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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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Derluyn, Joff
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Topics
Publications (9/9 displayed)
- 2021AlGaN channel high electron mobility transistors with regrown ohmic contactscitations
- 2020Remarkable Breakdown Voltage on AlN/AlGaN/AlN double heterostructurecitations
- 2019Buffer breakdown in GaN-on-Si HEMTs: a comprehensive study based on a sequential growth experimentcitations
- 20141900 V, 1.6 mΩ cm2 AlN/GaN-on-Si power devices realized by local substrate removalcitations
- 2010Very low sheet resistance AlInN/GaN HEMT grown on 100 mm Si(111) by MOVPEcitations
- 2008AlGaN photodetectors for applications in the extreme ultraviolet (EUV) wavelength rangecitations
- 2006Mechanism for Ohmic contact formation on Si3N4 passivated AlGaN∕GaN high-electron-mobility transistorscitations
- 2005The role of Al on Ohmic contact formation on n-type GaN and AlGaN∕GaNcitations
- 2005Improvement of AlGaN∕GaN high electron mobility transistor structures by in situ deposition of a Si3N4 surface layercitations
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article
Buffer breakdown in GaN-on-Si HEMTs: a comprehensive study based on a sequential growth experiment
Abstract
The aim of this work is to investigate the breakdown mechanisms of the layers constituting the vertical buffer of GaN-on-Si HEMTs; in addition, for the first time we demonstrate that the breakdown field of the AlN nucleation layer grown on a silicon substrate is equal to 3.2 MV/cm and evaluate its temperature dependence. To this aim, three samples, obtained by stopping the epitaxial growth of a GaN on Silicon stack at different steps, are studied and compared: Si/AlN, Si/AlN/AlGaN, full vertical stack up to the Carbon doped buffer layer. The current-voltage (IV) characterizations performed at both room temperature and high temperature show that: (i) the defectiveness of the AlN nucleation layer is the root cause of the leakage through an AlN/Silicon junction, and causes the vertical I-V characteristics to have a high device-to-device variability; (ii) the first AlGaN layer grown over the AlN, beside improving the breakdown voltage of the whole structure, causes the leakage current to be more stable and uniform across the sample area; (iii) a thick strain-relief stack and a carbon-doped GaN buffer enhance the breakdown voltage up to more than 750V at 170°C, and guarantee a remarkably low deviceto-device variability. Furthermore, a set of constant voltage stress on the Si/AlN sample demonstrate that the aluminum nitride layer shows a time dependent breakdown, with Weibull-distributed failures and a shape factor greater than 1, in line with the percolation model.