4.6 Article

Why are physical sputtering yields similar for incident ions with different masses?-physical sputtering yields of the Lennard-Jones system

Journal

JOURNAL OF PHYSICS D-APPLIED PHYSICS
Volume 55, Issue 22, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/1361-6463/ac57dc

Keywords

Lennard-Jones; molecular dynamics; physical sputtering

Funding

  1. Japan Society of Promotion of Science (JSPS) [15H05736, 21H04453]
  2. JSPS [JPJSCCA2019002]
  3. Osaka University
  4. Grants-in-Aid for Scientific Research [21H04453] Funding Source: KAKEN

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In the plasma etching of nano-meter-scale complex structures, understanding the etching mechanisms is crucial. By using molecular dynamics simulation, the sputtering yield of a system with interacting atoms was evaluated. The results showed that the sputtering yield only depends on the mass ratio and the interaction range parameter for specific incident ion energy. Furthermore, it was found that the physical sputtering yield weakly depends on the mass ratio in the limited parameter range of real materials used in plasma etching.
Plasma etching of nano-meter-scale complex structures for semiconductor device manufacturing requires a deeper understanding of etching mechanisms. For example, it is known experimentally that the sputtering yield of a material tends to have weak dependence on the mass of incident ions except for extremely light ions such as helium. To understand this property, the sputtering yield of a system of atoms interacting with Lennard-Jones (LJ) potentials was evaluated with molecular dynamics simulation. As the simplest possible case involving two atomic species, a single-element face-centered-cubit (fcc) LJ solid surface interacting with purely repulsive atoms was examined, which emulates a solid surface sputtered by noble-gas ions. The sputtering of such a system at specific incident ion energy depends only on two parameters, i.e. the mass ratio and a parameter representing the relative interaction range between the surface atom and the incident ion. For real materials of our concern used in plasma etching, the range of these two parameters was found to be relatively limited. It was also found that the physical sputtering yield of the LJ system weakly depends on the mass ratio in this relatively narrow parameter range. Because the simple model predicts the weak yield dependence on the incident ion mass, it is considered as a generic property of physical sputtering, independent of the detailed atomic interactions of the surface material and incident ion species.

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