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Naji, M. |
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Motta, Antonella |
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Mohamed, Tarek |
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Ertürk, Emre |
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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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Azam, Siraj |
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Ospanova, Alyiya |
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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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Bol, Ageeth
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Publications (7/7 displayed)
- 2024Nb Doping and Alloying of 2D WS2 by Atomic Layer Deposition for 2D Transition Metal Dichalcogenide Transistors and HER Electrocatalystscitations
- 2023Toolbox of Advanced Atomic Layer Deposition Processes for Tailoring Large-Area MoS2 Thin Films at 150 °Ccitations
- 2023MoS2 Synthesized by Atomic Layer Deposition as Cu Diffusion Barriercitations
- 2022Growth Mechanism and Film Properties of Atomic-Layer-Deposited Titanium Oxysulfidecitations
- 2022Atomic Layer Deposition of Large-Area Polycrystalline Transition Metal Dichalcogenides from 100 °C through Control of Plasma Chemistrycitations
- 2022Controlling transition metal atomic ordering in two-dimensional Mo1- xW xS2alloyscitations
- 2022Effects of the Structure and Temperature on the Nature of Excitons in the Mo0.6W0.4S2Alloycitations
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article
MoS2 Synthesized by Atomic Layer Deposition as Cu Diffusion Barrier
Abstract
Miniaturization in integrated circuits requires that the Cu diffusion barriers located in interconnects between the Cu metal line and the dielectric material should scale down. Replacing the conventional TaN with a 2D transition metal dichalcogenide barrier potentially offers the opportunity to scale to 1–2 nm thick barriers. In this article, it is demonstrated that MoS2 synthesized by atomic layer deposition (ALD) can be employed as a Cu diffusion barrier. ALD offers a controlled growth process at back-end-of-line (BEOL) compatible temperatures. MoS2 films of different thicknesses (i.e., 2.2, 4.3, and 6.5 nm) are tested by time-dependent dielectric breakdown (TDDB) measurements, demonstrating that ALD-grown MoS2 can enhance dielectric lifetime by a factor up to 17 at an electric field of 7 MV cm−1. Extrapolation to lower E-fields shows that the MoS2 barriers prepared by ALD have at least an order of magnitude higher median-time-to-failure during device operation at 0.5 MV cm−1 compared with MoS2 barriers prepared by other methods. By scaling the thickness further down in future work, the ALD MoS2 films can be applied as ultrathin Cu diffusion barriers.