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分散在多孔二氧化硅基质中的激光辐照γ-FeO纳米晶体的结构行为:γ-FeO向α-FeO的相变及ε-FeO的形成

Structural behavior of laser-irradiated γ-FeO nanocrystals dispersed in porous silica matrix : γ-FeO to α-FeO phase transition and formation of ε-FeO.

作者信息

El Mendili Yassine, Bardeau Jean-François, Randrianantoandro Nirina, Greneche Jean-Marc, Grasset Fabien

机构信息

Institut des Molécules et Matériaux du Mans, UMR CNRS 6283, LUNAM Université , Le Mans , France.

Institut des Sciences Chimiques de Rennes, CNRS UMR 6226, Université Rennes 1, Rennes, France; CNRS-Saint Gobain, Laboratory for Innovative Key Materials and Structures, UMI 3629 LINK, National Institute of Material Science, Tsukuba, Japan.

出版信息

Sci Technol Adv Mater. 2016 Sep 29;17(1):597-609. doi: 10.1080/14686996.2016.1222494. eCollection 2016.

DOI:10.1080/14686996.2016.1222494
PMID:27877906
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5101921/
Abstract

The effects of laser irradiation on γ-FeO 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-FeO phase were carefully examined by X-ray diffraction and transmission electron microscopy. It has been shown that γ-FeO nanocrystals are isolated from each other and uniformly dispersed in silica matrix. The phase stability of maghemite nanocrystals was examined under laser irradiation by Raman spectroscopy and compared with that resulting from heat treatment by X-ray diffraction. It was concluded that ε-FeO is an intermediate phase between γ-FeO and -FeO and a series of distinct Raman vibrational bands were identified with the ε-FeO phase. The structural transformation of γ-FeO into -FeO occurs either directly or via ε-FeO, 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.

摘要

研究了激光辐照对通过共沉淀法合成并通过溶胶 - 凝胶法分散到无定形二氧化硅基质中的直径为γ-FeO 4 ± 1 nm的磁赤铁矿纳米晶体的影响,该影响是作为氧化铁质量分数的函数。通过X射线衍射和透射电子显微镜仔细研究了γ-FeO相的结构性质。结果表明,γ-FeO纳米晶体彼此分离并均匀分散在二氧化硅基质中。通过拉曼光谱研究了磁赤铁矿纳米晶体在激光辐照下的相稳定性,并与通过X射线衍射进行热处理得到的相稳定性进行了比较。得出的结论是,ε-FeO是γ-FeO和-FeO之间的中间相,并且用ε-FeO相鉴定出了一系列不同的拉曼振动带。γ-FeO向-FeO的结构转变直接发生或通过ε-FeO发生,这取决于纳米晶体的团聚速率、纳米复合材料中氧化铁的浓度以及二氧化硅基质的性质。建立了作为激光功率密度和浓度函数的相图。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/589001f3823c/tsta_a_1222494_f0013_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/f838b0752bc1/tsta_a_1222494_uf0001_oc.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/9193bb14b1d9/tsta_a_1222494_f0005_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/669c7c5bcd74/tsta_a_1222494_f0006_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/f7ea3138a78b/tsta_a_1222494_f0007_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/d0cb9d121454/tsta_a_1222494_f0008_b.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/1da34f0bb2c1/tsta_a_1222494_f0009_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/12e1779e0265/tsta_a_1222494_f0010_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/8046488c7d63/tsta_a_1222494_f0011_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/d5269b973e3b/tsta_a_1222494_f0012_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/589001f3823c/tsta_a_1222494_f0013_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/f838b0752bc1/tsta_a_1222494_uf0001_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/f405a06492eb/tsta_a_1222494_f0001_b.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/523b8387ad6a/tsta_a_1222494_f0002_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/6216edc02415/tsta_a_1222494_f0003_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/87a884799582/tsta_a_1222494_f0004_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/9193bb14b1d9/tsta_a_1222494_f0005_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/669c7c5bcd74/tsta_a_1222494_f0006_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/f7ea3138a78b/tsta_a_1222494_f0007_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/d0cb9d121454/tsta_a_1222494_f0008_b.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/1da34f0bb2c1/tsta_a_1222494_f0009_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/12e1779e0265/tsta_a_1222494_f0010_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/8046488c7d63/tsta_a_1222494_f0011_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/d5269b973e3b/tsta_a_1222494_f0012_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9153/5101921/589001f3823c/tsta_a_1222494_f0013_oc.jpg

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