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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Main Authors: | , , , , , , , |
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Format: | Journal Article |
Language: | English |
Published: |
19-04-2023
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Subjects: | |
Online Access: | Get full text |
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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. |
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DOI: | 10.48550/arxiv.2304.10048 |