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Multibounce and Subsurface Scattering of H Atoms Colliding with a van der Waals Solid
[Image: see text] We report the results of inelastic differential scattering experiments and full-dimensional molecular dynamics trajectory simulations for 2.76 eV H atoms colliding at a surface of solid xenon. The interaction potential is based on an effective medium theory (EMT) fit to density fun...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical
Society
2021
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8279644/ https://www.ncbi.nlm.nih.gov/pubmed/34181858 http://dx.doi.org/10.1021/acs.jpca.1c03433 |
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author | Hertl, Nils Kandratsenka, Alexander Bünermann, Oliver Wodtke, Alec M. |
author_facet | Hertl, Nils Kandratsenka, Alexander Bünermann, Oliver Wodtke, Alec M. |
author_sort | Hertl, Nils |
collection | PubMed |
description | [Image: see text] We report the results of inelastic differential scattering experiments and full-dimensional molecular dynamics trajectory simulations for 2.76 eV H atoms colliding at a surface of solid xenon. The interaction potential is based on an effective medium theory (EMT) fit to density functional theory (DFT) energies. The translational energy-loss distributions derived from experiment and theory are in excellent agreement. By analyzing trajectories, we find that only a minority of the scattering results from simple single-bounce dynamics. The majority comes from multibounce collisions including subsurface scattering where the H atoms penetrate below the first layer of Xe atoms and subsequently re-emerge to the gas phase. This behavior leads to observable energy-losses as large as 0.5 eV, much larger than a prediction of the binary collision model (0.082 eV), which is often used to estimate the highest possible energy-loss in direct inelastic surface scattering. The sticking probability computed with the EMT-PES (0.15) is dramatically reduced (5 × 10(–6)) if we employ a full-dimensional potential energy surface (PES) based on Lennard-Jones (LJ) pairwise interactions. Although the LJ-PES accurately describes the interactions near the H–Xe and Xe–Xe energy minima, it drastically overestimates the effective size of the Xe atom seen by the colliding H atom at incidence energies above about 0.1 eV. |
format | Online Article Text |
id | pubmed-8279644 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | American Chemical
Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-82796442021-07-15 Multibounce and Subsurface Scattering of H Atoms Colliding with a van der Waals Solid Hertl, Nils Kandratsenka, Alexander Bünermann, Oliver Wodtke, Alec M. J Phys Chem A [Image: see text] We report the results of inelastic differential scattering experiments and full-dimensional molecular dynamics trajectory simulations for 2.76 eV H atoms colliding at a surface of solid xenon. The interaction potential is based on an effective medium theory (EMT) fit to density functional theory (DFT) energies. The translational energy-loss distributions derived from experiment and theory are in excellent agreement. By analyzing trajectories, we find that only a minority of the scattering results from simple single-bounce dynamics. The majority comes from multibounce collisions including subsurface scattering where the H atoms penetrate below the first layer of Xe atoms and subsequently re-emerge to the gas phase. This behavior leads to observable energy-losses as large as 0.5 eV, much larger than a prediction of the binary collision model (0.082 eV), which is often used to estimate the highest possible energy-loss in direct inelastic surface scattering. The sticking probability computed with the EMT-PES (0.15) is dramatically reduced (5 × 10(–6)) if we employ a full-dimensional potential energy surface (PES) based on Lennard-Jones (LJ) pairwise interactions. Although the LJ-PES accurately describes the interactions near the H–Xe and Xe–Xe energy minima, it drastically overestimates the effective size of the Xe atom seen by the colliding H atom at incidence energies above about 0.1 eV. American Chemical Society 2021-06-28 2021-07-08 /pmc/articles/PMC8279644/ /pubmed/34181858 http://dx.doi.org/10.1021/acs.jpca.1c03433 Text en © 2021 The Authors. Published by American Chemical Society Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Hertl, Nils Kandratsenka, Alexander Bünermann, Oliver Wodtke, Alec M. Multibounce and Subsurface Scattering of H Atoms Colliding with a van der Waals Solid |
title | Multibounce and Subsurface Scattering of H Atoms Colliding
with a van der Waals Solid |
title_full | Multibounce and Subsurface Scattering of H Atoms Colliding
with a van der Waals Solid |
title_fullStr | Multibounce and Subsurface Scattering of H Atoms Colliding
with a van der Waals Solid |
title_full_unstemmed | Multibounce and Subsurface Scattering of H Atoms Colliding
with a van der Waals Solid |
title_short | Multibounce and Subsurface Scattering of H Atoms Colliding
with a van der Waals Solid |
title_sort | multibounce and subsurface scattering of h atoms colliding
with a van der waals solid |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8279644/ https://www.ncbi.nlm.nih.gov/pubmed/34181858 http://dx.doi.org/10.1021/acs.jpca.1c03433 |
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