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Charge-optimized many-body interaction potential for AlN revisited to explore plasma–surface interactions
Plasma–surface interactions during AlN thin film sputter deposition could be studied by means of reactive molecular dynamics (RMD) methods. This requires an interaction potential that describes all species as well as wall interactions (e.g., particle emission, damage formation) appropriately. Howeve...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10066324/ https://www.ncbi.nlm.nih.gov/pubmed/37002255 http://dx.doi.org/10.1038/s41598-023-31862-8 |
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author | Gergs, Tobias Mussenbrock, Thomas Trieschmann, Jan |
author_facet | Gergs, Tobias Mussenbrock, Thomas Trieschmann, Jan |
author_sort | Gergs, Tobias |
collection | PubMed |
description | Plasma–surface interactions during AlN thin film sputter deposition could be studied by means of reactive molecular dynamics (RMD) methods. This requires an interaction potential that describes all species as well as wall interactions (e.g., particle emission, damage formation) appropriately. However, previous works focused on the establishment of AlN bulk potentials. Although for the third-generation charge-optimized many-body (COMB3) potential at least a single reference surface was taken into account, surface interactions are subject to limited reliability only. The demand for a revised COMB3 AlN potential is met in two steps: First, the Ziegler–Biersack–Littmark potential is tapered and the variable charge model QTE[Formula: see text] is implemented to account for high-energy collisions and distant charge transport, respectively. Second, the underlying parameterization is reworked by applying a self-adaptive evolution strategy implemented in the GARFfield software. Four wurtzite, three zinc blende and three rock salt surfaces are considered. An example study on the ion bombardment induced particle emission and point defect formation reveals that the revised COMB3 AlN potential is appropriate for the accurate investigation of plasma–surface interactions by means of RMD simulations. |
format | Online Article Text |
id | pubmed-10066324 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-100663242023-04-02 Charge-optimized many-body interaction potential for AlN revisited to explore plasma–surface interactions Gergs, Tobias Mussenbrock, Thomas Trieschmann, Jan Sci Rep Article Plasma–surface interactions during AlN thin film sputter deposition could be studied by means of reactive molecular dynamics (RMD) methods. This requires an interaction potential that describes all species as well as wall interactions (e.g., particle emission, damage formation) appropriately. However, previous works focused on the establishment of AlN bulk potentials. Although for the third-generation charge-optimized many-body (COMB3) potential at least a single reference surface was taken into account, surface interactions are subject to limited reliability only. The demand for a revised COMB3 AlN potential is met in two steps: First, the Ziegler–Biersack–Littmark potential is tapered and the variable charge model QTE[Formula: see text] is implemented to account for high-energy collisions and distant charge transport, respectively. Second, the underlying parameterization is reworked by applying a self-adaptive evolution strategy implemented in the GARFfield software. Four wurtzite, three zinc blende and three rock salt surfaces are considered. An example study on the ion bombardment induced particle emission and point defect formation reveals that the revised COMB3 AlN potential is appropriate for the accurate investigation of plasma–surface interactions by means of RMD simulations. Nature Publishing Group UK 2023-03-31 /pmc/articles/PMC10066324/ /pubmed/37002255 http://dx.doi.org/10.1038/s41598-023-31862-8 Text en © The Author(s) 2023 https://creativecommons.org/licenses/by/4.0/Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Article Gergs, Tobias Mussenbrock, Thomas Trieschmann, Jan Charge-optimized many-body interaction potential for AlN revisited to explore plasma–surface interactions |
title | Charge-optimized many-body interaction potential for AlN revisited to explore plasma–surface interactions |
title_full | Charge-optimized many-body interaction potential for AlN revisited to explore plasma–surface interactions |
title_fullStr | Charge-optimized many-body interaction potential for AlN revisited to explore plasma–surface interactions |
title_full_unstemmed | Charge-optimized many-body interaction potential for AlN revisited to explore plasma–surface interactions |
title_short | Charge-optimized many-body interaction potential for AlN revisited to explore plasma–surface interactions |
title_sort | charge-optimized many-body interaction potential for aln revisited to explore plasma–surface interactions |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10066324/ https://www.ncbi.nlm.nih.gov/pubmed/37002255 http://dx.doi.org/10.1038/s41598-023-31862-8 |
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