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氦介导沉积:He-TiO2(110)-(1×1)相互作用势的建模及基于密度泛函计算的氦液滴碰撞的应用。

Helium mediated deposition: modeling the He-TiO2(110)-(1×1) interaction potential and application to the collision of a helium droplet from density functional calculations.

机构信息

Instituto de Física Fundamental (C.S.I.C.), Serrano 123, E-28006 Madrid, Spain.

出版信息

J Chem Phys. 2012 Mar 28;136(12):124703. doi: 10.1063/1.3698173.

DOI:10.1063/1.3698173
PMID:22462884
Abstract

This paper is the first of a two-part series dealing with quantum-mechanical (density-functional-based) studies of helium-mediated deposition of catalytic species on the rutile TiO(2)(110)-(1×1) surface. The interaction of helium with the TiO(2)(110)-(1×1) surface is first evaluated using the Perdew-Burke-Ernzerhof functional at a numerical grid dense enough to build an analytical three-dimensional potential energy surface. Three (two prototype) potential models for the He-surface interaction in helium scattering calculations are analyzed to build the analytical potential energy surface: (1) the hard-corrugated-wall potential model; (2) the corrugated-Morse potential model; and (3) the three-dimensional Morse potential model. Different model potentials are then used to study the dynamics upon collision of a (4)He(300) cluster with the TiO(2)(110) surface at zero temperature within the framework of a time-dependent density-functional approach for the quantum fluid [D. Mateo, D. Jin, M. Barranco, and M. Pi, J. Chem. Phys. 134, 044507 (2011)] and classical dynamics calculations. The laterally averaged density functional theory-based potential with an added long-range dispersion interaction term is further applied. At variance with classical dynamics calculations, showing helium droplet splashing out of the surface at impact, the time evolution of the macroscopic helium wave-function predicts that the helium droplet spreads on the rutile surface and leads to the formation of a thin film above the substrate. This work thus provides a basis for simulating helium mediated deposition of metallic clusters embedded within helium nanodroplets.

摘要

本文是一个由两部分组成的系列的第一篇,主要研究氦介导的催化物种在金红石 TiO(2)(110)-(1×1)表面上沉积的量子力学(基于密度泛函)。首先使用 Perdew-Burke-Ernzerhof 泛函评估氦与 TiO(2)(110)-(1×1)表面的相互作用,数值网格足够密集,可构建分析三维势能面。为了构建分析势能面,分析了氦散射计算中用于氦表面相互作用的三种(两种原型)势能模型:(1)硬波纹壁势能模型;(2)波纹莫尔斯势能模型;(3)三维莫尔斯势能模型。然后使用不同的模型势来研究在零温度下,(4)He(300)团簇与 TiO(2)(110)表面碰撞时的动力学,这是在量子流体[D. Mateo、D. Jin、M. Barranco 和 M. Pi,J. Chem. Phys. 134, 044507(2011)]的时变密度泛函方法和经典动力学计算的框架内进行的。进一步应用了具有附加长程色散相互作用项的横向平均密度泛函理论基势。与经典动力学计算不同,经典动力学计算显示氦液滴在冲击时溅出表面,宏观氦波函数的时间演化表明氦液滴在金红石表面上扩展,并导致在衬底上方形成薄膜。这项工作为模拟嵌入氦纳米液滴中的金属团簇的氦介导沉积提供了基础。

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