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Electron-spin-resonance studies of donors in wurtzite GaN
131
Citations
28
References
1993
Year
Wide-bandgap SemiconductorEsr LinesEngineeringMagnetic ResonanceWurtzite Gan FilmsChemistryPhysicsAluminum Gallium NitrideGallium OxideQuantum ChemistrySynchrotron RadiationCategoryiii-v SemiconductorSpintronicsFilm ThicknessNatural SciencesApplied PhysicsCondensed Matter PhysicsGan Power DeviceWurtzite Gan
Electron-spin-resonance (ESR) measurements have been performed on a series of wurtzite GaN films grown on sapphire substrates by low-pressure metal-organic chemical-vapor deposition. The sample set included films grown with both AlN and GaN buffer layers. The ESR signal results from residual donors with ${\mathit{g}}_{\mathrm{\ensuremath{\parallel}}}$=1.9510 and ${\mathit{g}}_{\mathrm{\ensuremath{\perp}}}$=1.9483. The g value and the effective mass can be explained using a five-band k\ensuremath{\cdot}p model. Nuclear hyperfine interactions are observed as a shift in the central resonance position, due to the Overhauser effect from which the density of the wave function at the Ga nucleus is derived. The ESR lines all have quite a sharp Lorentzian shape due to motional narrowing. At low temperatures (T20 K) the linewidth narrows with increasing temperature, consistent with electrons hopping from donor site to donor site. At higher temperatures the line broadens due to electron-phonon interactions. The concentration of uncompensated donors is independent of film thickness for GaN buffered films but increases monotonically with thickness for AlN buffered films, probably due to a decrease in the concentration of compensating centers. Photoluminescence measurements indicate that only the thickest films are homogeneous along the growth direction.
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