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GaAs metal-oxide-semiconductor push with molecular beam epitaxy Y2O3 - In comparison with atomic layer deposited Al2O3
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GaAs metal-oxide-semiconductor push with molecular beam epitaxy Y2O3 - In comparison with atomic layer deposited Al2O3

H.W. Wan, K.Y. Lin, C.K. Cheng, Y.K. Su, W.C. Lee, C.H. Hsu, T.W. Pi, J. KwoM. Hong
Journal of Crystal Growth
2017

摘要

A1. interfacial trap density (D it ) A3. atomic-layer-deposition (ALD) A3. molecular-beam-epitaxy (MBE) B1. Y2O3 B2. GaAs B3. metal-oxide-semiconductor capacitors (MOSCAPs) Condensed Matter Physics Inorganic Chemistry Materials Chemistry
In-situ molecular beam epitaxy (MBE) Y 2 O 3 films 1-2nm thick were epitaxially grown on GaAs(001)-4×6 reconstructed surfaces. Despite a large lattice mismatch, the hetero-structure exhibits outstanding thermal stability to 900°C with excellent capacitance-voltage (C-V) characteristics. Low interfacial trap densities (D it 's) of (3-5)×10 11 eV -1 cm -2 were obtained using the conductance method (G-V) without discernible peaks at the mid-gap. The frequency dispersion of the measured C-Vs of the Y 2 O 3 /GaAs(001) is ~4.6% for p-GaAs and ~12.4% for n-GaAs. In contrast, the atomic layer deposited Al 2 O 3 on GaAs(001) shows large D it with a peak at the mid-gap, large C-V frequency dispersion, and low thermal stability at temperatures higher than 600°C. Synchrotron radiation photoemission results show intactness of the interfacial structure in the MBE-Y 2 O 3 /GaAs, while removal of the surface As atoms is found in the ALD-Al 2 O 3 /GaAs system.

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