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Thickness dependence of anomalous magnetic behavior in epitaxial Fe3O4(111) thin films: Effect of density of antiphase boundaries
135
Citations
30
References
2004
Year
Thin Film PhysicsMagnetic PropertiesSingle CrystalsEngineeringAntiphase BoundariesThin Film Process TechnologyMagnetoresistanceMagnetismMagnetic Thin FilmsEpitaxial GrowthMaterials ScienceThickness DependencePhysicsMagnetic MaterialMagnetic Moment VariesFerromagnetismNatural SciencesCondensed Matter PhysicsApplied PhysicsThin FilmsMagnetic Property
We study the magnetic behavior of ${\mathrm{Fe}}_{3}{\mathrm{O}}_{4}(111)$ thin films with thicknesses between $5\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$ and $50\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$. The films are epitaxially grown on $\ensuremath{\alpha}\text{\ensuremath{-}}{\mathrm{Al}}_{2}{\mathrm{O}}_{3}(0001)$ single crystals by atomic-oxygen-assisted molecular beam epitaxy. The ${\mathrm{Fe}}_{3}{\mathrm{O}}_{4}(111)$ thin films exhibit high structural order with sharp interfaces and low roughness and exhibit a Verwey transition for thicknesses above $8\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$. However, the samples have magnetic properties that deviate from the bulk ones. The magnetic moment varies between $2.4{\ensuremath{\mu}}_{B}$ for $5\text{\ensuremath{-}}\mathrm{nm}$-thick film and $3.2{\ensuremath{\mu}}_{B}$ for $50\text{\ensuremath{-}}\mathrm{nm}$-thick film in a field of $1.2\phantom{\rule{0.3em}{0ex}}\mathrm{T}$, which is lower than that of bulk samples ($4.1{\ensuremath{\mu}}_{B}∕{\mathrm{Fe}}_{3}{\mathrm{O}}_{4}$ formula). Still the magnetic saturation is never reached, even in fields as large as $2\phantom{\rule{0.3em}{0ex}}T$. The thinner the film, the slower the approach to saturation. Structural analysis, performed using high-resolution transmission electron microscopy, reveals the presence of antiphase boundaries (APB's), the density of which decreases when the thickness increases. Using a model of ferromagnetic domains separated by antiferromagnetically sharp interfaces, we show that the slow approach to saturation observed in the films as a function of thickness is driven by the APB density.
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