AVS 66th International Symposium & Exhibition | |
2D Materials | Monday Sessions |
Session 2D+AP+EM+MI+NS+PS+TF-MoA |
Session: | 2D Materials Growth and Fabrication |
Presenter: | James Engstrom, Cornell University |
Authors: | T. Suh, Cornell University R. Yalisove, Cornell University J.R. Engstrom, Cornell University |
Correspondent: | Click to Email |
The atomic layer deposition (ALD) of many metals, particularly Group VIII (now known as Groups 8, 9 and 10), on SiO2 has been an active area of research in many fields, which include microelectronics and heterogeneous catalysis. There have been many fewer studies of the inverse—the deposition of SiO2 on many of these same metals. One possible reason to explore the ALD growth of SiO2 on transition metals is that it might provide a route to an atomically thick SiO2 dielectric, silicatene. Silicatene is a 2D material that consists of a bilayer of Si2O3 linked to each other by bridging oxygen atoms (giving SiO2), where there are no dangling bonds or covalent bonds to the underlying substrate on which it is grown. For example, an established route to form silicatene involves deposition of elemental Si in UHV and subsequent high-temperature annealing on various single-crystalline metal surfaces including, but not limited to, Ru(0001), Pt(111), and Pd(100). Such a process, unfortunately, is likely not compatible with high-volume manufacturing. With this motivation we embarked on a study of the plasma-assisted ALD of SiO2 on e-beam deposited polycrystalline thin films of Ru, Pt and Pd using a commercial ALD reactor. We analyzed both the thin films and the starting substrates using a combination of techniques including contact angle, spectroscopic ellipsometry (SE) and X-ray photoelectron spectroscopy. Thin films of SiO2 were deposited using tris(dimethylamido)silane and an oxygen plasma at a substrate temperature of 200 °C, and we examined growth for 5, 10, 20, 50 and 100 cycles. Contact angle measurements showed immediate evidence for SiO2 deposition on all metal surfaces, and the contact angle decreased and remained constant and < 10° from 5 to 100 cycles of ALD. From SE we found little evidence of an incubation period, and growth was linear for the range of sample examined and the thickness deposited per cycle was remarkably constant at a value of 0.76-0.78 Å-cycle-1. Analysis of these films using angle-resolved XPS was consistent with the formation of a thin film of SiO2 with uniform thickness. Having characterized the thin film thickness-ALD cycle relationship we subjected SiO2 thin films with thickness of ~ 7-15 Å to post-deposition high-temperature anneals in oxygen furnace. Initial attempts to form silicatene with an anneal at 800 °C, produced a structure suggesting possible interfacial reaction between the SiO2 and Ru, perhaps involving silicide formation. We will end our presentation with a discussion of recent work involving a more extensive examination of the post-deposition annealing step, and deposition on patterned wafers.