金中∑= 13 (θ = 22.6°)[001]扭转边界的原子结构计算

S.M. Foiles
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引用次数: 25

摘要

用嵌入原子法(EAM)计算了金的∑= 13 (θ = 22.6°)[001]扭转边界的结构。计算了边界附近的原子位置,发现与菲茨西蒙斯和萨斯最近的x射线衍射结果很吻合。利用蒙特卡罗模拟计算了热位移的振幅,并与菲茨西蒙斯计算的边界平均德拜-沃勒系数进行了比较。伯克尔和萨斯。发现靠近边界的原子的振动幅值比体内的大,并且边界平面上的振动比与边界垂直的振动增强更大。使用EAM获得的这些结果也与使用两种不同的对相互作用获得的结果进行了比较。使用多体EAM相互作用的结果与使用对相互作用的结果之间的主要区别是,使用EAM发现边界的整体扩展较小。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Calculation of the atomic structure of the ∑ = 13 (θ = 22.6°) [001] twist boundary in gold

The structure of the ∑ = 13 (θ = 22.6°) [001] twist boundary in gold is computed using the Embedded Atom Method (EAM). The atomic positions near the boundary are computed and found to be in good agreement with the recent X-ray diffraction results of Fitzsimmons and Sass. The amplitude of the thermal displacements is also computed from the EAM using Monte Carlo simulations and compared with the results for the average Debye-Waller factor of the boundary obtained by Fitzsimmons. Burkel and Sass. The vibrational amplitudes of the atoms adjacent to the boundary are found to be larger than in the bulk and the enhancement is greater for vibrations in the plane of the boundary than for vibrations normal to the boundary. These results obtained using the EAM are also compared to results obtained using two different pair interactions. The main difference between the results using the many-body EAM interactions and the pair interactions is that the overall expansion of the boundary is found to be smaller using the EAM.

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