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Structural behavior of laser-irradiated γ-Fe(2)O(3) nanocrystals dispersed in porous silica matrix : γ-Fe(2)O(3) to α-Fe(2)O(3) phase transition and formation of ε-Fe(2)O(3)

The effects of laser irradiation on γ-Fe(2)O(3) 4 ± 1 nm diameter maghemite nanocrystals synthesized by co-precipitation and dispersed into an amorphous silica matrix by sol-gel methods have been investigated as function of iron oxide mass fraction. The structural properties of γ-Fe(2)O(3) phase wer...

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Autores principales: El Mendili, Yassine, Bardeau, Jean-François, Randrianantoandro, Nirina, Greneche, Jean-Marc, Grasset, Fabien
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Taylor & Francis 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5101921/
https://www.ncbi.nlm.nih.gov/pubmed/27877906
http://dx.doi.org/10.1080/14686996.2016.1222494
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author El Mendili, Yassine
Bardeau, Jean-François
Randrianantoandro, Nirina
Greneche, Jean-Marc
Grasset, Fabien
author_facet El Mendili, Yassine
Bardeau, Jean-François
Randrianantoandro, Nirina
Greneche, Jean-Marc
Grasset, Fabien
author_sort El Mendili, Yassine
collection PubMed
description The effects of laser irradiation on γ-Fe(2)O(3) 4 ± 1 nm diameter maghemite nanocrystals synthesized by co-precipitation and dispersed into an amorphous silica matrix by sol-gel methods have been investigated as function of iron oxide mass fraction. The structural properties of γ-Fe(2)O(3) phase were carefully examined by X-ray diffraction and transmission electron microscopy. It has been shown that γ-Fe(2)O(3) nanocrystals are isolated from each other and uniformly dispersed in silica matrix. The phase stability of maghemite nanocrystals was examined in situ under laser irradiation by Raman spectroscopy and compared with that resulting from heat treatment by X-ray diffraction. It was concluded that ε-Fe(2)O(3) is an intermediate phase between γ-Fe(2)O(3) and α-Fe(2)O(3) and a series of distinct Raman vibrational bands were identified with the ε-Fe(2)O(3) phase. The structural transformation of γ-Fe(2)O(3) into α-Fe(2)O(3) occurs either directly or via ε-Fe(2)O(3), depending on the rate of nanocrystal agglomeration, the concentration of iron oxide in the nanocomposite and the properties of silica matrix. A phase diagram is established as a function of laser power density and concentration.
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spelling pubmed-51019212016-11-22 Structural behavior of laser-irradiated γ-Fe(2)O(3) nanocrystals dispersed in porous silica matrix : γ-Fe(2)O(3) to α-Fe(2)O(3) phase transition and formation of ε-Fe(2)O(3) El Mendili, Yassine Bardeau, Jean-François Randrianantoandro, Nirina Greneche, Jean-Marc Grasset, Fabien Sci Technol Adv Mater Engineering and Structural materials The effects of laser irradiation on γ-Fe(2)O(3) 4 ± 1 nm diameter maghemite nanocrystals synthesized by co-precipitation and dispersed into an amorphous silica matrix by sol-gel methods have been investigated as function of iron oxide mass fraction. The structural properties of γ-Fe(2)O(3) phase were carefully examined by X-ray diffraction and transmission electron microscopy. It has been shown that γ-Fe(2)O(3) nanocrystals are isolated from each other and uniformly dispersed in silica matrix. The phase stability of maghemite nanocrystals was examined in situ under laser irradiation by Raman spectroscopy and compared with that resulting from heat treatment by X-ray diffraction. It was concluded that ε-Fe(2)O(3) is an intermediate phase between γ-Fe(2)O(3) and α-Fe(2)O(3) and a series of distinct Raman vibrational bands were identified with the ε-Fe(2)O(3) phase. The structural transformation of γ-Fe(2)O(3) into α-Fe(2)O(3) occurs either directly or via ε-Fe(2)O(3), depending on the rate of nanocrystal agglomeration, the concentration of iron oxide in the nanocomposite and the properties of silica matrix. A phase diagram is established as a function of laser power density and concentration. Taylor & Francis 2016-09-29 /pmc/articles/PMC5101921/ /pubmed/27877906 http://dx.doi.org/10.1080/14686996.2016.1222494 Text en © 2016 The Author(s). Published by National Institute for Materials Science in partnership with Taylor & Francis http://creativecommons.org/licenses/by/4.0/ This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Engineering and Structural materials
El Mendili, Yassine
Bardeau, Jean-François
Randrianantoandro, Nirina
Greneche, Jean-Marc
Grasset, Fabien
Structural behavior of laser-irradiated γ-Fe(2)O(3) nanocrystals dispersed in porous silica matrix : γ-Fe(2)O(3) to α-Fe(2)O(3) phase transition and formation of ε-Fe(2)O(3)
title Structural behavior of laser-irradiated γ-Fe(2)O(3) nanocrystals dispersed in porous silica matrix : γ-Fe(2)O(3) to α-Fe(2)O(3) phase transition and formation of ε-Fe(2)O(3)
title_full Structural behavior of laser-irradiated γ-Fe(2)O(3) nanocrystals dispersed in porous silica matrix : γ-Fe(2)O(3) to α-Fe(2)O(3) phase transition and formation of ε-Fe(2)O(3)
title_fullStr Structural behavior of laser-irradiated γ-Fe(2)O(3) nanocrystals dispersed in porous silica matrix : γ-Fe(2)O(3) to α-Fe(2)O(3) phase transition and formation of ε-Fe(2)O(3)
title_full_unstemmed Structural behavior of laser-irradiated γ-Fe(2)O(3) nanocrystals dispersed in porous silica matrix : γ-Fe(2)O(3) to α-Fe(2)O(3) phase transition and formation of ε-Fe(2)O(3)
title_short Structural behavior of laser-irradiated γ-Fe(2)O(3) nanocrystals dispersed in porous silica matrix : γ-Fe(2)O(3) to α-Fe(2)O(3) phase transition and formation of ε-Fe(2)O(3)
title_sort structural behavior of laser-irradiated γ-fe(2)o(3) nanocrystals dispersed in porous silica matrix : γ-fe(2)o(3) to α-fe(2)o(3) phase transition and formation of ε-fe(2)o(3)
topic Engineering and Structural materials
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5101921/
https://www.ncbi.nlm.nih.gov/pubmed/27877906
http://dx.doi.org/10.1080/14686996.2016.1222494
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