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Transition from AFM Spin Canting to Spin Glass–AFM Exchange as Particle Size Decreases in LaFeO(3)
In this work, we have studied structural and magnetic properties of LaFeO(3) as a function of the particle size d, from bulk (d >> 1 µm) to nanoscale (d ≈ 30 nm). A large number of twins were observed for large particles that disappear for small particle sizes. This could be related to the sof...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10224450/ https://www.ncbi.nlm.nih.gov/pubmed/37242073 http://dx.doi.org/10.3390/nano13101657 |
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author | Alshalawi, Dhoha Alonso, Jose María Landa-Cánovas, Angel R. de la Presa, Patricia |
author_facet | Alshalawi, Dhoha Alonso, Jose María Landa-Cánovas, Angel R. de la Presa, Patricia |
author_sort | Alshalawi, Dhoha |
collection | PubMed |
description | In this work, we have studied structural and magnetic properties of LaFeO(3) as a function of the particle size d, from bulk (d >> 1 µm) to nanoscale (d ≈ 30 nm). A large number of twins were observed for large particles that disappear for small particle sizes. This could be related to the softening of the FeO(6) distortion as particle size decreases. It was observed that the bulk sample showed spin canting that disappeared for d ~ 125 nm and can be associated with the smoothening of the orthorhombic distortion. On the other hand, for d < 60 nm, the surface/volume ratio became high and, despite the high crystallinity of the nanoparticle, a notable exchange effect bias appeared, originated by two magnetic interactions: spin glass and antiferromagnetism. This exchange bias interaction was originated by the formation of a “magnetic core–shell”: the broken bonds at the surface atoms give place to a spin glass behavior, whereas the inner atoms maintain the antiferromagnetic G-type order. The LaFeO(3) bulk material was synthesized by the ceramic method, whereas the LaFeO(3) nanoparticles were synthesized by the sol-gel method; the particle size was varied by annealing the samples at different temperatures. The physical properties of the materials have been investigated by XRD, HRTEM, TGA, and AC and DC magnetometry. |
format | Online Article Text |
id | pubmed-10224450 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-102244502023-05-28 Transition from AFM Spin Canting to Spin Glass–AFM Exchange as Particle Size Decreases in LaFeO(3) Alshalawi, Dhoha Alonso, Jose María Landa-Cánovas, Angel R. de la Presa, Patricia Nanomaterials (Basel) Article In this work, we have studied structural and magnetic properties of LaFeO(3) as a function of the particle size d, from bulk (d >> 1 µm) to nanoscale (d ≈ 30 nm). A large number of twins were observed for large particles that disappear for small particle sizes. This could be related to the softening of the FeO(6) distortion as particle size decreases. It was observed that the bulk sample showed spin canting that disappeared for d ~ 125 nm and can be associated with the smoothening of the orthorhombic distortion. On the other hand, for d < 60 nm, the surface/volume ratio became high and, despite the high crystallinity of the nanoparticle, a notable exchange effect bias appeared, originated by two magnetic interactions: spin glass and antiferromagnetism. This exchange bias interaction was originated by the formation of a “magnetic core–shell”: the broken bonds at the surface atoms give place to a spin glass behavior, whereas the inner atoms maintain the antiferromagnetic G-type order. The LaFeO(3) bulk material was synthesized by the ceramic method, whereas the LaFeO(3) nanoparticles were synthesized by the sol-gel method; the particle size was varied by annealing the samples at different temperatures. The physical properties of the materials have been investigated by XRD, HRTEM, TGA, and AC and DC magnetometry. MDPI 2023-05-17 /pmc/articles/PMC10224450/ /pubmed/37242073 http://dx.doi.org/10.3390/nano13101657 Text en © 2023 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 Alshalawi, Dhoha Alonso, Jose María Landa-Cánovas, Angel R. de la Presa, Patricia Transition from AFM Spin Canting to Spin Glass–AFM Exchange as Particle Size Decreases in LaFeO(3) |
title | Transition from AFM Spin Canting to Spin Glass–AFM Exchange as Particle Size Decreases in LaFeO(3) |
title_full | Transition from AFM Spin Canting to Spin Glass–AFM Exchange as Particle Size Decreases in LaFeO(3) |
title_fullStr | Transition from AFM Spin Canting to Spin Glass–AFM Exchange as Particle Size Decreases in LaFeO(3) |
title_full_unstemmed | Transition from AFM Spin Canting to Spin Glass–AFM Exchange as Particle Size Decreases in LaFeO(3) |
title_short | Transition from AFM Spin Canting to Spin Glass–AFM Exchange as Particle Size Decreases in LaFeO(3) |
title_sort | transition from afm spin canting to spin glass–afm exchange as particle size decreases in lafeo(3) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10224450/ https://www.ncbi.nlm.nih.gov/pubmed/37242073 http://dx.doi.org/10.3390/nano13101657 |
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