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金属系统中间隙原子的扩散,一个复杂研究案例的说明:铝。

Diffusion of interstitials in metallic systems, illustration of a complex study case: aluminum.

作者信息

David Matthieu, Connétable Damien

机构信息

CIRIMAT UMR 5085, CNRS-INP-UPS, ENSIACET 4, allée Émile Monso, BP 44362, F-31030 Toulouse Cedex 4, France.

出版信息

J Phys Condens Matter. 2017 Nov 15;29(45):455703. doi: 10.1088/1361-648X/aa8e5e. Epub 2017 Oct 19.

DOI:10.1088/1361-648X/aa8e5e
PMID:29049029
Abstract

While diffusion mechanisms of interstitial elements in fcc systems are generally well-known, especially in the case of H atoms, we show in this work that even in the case of a simple metallic system (aluminum), the diffusion of interstitials exhibits a wide variety of paths and mechanisms that depend on the specie. We used an approach based on first-principles calculations associated with kinetic Monte-Carlo simulations and a multi-state diffusion formalism to compute the diffusion coefficients of five interstitial elements: hydrogen, boron, carbon, nitrogen and oxygen. For instance, at the atomic scale, whilst we find that C atoms prefer to be located in octahedral sites (labeled o) rather than in tetrahedral positions (labeled t), we find one additional stable position in the lattice (M). The diffusion through these three stable positions are thus studied in detail. In the case of B atoms, for which the tetrahedral site is found unstable, the diffusion path is between o-o sites. Similarly, in the case of oxygen, t positions are found to be the only stable positions (o are unstable) and the path of migration, along t-t direction, is found through a twice degenerated asymmetric transition state. In the case of H and N atoms for which t and o sites are stable, we explain why the only path is along the t-o direction. Finally, we discuss explicit formulas to compute coefficients of diffusion of interstitials in fcc structures.

摘要

虽然面心立方(fcc)体系中间隙元素的扩散机制通常是广为人知的,尤其是氢原子的情况,但我们在这项工作中表明,即使在简单金属体系(铝)的情况下,间隙原子的扩散也表现出各种各样取决于种类的路径和机制。我们采用了一种基于第一性原理计算并结合动力学蒙特卡罗模拟和多态扩散形式的方法,来计算五种间隙元素:氢、硼、碳、氮和氧的扩散系数。例如,在原子尺度上,虽然我们发现碳原子更喜欢位于八面体位置(标记为o)而不是四面体位置(标记为t),但我们在晶格中发现了另一个稳定位置(M)。因此,对通过这三个稳定位置的扩散进行了详细研究。对于硼原子,发现四面体位置不稳定,其扩散路径是在o - o位置之间。同样,对于氧原子,发现t位置是唯一的稳定位置(o位置不稳定),并且沿着t - t方向的迁移路径是通过一个二度简并的不对称过渡态找到的。对于t和o位置都稳定的氢和氮原子,我们解释了为什么唯一的路径是沿着t - o方向。最后,我们讨论了计算fcc结构中间隙原子扩散系数的显式公式。

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