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The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary

The interplay between the critical fluctuations and the sample geometry is investigated numerically using thin random-field ferromagnets exhibiting the field-driven magnetisation reversal on the hysteresis loop. The system is studied along the theoretical critical line in the plane of random-field d...

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Autores principales: Tadić, Bosiljka, Mijatović, Svetislav, Janićević, Sanja, Spasojević, Djordje, Rodgers, Geoff J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6474887/
https://www.ncbi.nlm.nih.gov/pubmed/31004121
http://dx.doi.org/10.1038/s41598-019-42802-w
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author Tadić, Bosiljka
Mijatović, Svetislav
Janićević, Sanja
Spasojević, Djordje
Rodgers, Geoff J.
author_facet Tadić, Bosiljka
Mijatović, Svetislav
Janićević, Sanja
Spasojević, Djordje
Rodgers, Geoff J.
author_sort Tadić, Bosiljka
collection PubMed
description The interplay between the critical fluctuations and the sample geometry is investigated numerically using thin random-field ferromagnets exhibiting the field-driven magnetisation reversal on the hysteresis loop. The system is studied along the theoretical critical line in the plane of random-field disorder and thickness. The thickness is varied to consider samples of various geometry between a two-dimensional plane and a complete three-dimensional lattice with an open boundary in the direction of the growing thickness. We perform a multi-fractal analysis of the Barkhausen noise signals and scaling of the critical avalanches of the domain wall motion. Our results reveal that, for sufficiently small thickness, the sample geometry profoundly affects the dynamics by modifying the spectral segments that represent small fluctuations and promoting the time-scale dependent multi-fractality. Meanwhile, the avalanche distributions display two distinct power-law regions, in contrast to those in the two-dimensional limit, and the average avalanche shapes are asymmetric. With increasing thickness, the scaling characteristics and the multi-fractal spectrum in thicker samples gradually approach the hysteresis loop criticality in three-dimensional systems. Thin ferromagnetic films are growing in importance technologically, and our results illustrate some new features of the domain wall dynamics induced by magnetisation reversal in these systems.
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spelling pubmed-64748872019-04-26 The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary Tadić, Bosiljka Mijatović, Svetislav Janićević, Sanja Spasojević, Djordje Rodgers, Geoff J. Sci Rep Article The interplay between the critical fluctuations and the sample geometry is investigated numerically using thin random-field ferromagnets exhibiting the field-driven magnetisation reversal on the hysteresis loop. The system is studied along the theoretical critical line in the plane of random-field disorder and thickness. The thickness is varied to consider samples of various geometry between a two-dimensional plane and a complete three-dimensional lattice with an open boundary in the direction of the growing thickness. We perform a multi-fractal analysis of the Barkhausen noise signals and scaling of the critical avalanches of the domain wall motion. Our results reveal that, for sufficiently small thickness, the sample geometry profoundly affects the dynamics by modifying the spectral segments that represent small fluctuations and promoting the time-scale dependent multi-fractality. Meanwhile, the avalanche distributions display two distinct power-law regions, in contrast to those in the two-dimensional limit, and the average avalanche shapes are asymmetric. With increasing thickness, the scaling characteristics and the multi-fractal spectrum in thicker samples gradually approach the hysteresis loop criticality in three-dimensional systems. Thin ferromagnetic films are growing in importance technologically, and our results illustrate some new features of the domain wall dynamics induced by magnetisation reversal in these systems. Nature Publishing Group UK 2019-04-19 /pmc/articles/PMC6474887/ /pubmed/31004121 http://dx.doi.org/10.1038/s41598-019-42802-w Text en © The Author(s) 2019 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 license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license 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 license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Tadić, Bosiljka
Mijatović, Svetislav
Janićević, Sanja
Spasojević, Djordje
Rodgers, Geoff J.
The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary
title The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary
title_full The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary
title_fullStr The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary
title_full_unstemmed The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary
title_short The critical Barkhausen avalanches in thin random-field ferromagnets with an open boundary
title_sort critical barkhausen avalanches in thin random-field ferromagnets with an open boundary
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6474887/
https://www.ncbi.nlm.nih.gov/pubmed/31004121
http://dx.doi.org/10.1038/s41598-019-42802-w
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