 GHz to ~ 37.3 GHz. The low-frequency maximum of the μ(/) real part of permeability decreases from ~ 1.8 to ~ 0.9 and slightly shifts towards high frequencies up to ~ 34.7 GHz. The maximum of the tg(δ) magnetic loss tangent decreases from ~ 0.7 to ~ 0.5 and shifts slightly towards low frequencies from ~ 40.5 GHz to ~ 37.7 GHz. The discussion of microwave properties is based on the saturation magnetization, natural ferromagnetic resonance and dielectric polarization types. |
format | Online Article Text |
id | pubmed-8443609 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-84436092021-09-20 Features of structure, magnetic state and electrodynamic performance of SrFe(12−x)In(x)O(19) Turchenko, V. A. Trukhanov, S. V. Kostishin, V. G. Damay, F. Porcher, F. Klygach, D. S. Vakhitov, M. G. Lyakhov, D. Michels, D. Bozzo, B. Fina, I. Almessiere, M. A. Slimani, Y. Baykal, A. Zhou, D. Trukhanov, A. V. Sci Rep Article Indium-substituted strontium hexaferrites were prepared by the conventional solid-phase reaction method. Neutron diffraction patterns were obtained at room temperature and analyzed using the Rietveld methods. A linear dependence of the unit cell parameters is found. In(3+) cations are located mainly in octahedral positions of 4f(VI) and 12 k. The average crystallite size varies within 0.84–0.65 μm. With increasing substitution, the T(C) Curie temperature decreases monotonically down to ~ 520 K. ZFC and FC measurements showed a frustrated state. Upon substitution, the average and maximum sizes of ferrimagnetic clusters change in the opposite direction. The M(r) remanent magnetization decreases down to ~ 20.2 emu/g at room temperature. The M(s) spontaneous magnetization and the k(eff) effective magnetocrystalline anisotropy constant are determined. With increasing substitution, the maximum of the ε(/) real part of permittivity decreases in magnitude from ~ 3.3 to ~ 1.9 and shifts towards low frequencies from ~ 45.5 GHz to ~ 37.4 GHz. The maximum of the tg(α) dielectric loss tangent decreases from ~ 1.0 to ~ 0.7 and shifts towards low frequencies from ~ 40.6 GHz to ~ 37.3 GHz. The low-frequency maximum of the μ(/) real part of permeability decreases from ~ 1.8 to ~ 0.9 and slightly shifts towards high frequencies up to ~ 34.7 GHz. The maximum of the tg(δ) magnetic loss tangent decreases from ~ 0.7 to ~ 0.5 and shifts slightly towards low frequencies from ~ 40.5 GHz to ~ 37.7 GHz. The discussion of microwave properties is based on the saturation magnetization, natural ferromagnetic resonance and dielectric polarization types. Nature Publishing Group UK 2021-09-15 /pmc/articles/PMC8443609/ /pubmed/34526572 http://dx.doi.org/10.1038/s41598-021-97684-8 Text en © The Author(s) 2021 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Article Turchenko, V. A. Trukhanov, S. V. Kostishin, V. G. Damay, F. Porcher, F. Klygach, D. S. Vakhitov, M. G. Lyakhov, D. Michels, D. Bozzo, B. Fina, I. Almessiere, M. A. Slimani, Y. Baykal, A. Zhou, D. Trukhanov, A. V. Features of structure, magnetic state and electrodynamic performance of SrFe(12−x)In(x)O(19) |
title | Features of structure, magnetic state and electrodynamic performance of SrFe(12−x)In(x)O(19) |
title_full | Features of structure, magnetic state and electrodynamic performance of SrFe(12−x)In(x)O(19) |
title_fullStr | Features of structure, magnetic state and electrodynamic performance of SrFe(12−x)In(x)O(19) |
title_full_unstemmed | Features of structure, magnetic state and electrodynamic performance of SrFe(12−x)In(x)O(19) |
title_short | Features of structure, magnetic state and electrodynamic performance of SrFe(12−x)In(x)O(19) |
title_sort | features of structure, magnetic state and electrodynamic performance of srfe(12−x)in(x)o(19) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8443609/ https://www.ncbi.nlm.nih.gov/pubmed/34526572 http://dx.doi.org/10.1038/s41598-021-97684-8 |
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