Chemistry of Materials · 2004 · 437 citations · 26 references
Natural SciencesMaterials SciencePhysicsCrystal StructureMaterials CharacterizationOptical MaterialsCrystal ChemistryElectron DiffractionInorganic SpectroscopyOptical Properties Of SolidsPerovskite MaterialsCubic Crystal LatticesOptical Absorption SpectraOptical Band GapPerovskite Crystal StructurePerovskite DielectricsPowder DiffractionPowder Diffraction AnalysisPowder X-ray Diffraction
The syntheses, crystal structures, electrical properties, and optical absorbance spectra of six perovskite oxynitrides, AMO 2 N (A = Ba, Sr, Ca; M = Ta, Nb) have been investigated. The average crystal structure of BaTaO 2 N is a cubic perovskite, with a Ta−O/N distance of 2.056 Å. SrTaO 2 N and CaTaO 2 N are distorted by octahedral tilting, showing noticeably smaller Ta−O/N distances of approximately 2.02 Å. Electron diffraction studies of BaTaO 2 N are consistent with the simple cubic perovskite crystal structure determined using X-ray powder diffraction methods. Each of the niobium oxynitrides is isostructural with its tantalum analogue, though the Nb−O/N distances are observed to be slightly longer. The optical band gaps are estimated from diffuse reflectance spectra as follows: BaTaO 2 N, 1.8 eV; SrTaO 2 N, 2.1 eV; CaTaO 2 N, 2.4 eV; BaNbO 2 N, 1.8 eV; SrNbO 2 N, 1.9 eV; CaNbO 2 N, 2.1 eV. Impedance spectroscopy was carried out on sintered pellets of the ATaO 2 N and BaNbO 2 N to investigate the dielectric and electrical transport properties. The BaNbO 2 N sample shows metallic-type conductivity apparently from a slight reduction that occurs during sintering. In contrast, the tantalum compounds are semiconductors/insulators with conductivities of ∼10 - 5 S/cm (A = Ba, Sr) and ∼10 - 8 S/cm (A = Ca). Interpretation of the impedance data for BaTaO 2 N and SrTaO 2 N reveals that these two compounds have unexpectedly high bulk dielectric constants, κ ≈ 4900 and 2900, respectively, at room temperature. The dielectric constants of both compounds are frequency dependent and show a relatively weak linear dependence upon temperature with no sign of a phase transition over the temperature range 300−180 K.
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