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Relation of the average interaction field with the coercive and interaction field distributions in First order reversal curve diagrams of nanowire arrays
First-order reversal curve diagrams, or FORC diagrams, have been studied to determine if the widths of their distributions along the interaction and coercivity axes can be related to the mean-field magnetization dependent interaction field (MDIF). Arrays of nanowires with diameters ranging from 18 u...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7721885/ https://www.ncbi.nlm.nih.gov/pubmed/33288826 http://dx.doi.org/10.1038/s41598-020-78279-1 |
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author | Velázquez, Y. G. Guerrero, A. Lobo Martínez, J. M. Araujo, E. Tabasum, M. R. Nysten, B. Piraux, L. Encinas, A. |
author_facet | Velázquez, Y. G. Guerrero, A. Lobo Martínez, J. M. Araujo, E. Tabasum, M. R. Nysten, B. Piraux, L. Encinas, A. |
author_sort | Velázquez, Y. G. |
collection | PubMed |
description | First-order reversal curve diagrams, or FORC diagrams, have been studied to determine if the widths of their distributions along the interaction and coercivity axes can be related to the mean-field magnetization dependent interaction field (MDIF). Arrays of nanowires with diameters ranging from 18 up to 100 nm and packing fractions varying from 0.4 to 12% have been analyzed. The mean-field MDIF has been measured using the remanence curves and used as a measuring scale on the FORC diagrams. Based on these measurements, the full width of the interaction field distribution and the full width at half maximum (FWHM) of the FORC distribution profile along the interaction field direction are shown to be proportional to the MDIF, and the relation between them is found. Moreover, by interpreting the full width of the coercive field distribution in terms of the dipolar induced shearing, a simple relation is found between the width of this distribution and the MDIF. Furthermore, we show that the width of the FORC distribution along the coercive field axis is equal to the width of the switching field distribution obtained by the derivation of the DC remanence curve. This was further verified with the switching field distribution determined using in-field magnetic force microscopy (MFM) for very low density nanowires. The results are further supported by the good agreement found between the experiments and the values calculated using the mean-field model, which provides analytical expressions for both FORC distributions. |
format | Online Article Text |
id | pubmed-7721885 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-77218852020-12-09 Relation of the average interaction field with the coercive and interaction field distributions in First order reversal curve diagrams of nanowire arrays Velázquez, Y. G. Guerrero, A. Lobo Martínez, J. M. Araujo, E. Tabasum, M. R. Nysten, B. Piraux, L. Encinas, A. Sci Rep Article First-order reversal curve diagrams, or FORC diagrams, have been studied to determine if the widths of their distributions along the interaction and coercivity axes can be related to the mean-field magnetization dependent interaction field (MDIF). Arrays of nanowires with diameters ranging from 18 up to 100 nm and packing fractions varying from 0.4 to 12% have been analyzed. The mean-field MDIF has been measured using the remanence curves and used as a measuring scale on the FORC diagrams. Based on these measurements, the full width of the interaction field distribution and the full width at half maximum (FWHM) of the FORC distribution profile along the interaction field direction are shown to be proportional to the MDIF, and the relation between them is found. Moreover, by interpreting the full width of the coercive field distribution in terms of the dipolar induced shearing, a simple relation is found between the width of this distribution and the MDIF. Furthermore, we show that the width of the FORC distribution along the coercive field axis is equal to the width of the switching field distribution obtained by the derivation of the DC remanence curve. This was further verified with the switching field distribution determined using in-field magnetic force microscopy (MFM) for very low density nanowires. The results are further supported by the good agreement found between the experiments and the values calculated using the mean-field model, which provides analytical expressions for both FORC distributions. Nature Publishing Group UK 2020-12-07 /pmc/articles/PMC7721885/ /pubmed/33288826 http://dx.doi.org/10.1038/s41598-020-78279-1 Text en © The Author(s) 2020 Open AccessThis 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/. |
spellingShingle | Article Velázquez, Y. G. Guerrero, A. Lobo Martínez, J. M. Araujo, E. Tabasum, M. R. Nysten, B. Piraux, L. Encinas, A. Relation of the average interaction field with the coercive and interaction field distributions in First order reversal curve diagrams of nanowire arrays |
title | Relation of the average interaction field with the coercive and interaction field distributions in First order reversal curve diagrams of nanowire arrays |
title_full | Relation of the average interaction field with the coercive and interaction field distributions in First order reversal curve diagrams of nanowire arrays |
title_fullStr | Relation of the average interaction field with the coercive and interaction field distributions in First order reversal curve diagrams of nanowire arrays |
title_full_unstemmed | Relation of the average interaction field with the coercive and interaction field distributions in First order reversal curve diagrams of nanowire arrays |
title_short | Relation of the average interaction field with the coercive and interaction field distributions in First order reversal curve diagrams of nanowire arrays |
title_sort | relation of the average interaction field with the coercive and interaction field distributions in first order reversal curve diagrams of nanowire arrays |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7721885/ https://www.ncbi.nlm.nih.gov/pubmed/33288826 http://dx.doi.org/10.1038/s41598-020-78279-1 |
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