Control of conductivity in Fe-rich cobalt-ferrite thin films with perpendicular magnetic anisotropy

We fabricated two types of cobalt-ferrite (001) thin films, insulative Fe-rich cobalt-ferrite CoxFe3-xO4+{\delta} (I-CFO) and conductive Fe-rich cobalt-ferrite CoyFe3-yO4 (C-CFO), with perpendicular magnetic anisotropy (PMA) on MgO (001) substrates. Although the stoichiometric cobalt-ferrite is know...

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Bibliographic Details
Main Authors: Morishita, Masaya, Ichikawa, Tomoyuki, Tanaka, Masaaki A, Furuta, Motoharu, Mashimo, Daisuke, Honda, Syuta, Okabayashi, Jun, Mibu, Ko
Format: Journal Article
Language:English
Published: 19-04-2023
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Summary:We fabricated two types of cobalt-ferrite (001) thin films, insulative Fe-rich cobalt-ferrite CoxFe3-xO4+{\delta} (I-CFO) and conductive Fe-rich cobalt-ferrite CoyFe3-yO4 (C-CFO), with perpendicular magnetic anisotropy (PMA) on MgO (001) substrates. Although the stoichiometric cobalt-ferrite is known as an insulating material, it is found that the conductivity of Fe-rich cobalt-ferrites can be controlled by changing the source materials and deposition conditions in the pulsed laser deposition technique. The I-CFO and C-CFO films exhibit PMA through the in-plane lattice distortion. We investigated the Fe-ion-specific valence states in both I-CFO and C-CFO films by M\"ossbauer spectroscopy and X-ray magnetic circular dichroism, and found that the difference in conductivity corresponds to the abundance ratio of Fe2+ state at the octahedral B-site (Oh) in the inverse spinel structure. Furthermore, first-principles calculations reproduce the changes in the density of states at the Fermi level depending on the cation vacancies at the B-site, which explains the difference in the conductivity between I-CFO and C-CFO.
DOI:10.48550/arxiv.2304.10048