Box Connor L, Hertl Nils, Stark Wojciech G, Maurer Reinhard J
Department of Chemistry, University of Warwick, Gibbet Hill Road, CV4 7AL Coventry, U.K.
Department of Physics, University of Warwick, Gibbet Hill Road, CV4 7AL Coventry, U.K.
J Phys Chem Lett. 2024 Dec 26;15(51):12520-12525. doi: 10.1021/acs.jpclett.4c02468. Epub 2024 Dec 13.
In the dynamics of atoms and molecules at metal surfaces, electron-hole pair excitations can play a crucial role. In the case of hyperthermal hydrogen atom scattering, they lead to nonadiabatic energy loss and highly inelastic scattering. Molecular dynamics with electronic friction simulation results, based on an isotropic homogeneous electron gas approximation, have previously aligned well with measured kinetic energy loss distributions, indicating that this level of theoretical description is sufficient to describe nonadiabatic effects during scattering. In this study, we demonstrate that friction derived from density functional theory linear response calculations can also describe the experimental energy loss distributions, although agreement is slightly worse than for the simpler isotropic homogeneous electron gas approximation. We show that the apparent agreement of the homogeneous electron gas approximation with experiment arises from a fortuitous cancellation of errors as friction is overestimated close to the surface and the spin transition is neglected. Differences in frictional treatment affect single, double, and multibounce scattering trajectories in distinct ways, altering the shape of low-temperature energy loss distributions. These distinctions are largely absent at room temperature but may be measurable in future low-temperature scattering experiments.
在金属表面原子和分子的动力学过程中,电子 - 空穴对激发可能起着关键作用。在超热氢原子散射的情况下,它们会导致非绝热能量损失和高度非弹性散射。基于各向同性均匀电子气近似的带有电子摩擦的分子动力学模拟结果,此前与测量得到的动能损失分布吻合得很好,这表明这种理论描述水平足以描述散射过程中的非绝热效应。在本研究中,我们证明从密度泛函理论线性响应计算得出的摩擦也能描述实验能量损失分布,尽管其与实验的吻合度略逊于更简单的各向同性均匀电子气近似。我们表明,均匀电子气近似与实验的明显吻合源于一种偶然的误差抵消,因为在靠近表面处摩擦被高估且自旋跃迁被忽略。摩擦处理方式的差异以不同方式影响单、双和多反弹散射轨迹,改变低温能量损失分布的形状。这些差异在室温下基本不存在,但在未来的低温散射实验中可能是可测量的。