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Sn(2+) Doping: A Strategy for Tuning of Fe(3)O(4) Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point
Doped magnetite (Sn(x)Fe(3-2/3x)O(4)) nanoparticles (NPs) (12–50 nm) with different amount of Sn(2+) ions (x) were synthesized using co-precipitation method. Sn(2+) doping reduces the anticipated oxidation of Fe(3)O(4) NPs to maghemite (γ-Fe(2)O(3)), making them attractive in several magnetic applic...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Springer US
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7530164/ https://www.ncbi.nlm.nih.gov/pubmed/33001332 http://dx.doi.org/10.1186/s11671-020-03423-9 |
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author | Al-Kindi, Umaima S. H. Al-Harthi, Salim H. Widatallah, Hisham M. Elzain, Mohamed E. Myint, Myo T. Z. Kyaw, Htet H. |
author_facet | Al-Kindi, Umaima S. H. Al-Harthi, Salim H. Widatallah, Hisham M. Elzain, Mohamed E. Myint, Myo T. Z. Kyaw, Htet H. |
author_sort | Al-Kindi, Umaima S. H. |
collection | PubMed |
description | Doped magnetite (Sn(x)Fe(3-2/3x)O(4)) nanoparticles (NPs) (12–50 nm) with different amount of Sn(2+) ions (x) were synthesized using co-precipitation method. Sn(2+) doping reduces the anticipated oxidation of Fe(3)O(4) NPs to maghemite (γ-Fe(2)O(3)), making them attractive in several magnetic applications. Detailed characterizations during heating–cooling cycles revealed the possibility of tuning the unusual observed magnetization dipping temperature/amplitude, irreversibility, and Curie point of these NPs. We attribute this dip to the chemical reduction of γ-Fe(2)O(3) at the NPs surfaces. Along with an increase in the dipping temperature, we found that doping with Sn(2+) reduces the dipping amplitude, until it approximately disappears when x = 0.150. Based on the core-shell structure of these NPs, a phenomenological expression that combines both modified Bloch law (M = M(0)[1 − γ(T/T(C))](β)) and a modified Curie–Weiss law (M = − α[1/(T − T(C))(δ)]) is developed in order to explain the observed M-T behavior at different applied external magnetic fields and for different Sn(2+) concentrations. By applying high enough magnetic field, the value of the parameters γ and δ ≈ 1 which are the same in modified Bloch and Curie–Weiss laws. They do not change with the magnetic field and depend only on the material structure and size. The power β for high magnetic field was 2.6 which is as expected for this size of nanoparticles with the core dominated magnetization. However, the β value fluctuates between 3 and 10 for small magnetic fields indicating an extra magnetic contribution from the shell structure presented by Curie–Weiss term. The parameter (α) has a very small value and it turns to negative values for high magnetic fields. |
format | Online Article Text |
id | pubmed-7530164 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | Springer US |
record_format | MEDLINE/PubMed |
spelling | pubmed-75301642020-10-19 Sn(2+) Doping: A Strategy for Tuning of Fe(3)O(4) Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point Al-Kindi, Umaima S. H. Al-Harthi, Salim H. Widatallah, Hisham M. Elzain, Mohamed E. Myint, Myo T. Z. Kyaw, Htet H. Nanoscale Res Lett Nano Express Doped magnetite (Sn(x)Fe(3-2/3x)O(4)) nanoparticles (NPs) (12–50 nm) with different amount of Sn(2+) ions (x) were synthesized using co-precipitation method. Sn(2+) doping reduces the anticipated oxidation of Fe(3)O(4) NPs to maghemite (γ-Fe(2)O(3)), making them attractive in several magnetic applications. Detailed characterizations during heating–cooling cycles revealed the possibility of tuning the unusual observed magnetization dipping temperature/amplitude, irreversibility, and Curie point of these NPs. We attribute this dip to the chemical reduction of γ-Fe(2)O(3) at the NPs surfaces. Along with an increase in the dipping temperature, we found that doping with Sn(2+) reduces the dipping amplitude, until it approximately disappears when x = 0.150. Based on the core-shell structure of these NPs, a phenomenological expression that combines both modified Bloch law (M = M(0)[1 − γ(T/T(C))](β)) and a modified Curie–Weiss law (M = − α[1/(T − T(C))(δ)]) is developed in order to explain the observed M-T behavior at different applied external magnetic fields and for different Sn(2+) concentrations. By applying high enough magnetic field, the value of the parameters γ and δ ≈ 1 which are the same in modified Bloch and Curie–Weiss laws. They do not change with the magnetic field and depend only on the material structure and size. The power β for high magnetic field was 2.6 which is as expected for this size of nanoparticles with the core dominated magnetization. However, the β value fluctuates between 3 and 10 for small magnetic fields indicating an extra magnetic contribution from the shell structure presented by Curie–Weiss term. The parameter (α) has a very small value and it turns to negative values for high magnetic fields. Springer US 2020-10-01 /pmc/articles/PMC7530164/ /pubmed/33001332 http://dx.doi.org/10.1186/s11671-020-03423-9 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 | Nano Express Al-Kindi, Umaima S. H. Al-Harthi, Salim H. Widatallah, Hisham M. Elzain, Mohamed E. Myint, Myo T. Z. Kyaw, Htet H. Sn(2+) Doping: A Strategy for Tuning of Fe(3)O(4) Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point |
title | Sn(2+) Doping: A Strategy for Tuning of Fe(3)O(4) Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point |
title_full | Sn(2+) Doping: A Strategy for Tuning of Fe(3)O(4) Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point |
title_fullStr | Sn(2+) Doping: A Strategy for Tuning of Fe(3)O(4) Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point |
title_full_unstemmed | Sn(2+) Doping: A Strategy for Tuning of Fe(3)O(4) Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point |
title_short | Sn(2+) Doping: A Strategy for Tuning of Fe(3)O(4) Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point |
title_sort | sn(2+) doping: a strategy for tuning of fe(3)o(4) nanoparticles magnetization dipping temperature/amplitude, irreversibility, and curie point |
topic | Nano Express |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7530164/ https://www.ncbi.nlm.nih.gov/pubmed/33001332 http://dx.doi.org/10.1186/s11671-020-03423-9 |
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