Physical Review B · 2005 · 75 citations · 22 references
Natural SciencesMaterials EngineeringMaterials ScienceMaterials CharacterizationMaterials PhysicsSemiconductor MaterialsElectronic Band StructureElectronic Material CharacterizationX-ray CrystallographyX-ray Data AnalysisX-ray DiffractionX-ray SpectroscopyAtomic Fine StructureBand Structure CalculationExtended X-ray Absorption Fine StructureLocal StructureMolecular Beam EpitaxyX-ray Absorption Near Edge StructureX-ray Absorption SpectroscopyX-ray Spectra
The band structure of the diluted magnetic semiconductor (Ga,Mn)N, and the x-ray absorption near-edge structure (XANES) at the K edge of Mn, were calculated using the linearized augmented plane wave method. The calculated K-edge spectra fit well with experimental data obtained on samples of ${\mathrm{Ga}}_{1\ensuremath{-}x}{\mathrm{Mn}}_{x}\mathrm{N}$ with a wide range of Mn content, from $x=0.3%$ to 5.7%. These samples were grown by molecular beam epitaxy. X-ray diffraction measurements and extended x-ray absorption fine structure studies were used to confirm the wurtzite structure of the samples, the absence of any secondary phase, and the substitutional position of Mn in the gallium sublattice of GaN. The shape of the measured XANES spectra does not depend on the Mn content, implying the same valence state and local atomic structure around the Mn atom in all samples. The comparison between the measured spectra and the results of the ab initio calculation offers a clear interpretation of the preedge structure: It is mainly due to dipolar transitions, with a single peak in the case of ${\mathrm{Mn}}^{2+}$ and an additional peak for ${\mathrm{Mn}}^{3+}$. Such a behavior of the XANES preedge of ${\mathrm{Mn}}^{2+}$ was confirmed experimentally on (Ga,Mn)As and (Zn,Mn)Te. We conclude that the valence state of Mn in wurtzite (Ga,Mn)N is $3+$, a conclusion which is also supported by infrared optical transmission and magnetization data obtained on the same samples.
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