AVS 64th International Symposium & Exhibition | |
Plasma Science and Technology Division | Friday Sessions |
Session PS+NS+SS+TF-FrM |
Session: | Atomic Layer Etching II |
Presenter: | Chad Huard, University of Michigan |
Authors: | C.M. Huard, University of Michigan Y. Zhang, Lam Research Corporation S. Sriraman, Lam Research Corporation A. Paterson, Lam Research Corporation M.J. Kushner, University of Michigan |
Correspondent: | Click to Email |
Atomic layer etching (ALE) typically separates the etch process into (at least) two self-limited steps, repeated cyclically – a passivation and an etch step. To obtain all of the benefits of ALE, each of the steps should be fully self-limited, and produce no continuous etching during either step. Only by the synergy between the two steps being repeated cyclically is atomic etching achieved. ALE etching mechanisms have been demonstrated for several materials (e.g., Si, Ge) that do not involve thick passivation layers. ALE-like etching has also been demonstrated for SiO2 and Si3N4, however with the etching mechanisms for these materials relying on the non-self-limited deposition of a polymer layer, it is more difficult to obtain the full benefits of ALE in these systems.
To investigate the benefits and limitations of using an ALE-like pulsing scheme for etching SiO2, a representation of the through-polymer etching mechanism of SiO2 in Ar/C4F8/O2 plasmas was developed and implemented into the 3-dimensional Monte Carlo Feature Profile Model (MCFPM). The model includes diffusion of radical atomic species (F and O) through the polymer capping layer and ion-energy activated reactions at the SiO2/polymer interface stimulated by ions implanting through the polymer capping layer. These processes allow for the simulation of SiO2 (and Si) etching through a finite thickness of polymer. The model reproduces systematic trends for selectivity and etch rates as a function of polymer thickness observed for continuous etching.
Results from the model suggest that the non-self-limited nature of the polymer deposition step can limit the benefits of applying ALE techniques to SiO2, particularly in 3D features. The balance of polymer deposition by radical CFx species and erosion by F radicals is subject to neutral transport issues and so are more sensitive to geometry and aspect ratio than for fully self-limited passivation, as occurs in ALE of Si using, for example, Cl2 containing gases. The reactive sticking coefficients of CFx radicals on the polymer surface depends, in part, on ion generated dangling bonds which can result in a non-uniform polymer thickness in 3D features. The etch depth per cycle (EPC) was found to depend on polymer thickness, introducing non-uniformity and aspect ratio dependent etch rates in 3D features during ALE. Methods for mitigating the dependence of EPC on polymer thickness using carefully controlled ion energies and the introduction of O2 will be discussed.
Work was supported by Lam Research Corp., DOE Office of Fusion Energy Science and the National Science Foundation.