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Single Diameter Modulation Effects on Ni Nanowire Array Magnetization Reversal
Geometrically modulated magnetic nanowires are a simple yet efficient strategy to modify the magnetic domain wall propagation since a simple diameter modulation can achieve its pinning during the nanowire magnetization reversal. However, in dense systems of parallel nanowires, the stray fields arisi...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8706999/ https://www.ncbi.nlm.nih.gov/pubmed/34947752 http://dx.doi.org/10.3390/nano11123403 |
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author | Arzuza, Luis C. C. Vega, Victor Prida, Victor M. Moura, Karoline O. Pirota, Kleber R. Béron, Fanny |
author_facet | Arzuza, Luis C. C. Vega, Victor Prida, Victor M. Moura, Karoline O. Pirota, Kleber R. Béron, Fanny |
author_sort | Arzuza, Luis C. C. |
collection | PubMed |
description | Geometrically modulated magnetic nanowires are a simple yet efficient strategy to modify the magnetic domain wall propagation since a simple diameter modulation can achieve its pinning during the nanowire magnetization reversal. However, in dense systems of parallel nanowires, the stray fields arising at the diameter interface can interfere with the domain wall propagation in the neighboring nanowires. Therefore, the magnetic behavior of diameter-modulated nanowire arrays can be quite complex and depending on both short and long-range interaction fields, as well as the nanowire geometric dimensions. We applied the first-order reversal curve (FORC) method to bi-segmented Ni nanowire arrays varying the wide segment (45–65 nm diameter, 2.5–10.0 μm length). The FORC results indicate a magnetic behavior modification depending on its length/diameter aspect ratio. The distributions either exhibit a strong extension along the coercivity axis or a main distribution finishing by a fork feature, whereas the extension greatly reduces in amplitude. With the help of micromagnetic simulations, we propose that a low aspect ratio stabilizes pinned domain walls at the diameter modulation during the magnetization reversal. In this case, long-range axial interaction fields nucleate a domain wall at the nanowire extremities, while short-range ones could induce a nucleation at the diameter interface. However, regardless of the wide segment aspect ratio, the magnetization reversal is governed by the local radial stray fields of the modulation near null magnetization. Our findings demonstrate the capacity of distinguishing between complex magnetic behaviors involving convoluted interaction fields. |
format | Online Article Text |
id | pubmed-8706999 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-87069992021-12-25 Single Diameter Modulation Effects on Ni Nanowire Array Magnetization Reversal Arzuza, Luis C. C. Vega, Victor Prida, Victor M. Moura, Karoline O. Pirota, Kleber R. Béron, Fanny Nanomaterials (Basel) Article Geometrically modulated magnetic nanowires are a simple yet efficient strategy to modify the magnetic domain wall propagation since a simple diameter modulation can achieve its pinning during the nanowire magnetization reversal. However, in dense systems of parallel nanowires, the stray fields arising at the diameter interface can interfere with the domain wall propagation in the neighboring nanowires. Therefore, the magnetic behavior of diameter-modulated nanowire arrays can be quite complex and depending on both short and long-range interaction fields, as well as the nanowire geometric dimensions. We applied the first-order reversal curve (FORC) method to bi-segmented Ni nanowire arrays varying the wide segment (45–65 nm diameter, 2.5–10.0 μm length). The FORC results indicate a magnetic behavior modification depending on its length/diameter aspect ratio. The distributions either exhibit a strong extension along the coercivity axis or a main distribution finishing by a fork feature, whereas the extension greatly reduces in amplitude. With the help of micromagnetic simulations, we propose that a low aspect ratio stabilizes pinned domain walls at the diameter modulation during the magnetization reversal. In this case, long-range axial interaction fields nucleate a domain wall at the nanowire extremities, while short-range ones could induce a nucleation at the diameter interface. However, regardless of the wide segment aspect ratio, the magnetization reversal is governed by the local radial stray fields of the modulation near null magnetization. Our findings demonstrate the capacity of distinguishing between complex magnetic behaviors involving convoluted interaction fields. MDPI 2021-12-16 /pmc/articles/PMC8706999/ /pubmed/34947752 http://dx.doi.org/10.3390/nano11123403 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Arzuza, Luis C. C. Vega, Victor Prida, Victor M. Moura, Karoline O. Pirota, Kleber R. Béron, Fanny Single Diameter Modulation Effects on Ni Nanowire Array Magnetization Reversal |
title | Single Diameter Modulation Effects on Ni Nanowire Array Magnetization Reversal |
title_full | Single Diameter Modulation Effects on Ni Nanowire Array Magnetization Reversal |
title_fullStr | Single Diameter Modulation Effects on Ni Nanowire Array Magnetization Reversal |
title_full_unstemmed | Single Diameter Modulation Effects on Ni Nanowire Array Magnetization Reversal |
title_short | Single Diameter Modulation Effects on Ni Nanowire Array Magnetization Reversal |
title_sort | single diameter modulation effects on ni nanowire array magnetization reversal |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8706999/ https://www.ncbi.nlm.nih.gov/pubmed/34947752 http://dx.doi.org/10.3390/nano11123403 |
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