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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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Pasanen, Toni P.
Helsinki Institute of Physics
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (21/21 displayed)
- 2023Surface passivation of Germanium with ALD Al2O3: Impact of Composition and Crystallinity of GeOx Interlayercitations
- 2023Excellent Responsivity and Low Dark Current Obtained with Metal-Assisted Chemical Etched Si Photodiodecitations
- 2023Comparison of SiNx-based Surface Passivation Between Germanium and Siliconcitations
- 2023Plasma-enhanced atomic layer deposited SiO2 enables positive thin film charge and surface recombination velocity of 1.3 cm/s on germaniumcitations
- 2023Quantifying the Impact of Al Deposition Method on Underlying Al2O3/Si Interface Qualitycitations
- 2022Perspectives on Black Silicon in Semiconductor Manufacturing: Experimental Comparison of Plasma Etching, MACE and Fs-Laser Etchingcitations
- 2022Millisecond-Level Minority Carrier Lifetime in Femtosecond Laser-Textured Black Siliconcitations
- 2022(oral talk) Compatibility of Al-neal in processing of Si devices with Al2O3 layer
- 2022Impact of doping and silicon substrate resistivity on the blistering of atomic-layer-deposited aluminium oxidecitations
- 2021Efficient photon capture on germanium surfaces using industrially feasible nanostructure formationcitations
- 2021Al-neal Degrades Al2O3 Passivation of Silicon Surfacecitations
- 2020Modeling Field-effect in Black Silicon and its Impact on Device Performancecitations
- 2020Passivation of Detector-Grade Float Zone Silicon with Atomic Layer Deposited Aluminum Oxidecitations
- 2020Impact of doping and silicon substrate resistivity on the blistering of atomic-layer-deposited aluminium oxidecitations
- 2019Effect of MACE Parameters on Electrical and Optical Properties of ALD Passivated Black Siliconcitations
- 2019Compatibility of 3-D Printed Devices in Cleanroom Environments for Semiconductor Processingcitations
- 2019Compatibility of 3-D Printed Devices in Cleanroom Environments for Semiconductor Processingcitations
- 2019Passivation of Detector‐Grade FZ‐Si with ALD‐Grown Aluminium Oxidecitations
- 2018Economic Advantages of Dry-Etched Black Silicon in Passivated Emitter Rear Cell (PERC) Photovoltaic Manufacturingcitations
- 2018Economic Advantages of Dry-Etched Black Silicon in Passivated Emitter Rear Cell (PERC) Photovoltaic Manufacturingcitations
- 2017Surface passivation of black silicon phosphorus emitters with atomic layer deposited SiO2/Al2O3 stackscitations
Places of action
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article
Quantifying the Impact of Al Deposition Method on Underlying Al2O3/Si Interface Quality
Abstract
Oxide-semiconductor interface quality has often a direct impact on the electrical properties of devices and on their performance. Traditionally, the properties are characterised through metal-oxide-semiconductor (MOS) structures by depositing a metal layer and measuring the capacitance-voltage (C-V) characteristics.However, metal deposition process itself may have an impact on the oxide and the oxide-semiconductor interface. The impact of magnetron sputtering, e-beam evaporation, and thermal evaporation on an Al2O3/Si interface was studied, where<br/>atomic layer deposited (ALD) Al2O3 was used, by MOS C-V and Corona Oxide Characterization of Semiconductors (COCOS) measurements. The latter allows characterisation of the interface also in its original state before metallisation. The results show that sputtering induces significant damage at the underlaying Al2O3/Si interface as the measured interface defect density Dit increases from 1011 cm−2eV to 1013 cm−2eV. Interestingly, sputtering also generates a high density of positive charges Qtot at the interface as the charge changes from –2 · 1012 cm−2 to +7 · 1012 cm−2. Thermal evaporation is found to be a softer method, with modest impact on Dit and Qtot. Finally, we show that Alnealing heals the damage but has also a significant impact on the charge of the film recovering the characteristic negative charge of Al2O3 (∼ –4 · 1012 cm−2).