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氢原子与范德华固体碰撞中的多次反弹和次表面散射

Multibounce and Subsurface Scattering of H Atoms Colliding with a van der Waals Solid.

作者信息

Hertl Nils, Kandratsenka Alexander, Bünermann Oliver, Wodtke Alec M

机构信息

Institut für physikalische Chemie, Universität Göttingen, Tammannstrasse 6, 37077 Göttingen, Germany.

Department of Dynamics at Surfaces, Max-Planck Institute for Biophysical Chemistry, am Faßberg 11, 37077 Göttingen, Germany.

出版信息

J Phys Chem A. 2021 Jul 8;125(26):5745-5752. doi: 10.1021/acs.jpca.1c03433. Epub 2021 Jun 28.

DOI:10.1021/acs.jpca.1c03433
PMID:34181858
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8279644/
Abstract

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) 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.

摘要

我们报告了2.76电子伏特的氢原子在固态氙表面碰撞的非弹性微分散射实验结果以及全维分子动力学轨迹模拟结果。相互作用势基于对密度泛函理论(DFT)能量进行拟合的有效介质理论(EMT)。实验和理论得出的平动能损失分布高度吻合。通过分析轨迹,我们发现只有少数散射是由简单的单次反弹动力学导致的。大部分散射来自多次反弹碰撞,包括次表面散射,即氢原子穿透到第一层氙原子以下,随后重新回到气相。这种行为导致可观测到的能量损失高达0.5电子伏特,远大于二元碰撞模型的预测值(0.082电子伏特),二元碰撞模型常用于估计直接非弹性表面散射中可能的最高能量损失。如果我们采用基于 Lennard-Jones(LJ)对相互作用的全维势能面(PES),用EMT-PES计算出的 sticking 概率(0.15)会大幅降低(5×10)。尽管LJ-PES能准确描述氢-氙和氙-氙能量最小值附近的相互作用,但在入射能量高于约0.1电子伏特时,它会大幅高估碰撞氢原子所看到的氙原子的有效尺寸。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/2eca8ca75401/jp1c03433_0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/40af13235558/jp1c03433_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/e33b85424ae5/jp1c03433_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/367fa3c972ce/jp1c03433_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/333c1d34bf71/jp1c03433_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/d65640bd9f3c/jp1c03433_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/2eca8ca75401/jp1c03433_0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/40af13235558/jp1c03433_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/e33b85424ae5/jp1c03433_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/367fa3c972ce/jp1c03433_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/333c1d34bf71/jp1c03433_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/d65640bd9f3c/jp1c03433_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/259a/8279644/2eca8ca75401/jp1c03433_0007.jpg

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Following the microscopic pathway to adsorption through chemisorption and physisorption wells.沿着微观吸附途径,通过化学吸附和物理吸附势阱。
氢原子从W(110)表面的散射:含电子摩擦的分子动力学的一个基准。
Phys Chem Chem Phys. 2022 Sep 14;24(35):20813-20819. doi: 10.1039/d2cp01850k.
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Effective medium theory for bcc metals: electronically non-adiabatic H atom scattering in full dimensions.体心立方金属的有效介质理论:全维度电子非绝热氢原子散射
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