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Magneto-optic spectra and the dielectric tensor elements of bismuth-substituted iron garnets at photon energies between 2.2-5.2 eV
353
Citations
19
References
1975
Year
Bismuth-substituted Iron GarnetsMagnetic PropertiesOptical MaterialsEngineeringMagnetic ResonanceMagnetic MaterialsMagnetoresistanceMagnetismMultiferroicsMagnetoplasmonicsOptical PropertiesDielectric Tensor ElementsMossbauer SpectroscopyKerr RotationMaterials SciencePhysicsBismuth SubstitutionMagnetoelasticityMagnetic MaterialQuantum MagnetismFerromagnetismNatural SciencesCondensed Matter PhysicsApplied PhysicsPhoton EnergiesEnergy Level SchemeThin FilmsMagnetic Property
Optical and magneto-optical measurements have been performed at room temperature on both polycrystalline samples and thin single-crystal films of bismuth-substituted iron garnets. Kerr rotation, ellipticity, and reflectivity are given for polycrystalline samples of composition ${\mathrm{Y}}_{3\ensuremath{-}x}{\mathrm{Bi}}_{x}{\mathrm{Fe}}_{5}{\mathrm{O}}_{12}$ ($0<x\ensuremath{\le}1$) between 2.0 and 5.2 eV (wavelengths between 0.6 and 0.24 \ensuremath{\mu}m). The absorption and the Faraday rotation and ellipticity of epitaxial films with $0<x<0.5$ were measured up to 3.5 eV. The experimental results have been used to calculate the diagonal and off-diagonal elements of the dielectric tensor at optical frequencies. Strong magneto-optic active transitions have been found at 2.8, 3.3, 4.1, and 4.9 eV, apart from the weaker crystal-field transitions. The bands at 2.8 and 3.3 have been studied in more detail: The oscillator strengths and splittings due to spin-orbit coupling were calculated, both increase with bismuth substitution. The large splitting of the band at 3.3 eV for the bismuth-substituted compounds is concluded to be the origin of the anomalous Faraday rotation of these compounds. The assignment of these bands in terms of an energy level scheme is discussed.
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