Publication | Open Access
Structural behavior of laser-irradiated γ-Fe<sub>2</sub>O<sub>3</sub> nanocrystals dispersed in porous silica matrix : γ-Fe<sub>2</sub>O<sub>3</sub> to α-Fe<sub>2</sub>O<sub>3</sub> phase transition and formation of ε-Fe<sub>2</sub>O<sub>3</sub>
65
Citations
48
References
2016
Year
The effects of laser irradiation on γ-Fe<sub>2</sub>O<sub>3</sub> 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<sub>2</sub>O<sub>3</sub> phase were carefully examined by X-ray diffraction and transmission electron microscopy. It has been shown that γ-Fe<sub>2</sub>O<sub>3</sub> nanocrystals are isolated from each other and uniformly dispersed in silica matrix. The phase stability of maghemite nanocrystals was examined <i>in situ</i> under laser irradiation by Raman spectroscopy and compared with that resulting from heat treatment by X-ray diffraction. It was concluded that ε-Fe<sub>2</sub>O<sub>3</sub> is an intermediate phase between γ-Fe<sub>2</sub>O<sub>3</sub> and <i>α</i>-Fe<sub>2</sub>O<sub>3</sub> and a series of distinct Raman vibrational bands were identified with the ε-Fe<sub>2</sub>O<sub>3</sub> phase. The structural transformation of γ-Fe<sub>2</sub>O<sub>3</sub> into <i>α</i>-Fe<sub>2</sub>O<sub>3</sub> occurs either directly or via ε-Fe<sub>2</sub>O<sub>3</sub>, 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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