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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Pedersen, Kjeld
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Topics
Publications (10/10 displayed)
- 2023Magnetron Sputter Grown AlN Nanostructures with Giant Piezoelectric Response toward Energy Generationcitations
- 2023Magnetron Sputter Deposition of Nanostructured AlN Thin Filmscitations
- 2019Structure and properties of Ta/Al/Ta and Ti/Al/Ti/Au multilayer metal stacks formed as ohmic contacts on n-GaNcitations
- 2018Ultra-thin titanium nitride films for refractory spectral selectivity [Invited]citations
- 2018Ultra-thin titanium nitride films for refractory spectral selectivitycitations
- 2018Optical characterization of SiC films grown on Si(111)
- 2018Optical characterization of SiC films grown on Si(111)
- 2017Growth of aluminum oxide on silicon carbide with an atomically sharp interfacecitations
- 2016Atomically controlled, self-limiting procedures for growth of aluminum oxide on SiC-on-Si
- 2015Electric field mapping inside metallized film capacitorscitations
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article
Growth of aluminum oxide on silicon carbide with an atomically sharp interface
Abstract
The development of SiC wafers with properties suitable for electronic device fabrication is now well established commercially. A critical issue for developing metal-oxide-semiconductor field effect transistor devices of SiC is the choice of dielectric materials for surface passivation and insulating coatings. Although SiO 2 grown thermally on SiC is a possibility for the gate dielectric, this system has a number of problems related to the higher band gap of SiC, which energetically favors more interface states than for SiO 2 on Si, and the low dielectric constant of SiO 2 leading to 2.5× higher electric fields across the oxide than in the surface of SiC, and to a premature breakdown at the higher fields and higher temperatures that SiC devices are designed to operate under. As a replacement for SiO 2 , amorphous Al 2 O 3 thin film coatings have some strong advocates, both for n- and p-type SiC, due to the value of its band gap and the position of its band edges with respect to the band edges of the underlying semiconductor, a number of other material properties, and not the least due to the advances of the atomic-layer-deposition process. Exploring the fact that the chemical bonding of Al 2 O 3 is the strongest among the oxides and therefore stronger than in SiO 2 , the authors have previously shown how to form an Al 2 O 3 film on Si (111) and Si (100), by simply depositing a few atomic layers of Al on top of an ultrathin (0.8 nm) SiO 2 film previously grown on Si surfaces [Si (111) and Si (100)] and heating this system up to around 600 °C (all in ultrahigh vacuum). This converts all the SiO 2 into a uniform layer of Al 2 O 3 with an atomically sharp interface between the Al 2 O 3 and the Si surface. In the present work, the same procedures are applied to form Al 2 O 3 on a SiC film grown on top of Si (111). The results indicate that a similar process, resulting in a uniform layer of 1-2 nm of Al 2 O 3 with an atomically sharp Al 2 O 3 /SiC interface, also works in this case.