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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Global Potentials for the Interaction between Rare Gases and Graphene-Based Surfaces: An Atom-Bond Pairwise Additive Representation
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Global Potentials for the Interaction between Rare Gases and Graphene-Based Surfaces: An Atom-Bond Pairwise Additive Representation

机译:稀有气体与基于石墨烯的表面之间相互作用的全局势能:原子键成对加法表示

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摘要

Global potentials for the physisorption of rare-gas atoms on graphene and graphite, amenable for a variety of dynamics simulations, are reported. An atom-bond pairwise additive form of the potential is used, where the interaction pairs, represented by proper analytical functions, are constituted by the Rg atom (Rg = He, Ne, Ar, Kr) and the C-C bonds of the graphene sheet(s). The parameters of the atom-bond pair potential, derived from the polarizability of the interacting partners, are fine-tuned, exploiting calculations of the prototypical Rg-coronene system using high-level electronic structure methods and large basis sets. The atom-graphene/graphite potential is further expanded in a Fourier series, and it is found that for an accurate representation of the interaction only a small number of corrugation terms need to be added to the laterally averaged potential. Furthermore, this corrugation part of the potential is both identical for Rg-graphene and Rg- graphite; in other words, inner layers of graphite only play a role in the laterally averaged Rg~graphite potential. For all systems, the hollow at the center of the carbon ring is the preferred adsorption site, although diffusion barriers are low. The present results compare well with previous data regarding well depths and equilibrium distances at different adsorption sites and, for graphite, the long-range dispersion coefficient C3. In addition, binding energies (eigenvalues of the laterally averaged potentials) are in a fairly good agreement with experimental determinations, providing further support for the reliability of the potentials.
机译:据报道,适用于各种动力学模拟的稀有气体原子在石墨烯和石墨上的物理吸附潜力很大。使用电位的原子键成对加成形式,其中相互作用对由适当的解析函数表示,由Rg原子(Rg = He,Ne,Ar,Kr)和石墨烯片的CC键构成( s)。通过使用高级电子结构方法和大型基础集计算原型Rg-异戊二烯体系的计算,可以微调源自相互作用对象的极化性的原子键对电势的参数。原子-石墨烯/石墨势以傅立叶级数进一步扩展,并且发现为了精确表示相互作用,仅需要向横向平均势添加少量波纹项。此外,Rg-石墨烯和Rg-石墨的电位的该波纹部分都是相同的。换句话说,石墨的内层仅在横向平均的Rg-石墨势中起作用。对于所有系统,尽管扩散势垒很低,但在碳环中心的空心是首选的吸附位置。目前的结果与以前的数据进行了很好的比较,以前的数据是关于在不同吸附位点的井深和平衡距离,而对于石墨,则是长程分散系数C3。此外,结合能(横向平均电位的特征值)与实验确定值相当吻合,为电位的可靠性提供了进一步的支持。

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