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 × 10–6) 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.

Highlights

  • Collisions of atoms and molecules with surfaces typically lead to two experimentally identifiable outcomes: direct inelastic scattering (DIS) and trapping followed by thermal desorption (TD).[1]

  • For the Molecular dynamics (MD) simulations with our effective medium theory (EMT)-potential energy surface (PES), we modeled Xe as a (6 × 6) 6-layered slab with periodic boundary conditions

  • The minimum energy structure represented by the PES corresponds to H atoms adsorbed at an fcc hollow where the H atom is 2.8 Å displaced toward the vacuum from the plane defined by the equilibrium positions of the first layer of Xe atoms

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Summary

Introduction

Collisions of atoms and molecules with surfaces typically lead to two experimentally identifiable outcomes: direct inelastic scattering (DIS) and trapping followed by thermal desorption (TD).[1]. This may involve surface penetration followed by resurfacing.[11,12]

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