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独立石墨烯的热膨胀:半经验势的基准测试

Thermal expansion of free-standing graphene: benchmarking semi-empirical potentials.

作者信息

Magnin Y, Förster G D, Rabilloud F, Calvo F, Zappelli A, Bichara C

机构信息

Institut Lumière Matière, UMR 5306 Université Claude Bernard Lyon 1-CNRS, Université de Lyon, 10 Rue Ada Byron, F69622 Villeurbanne Cedex, France.

出版信息

J Phys Condens Matter. 2014 May 7;26(18):185401. doi: 10.1088/0953-8984/26/18/185401. Epub 2014 Apr 23.

DOI:10.1088/0953-8984/26/18/185401
PMID:24759233
Abstract

The thermodynamical properties of free-standing graphene have been investigated under constant zero pressure as a function of temperature using Monte Carlo simulations. A variety of atomistic models have been used, including the simple three-body Stillinger potential and a series of bond-order many-body potentials based on the Tersoff-Brenner seminal models, with recent reparametrizations dedicated to graphene, extensions to medium-range or long-range dispersion corrections. In addition, we have also tested a tight-binding potential in the fourth-moment approximation. The simulations reveal significant discrepancies in the in-plane lattice parameter and the thermal expansion coefficient, which despite showing monotonically increasing variations with temperature, can be positive, negative or change sign at moderate temperature depending on the potential. Comparison with existing experimental and theoretical data obtained from complementary approaches indicates that empirical potentials limited to nearest-neighbour interactions give rather dispersed results, and that van der Waals corrections generally tend to flatten the variations of the in-plane lattice constant, in contradiction with experiment. Only the medium-range corrected potentials of Los and Fasolino, as well as the tight-binding model in the fourth-moment approximation, are reasonably close to the reference results near room temperature. Our results suggest that classical potentials should be used with caution for thermal properties.

摘要

利用蒙特卡罗模拟,在恒定零压力下研究了独立石墨烯的热力学性质随温度的变化。使用了多种原子模型,包括简单的三体斯廷林格势以及基于特索夫 - 布伦纳开创性模型的一系列键序多体势,近期有专门针对石墨烯的重新参数化,以及对中程或长程色散修正的扩展。此外,我们还测试了四阶矩近似下的紧束缚势。模拟结果显示,面内晶格参数和热膨胀系数存在显著差异,尽管它们随温度呈现单调递增变化,但根据所使用的势,可能为正、为负或在中等温度下改变符号。与通过互补方法获得的现有实验和理论数据进行比较表明,限于最近邻相互作用的经验势给出的结果相当分散,并且范德华修正通常倾向于使面内晶格常数的变化趋于平缓,这与实验结果相矛盾。只有洛斯和法索利诺的中程修正势以及四阶矩近似下的紧束缚模型在室温附近与参考结果相当接近。我们的结果表明,对于热性质,经典势的使用应谨慎。

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