Bottomless Barrier Strategy for Next-Generation Cu Interconnects Using Phenylethyl Mercaptan-Assisted Area-Selective ALD for Scalable Ru/ZnO Bilayer Integration

材料科学 堆积 原子层沉积 双层 单层 图层(电子) 化学工程 纳米技术 化学吸附 半导体 沉积(地质) 烷基 阻挡层 光电子学 异质结 化学气相沉积 聚合物 选择性 粘附 薄膜 纳米电子学 含氟聚合物 复合材料 透射电子显微镜
作者
Minwoo Kim,Debananda Mohapatra,Sang Bok Kim,Yeseul Son,Jeongha Kim,Soo‐Hyun Kim
出处
期刊:ACS Applied Materials & Interfaces [American Chemical Society]
卷期号:18 (31): 43494-43503
标识
DOI:10.1021/acsami.6c12802
摘要

Self-assembled monolayers (SAMs) consist of long alkyl chains of large molecular size and low volatility, which require conventional solution-based processes that are incompatible with bottomless barrier structures, especially for sub-10 nm 3D semiconductor fabrication, leading to nonuniform inhibition and poor selectivity. Here, we introduce a bottomless barrier architecture strategy that selectively deposits barrier material on the SiO2 via-sidewall surfaces using area-selective atomic layer deposition (AS-ALD), while leaving the Cu bottom surface exposed. A phenylethyl mercaptan (PEM) small-molecule inhibitor (SMI) is employed as a Cu-selective passivating agent, exploiting strong Cu-S chemisorption and π-π stacking interactions to form a densely packed inhibition layer on Cu surfaces, thereby directing ZnO ALD exclusively onto the SiO2 sidewalls with superior selectivity compared to bulkier SAM-based approaches. ZnO is decided as the barrier material due to its low-temperature ALD capability (<150 °C), strong interfacial adhesion with Si-based dielectric, and effective suppression of Cu diffusion. The PEM inhibitor exhibited sufficient vapor pressure for a stable vapor-phase ALD-ZnO process that selectively adsorbs approximately 90% during a 50-cycle ZnO film with a thickness of about 9.1 nm. Notably, both H2 molecular and H2 plasma treatments are found to be efficient in removing PEM inhibitor from Cu surfaces before Ru deposition. ALD-Ru is subsequently deposited controllably as a low-resistivity (∼23 μΩ·cm) liner and seed layer with a thickness of ∼15 nm, further maintaining a low resistivity of ∼38.1 μΩ·cm even at a thickness of ∼6 nm, as well as nearly 100% step coverage in dual-trench structures with an aspect ratio of ∼6.3. The resulting Ru/ZnO bilayer on SiO2 sidewalls and the Ru layer on the Cu bottom surface could be incorporated into dual-damascene patterns prior to Cu filling for modern-day interconnects.

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