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Magneto-optical properties of Fe-Pt alloy films in the range 1.55–10.5 eV
33
Citations
26
References
1993
Year
Magnetic PropertiesOptical MaterialsRange 1.55–10.5EngineeringMagnetic ResonanceBulk FeMagnetic MaterialsMagnetoresistanceMagnetismMultiferroicsPeak ShiftOptical PropertiesFe-pt Alloy FilmsMagnetic Thin FilmsEv RegionMaterials SciencePhysicsLow-dimensional SystemsMagnetoelasticityMagnetic MaterialFerromagnetismMagneto-optical PropertiesNatural SciencesApplied PhysicsCondensed Matter PhysicsThin FilmsMagnetic Property
The optical and magneto-optical properties of as-deposited and annealed ${\mathrm{Fe}}_{51}$${\mathrm{Pt}}_{49}$ films were investigated in the photon energy range 1.55--10.5 eV. The magneto-optical Kerr rotation (${\mathrm{\ensuremath{\theta}}}_{\mathrm{K}}$) spectra of both films were found to show a dispersion-type structure in the 4.6--7.8 eV region: they have large negative and broad positive peaks at around 4.8 and 7.8 eV, respectively. The ${\mathrm{\ensuremath{\theta}}}_{\mathrm{K}}$ spectra showed a tendency that is essentially quite similar to that of bulk Fe. The Kerr ellipticity (${\mathrm{\ensuremath{\eta}}}_{\mathrm{K}}$) spectra are bell shaped, exhibiting a large negative peak at 6.3 eV. Plasma edges were observed at 6.9 eV for the as-deposited film and at 7.3 eV for the annealed film. The absolute value of the real part of the off-diagonal dielectric element (${\mathrm{\ensuremath{\varepsilon}}}_{\mathrm{XY}}^{\ensuremath{'}}$) of both films at \ensuremath{\sim}4.8 eV are almost the same as that of bulk Fe. This leads to the conclusion that the ${\mathrm{\ensuremath{\theta}}}_{\mathrm{K}}$ enhancement at 4.8 eV is mainly due to a decrease in ${\mathrm{\ensuremath{\varepsilon}}}_{\mathrm{XX}}^{\mathrm{\ensuremath{''}}}$ and a peak shift in ${\mathrm{\ensuremath{\varepsilon}}}_{\mathrm{XY}}^{\ensuremath{'}}$ towards lower energy, but not to a plasma-resonance effect.
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