Influence of misfit dislocations on the phase transition of iron(<scp>iii</scp>) oxides

Dislocations commonly occur in thin films under large misfit strain due to the accumulation of strain energy, significantly altering the films' properties. This study investigates the microstructure of Fe<sub>2</sub>O<sub>3</sub> polymorphs in films of various thicknesses deposited on yttria-stabilized zirconia (001) substrates. The results reveal that the ε-Fe<sub>2</sub>O<sub>3</sub> phase is formed and stabilized at thicknesses below a critical threshold of 20 nm. Beyond this threshold, the volume fraction of the ε-Fe<sub>2</sub>O<sub>3</sub> phase decreases, and the α-Fe<sub>2</sub>O<sub>3</sub> phase begins to emerge. With further increases in thickness, the ε-Fe<sub>2</sub>O<sub>3</sub> phase fully transforms into the α-Fe<sub>2</sub>O<sub>3</sub> phase. Detailed analysis suggests that this phase transformation is driven by the formation of misfit dislocations at the film/substrate interface, which compensates for the tensile strain induced by the substrate.

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Publication Details

Journal
Nanoscale Advances
Published
2025-01-01
DOI
https://doi.org/10.1039/d4na01061b
Primary Topic
Iron oxide chemistry and applications
Type
article
Field-Weighted Citation Impact
0.00

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article

Influence of misfit dislocations on the phase transition of iron(iii) oxides

Van-Hien Hoang, Nam‐Suk Lee, Heon‐Jung Kim
Nanoscale Advances
Iron oxide chemistry and applications
article

Influence of misfit dislocations on the phase transition of iron(iii) oxides

Van-Hien Hoang, Nam‐Suk Lee, Heon‐Jung Kim
article en

Abstract

Dislocations commonly occur in thin films under large misfit strain due to the accumulation of strain energy, significantly altering the films' properties. This study investigates the microstructure of Fe<sub>2</sub>O<sub>3</sub> polymorphs in films of various thicknesses deposited on yttria-stabilized zirconia (001) substrates. The results reveal that the ε-Fe<sub>2</sub>O<sub>3</sub> phase is formed and stabilized at thicknesses below a critical threshold of 20 nm. Beyond this threshold, the volume fraction of the ε-Fe<sub>2</sub>O<sub>3</sub> phase decreases, and the α-Fe<sub>2</sub>O<sub>3</sub> phase begins to emerge. With further increases in thickness, the ε-Fe<sub>2</sub>O<sub>3</sub> phase fully transforms into the α-Fe<sub>2</sub>O<sub>3</sub> phase. Detailed analysis suggests that this phase transformation is driven by the formation of misfit dislocations at the film/substrate interface, which compensates for the tensile strain induced by the substrate.

Nanoscale AdvancesVol. 7(14)
Pohang University of Science and Technology (KR), Daegu University (KR)
National Research Foundation, National Research Foundation of Korea, Ministry of SMEs and Startups
Affordable and clean energy
Openalex Percentile: Top 92%
Iron oxide chemistry and applications
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