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Spin-Glass Transitions in Zn(1-x)Fe(x)O Nanoparticles
Monophasic Zn(1-x)Fe(x)O nanoparticles with wurtzite structure were synthesized in the 0 ≤ x ≤ 0.05 concentration range using a freeze-drying process followed by heat treatment. The samples were characterized regarding their optical, structural, and magnetic properties. The analyses revealed that ir...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7079620/ https://www.ncbi.nlm.nih.gov/pubmed/32075143 http://dx.doi.org/10.3390/ma13040869 |
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author | Felipe S. Tupan, Lilian Valerio-Cuadros, Marlon I. Oliveira, Aline Alves Barco, Reginaldo Ivashita, Flávio Francisco Lopes, Lutiene F. Passamani, Edson C. Paesano, Andrea |
author_facet | Felipe S. Tupan, Lilian Valerio-Cuadros, Marlon I. Oliveira, Aline Alves Barco, Reginaldo Ivashita, Flávio Francisco Lopes, Lutiene F. Passamani, Edson C. Paesano, Andrea |
author_sort | Felipe S. Tupan, Lilian |
collection | PubMed |
description | Monophasic Zn(1-x)Fe(x)O nanoparticles with wurtzite structure were synthesized in the 0 ≤ x ≤ 0.05 concentration range using a freeze-drying process followed by heat treatment. The samples were characterized regarding their optical, structural, and magnetic properties. The analyses revealed that iron doping of the ZnO matrix induces morphological changes in the crystallites. Iron is substitutional for zinc, trivalent and distributed in the wurtzite lattice in two groups: isolated iron atoms and iron atoms with one or more neighboring iron atoms. It was also shown that the energy band gap decreases with a higher doping level. The samples are paramagnetic at room temperature, but they undergo a spin-glass transition when the temperature drops below 75 K. The magnetic frustration is attributed to the competition of magnetic interactions among the iron moments. There are a superexchange interaction and an indirect exchange interaction that is provided by the spin (and charge) itinerant carriers in a spin-polarized band situated in the vicinity of the Fermi level of the Fe-doped ZnO semiconductor. The former interaction actuates for an antiferromagnetic coupling among iron ions, whereas the latter constitutes a driving force for a ferromagnetic coupling that weakens, decreasing the temperature. Our results strongly contribute to the literature because they elucidate the controversies reported in the literature for the magnetic state of the Fe-doped ZnO system. |
format | Online Article Text |
id | pubmed-7079620 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-70796202020-03-24 Spin-Glass Transitions in Zn(1-x)Fe(x)O Nanoparticles Felipe S. Tupan, Lilian Valerio-Cuadros, Marlon I. Oliveira, Aline Alves Barco, Reginaldo Ivashita, Flávio Francisco Lopes, Lutiene F. Passamani, Edson C. Paesano, Andrea Materials (Basel) Article Monophasic Zn(1-x)Fe(x)O nanoparticles with wurtzite structure were synthesized in the 0 ≤ x ≤ 0.05 concentration range using a freeze-drying process followed by heat treatment. The samples were characterized regarding their optical, structural, and magnetic properties. The analyses revealed that iron doping of the ZnO matrix induces morphological changes in the crystallites. Iron is substitutional for zinc, trivalent and distributed in the wurtzite lattice in two groups: isolated iron atoms and iron atoms with one or more neighboring iron atoms. It was also shown that the energy band gap decreases with a higher doping level. The samples are paramagnetic at room temperature, but they undergo a spin-glass transition when the temperature drops below 75 K. The magnetic frustration is attributed to the competition of magnetic interactions among the iron moments. There are a superexchange interaction and an indirect exchange interaction that is provided by the spin (and charge) itinerant carriers in a spin-polarized band situated in the vicinity of the Fermi level of the Fe-doped ZnO semiconductor. The former interaction actuates for an antiferromagnetic coupling among iron ions, whereas the latter constitutes a driving force for a ferromagnetic coupling that weakens, decreasing the temperature. Our results strongly contribute to the literature because they elucidate the controversies reported in the literature for the magnetic state of the Fe-doped ZnO system. MDPI 2020-02-14 /pmc/articles/PMC7079620/ /pubmed/32075143 http://dx.doi.org/10.3390/ma13040869 Text en © 2020 by the authors. 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 (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Felipe S. Tupan, Lilian Valerio-Cuadros, Marlon I. Oliveira, Aline Alves Barco, Reginaldo Ivashita, Flávio Francisco Lopes, Lutiene F. Passamani, Edson C. Paesano, Andrea Spin-Glass Transitions in Zn(1-x)Fe(x)O Nanoparticles |
title | Spin-Glass Transitions in Zn(1-x)Fe(x)O Nanoparticles |
title_full | Spin-Glass Transitions in Zn(1-x)Fe(x)O Nanoparticles |
title_fullStr | Spin-Glass Transitions in Zn(1-x)Fe(x)O Nanoparticles |
title_full_unstemmed | Spin-Glass Transitions in Zn(1-x)Fe(x)O Nanoparticles |
title_short | Spin-Glass Transitions in Zn(1-x)Fe(x)O Nanoparticles |
title_sort | spin-glass transitions in zn(1-x)fe(x)o nanoparticles |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7079620/ https://www.ncbi.nlm.nih.gov/pubmed/32075143 http://dx.doi.org/10.3390/ma13040869 |
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