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Dielectric properties of Mn doped SrTiO<sub>3</sub>
49
Citations
19
References
2008
Year
Materials EngineeringOxide HeterostructuresMaterials ScienceDielectric PropertiesEngineeringFerroelectric ApplicationOptical PropertiesOxide ElectronicsEnergy CeramicApplied PhysicsCondensed Matter PhysicsFerroelectric MaterialsMicrowave CeramicDielectric PermittivityIr ReflectivityFunctional MaterialsCrystal Inhomogeneity
The dielectric permittivity (100 Hz–1 MHz) and IR reflectivity of SrTiO3:Mn(0.1 at.%) crystals and SrTiO3:Mn(0.1–3 at.%) ceramics prepared maintaining the ratio (Sr+Mn)/ Ti = 1 or (Ti+Mn)/Sr = 1 (A- and B-type ceramics, respectively) were studied. Surprisingly, the magnitude and ε'(T) dependence for the crystals and B-type ceramics with 0.1 at.% of Mn appeared to be nearly the same; the magnitudes rise on cooling and reach ∼3000 at T = 7 K. At the same time, IR spectra of SrTiO3:Mn(0.1 at.%) crystals reveal that TO (transverse optical) phonons yield a magnitude of low frequency permittivity of ∼4000 at T = 5 K, evidencing crystal inhomogeneity. Both crystals, like B-type SrTiO3:Mn(0.1 at.%) ceramics, reveal faint low temperature relaxations with the Arrhenius activation energies ∼37–40 meV and ∼120–130 meV (P- and T-relaxations). These relaxations emerge in losses only and were tentatively attributed to reorientation of defects associated with MnTi2+–O−-type polaronic centres and Oh1–D4h18 phase transition related effects, respectively. In reduced crystals P-relaxation strongly enhances, becoming distinctly seen in the real part of the permittivity. More heavily Mn doped A- and B-type ceramics reveal strongly pronounced Arrhenius-type dielectric relaxation with activation energy ∼59–68 meV depending on the Mn concentration.
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