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通过准弹性中子散射和分子动力学模拟探测液态镓及镓镍合金中的原子扩散。

Atomic diffusion in liquid gallium and gallium-nickel alloys probed by quasielastic neutron scattering and molecular dynamic simulations.

作者信息

Shahzad A, Yang F, Steffen J, Neiss C, Panchenko A, Goetz K, Vogel C, Weisser M, Embs J P, Petry W, Lohstroh W, Görling A, Goychuk I, Unruh T

机构信息

Institute for Crystallography and Structural Physics, Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Staudtstraße 3, Erlangen 91058, Germany.

Interdisciplinary Center for Nanostructured Films (IZNF) and Center for Nanoanalysis and Electron Microscopy (CENEM), Cauerstraße 3, Erlangen 91058, Germany.

出版信息

J Phys Condens Matter. 2024 Feb 1;36(17). doi: 10.1088/1361-648X/ad1e9f.

Abstract

The atomic mobility in liquid pure gallium and a gallium-nickel alloy with 2 at% of nickel is studied experimentally by incoherent quasielastic neutron scattering. The integral diffusion coefficients for all-atom diffusion are derived from the experimental data at different temperatures. DFT-basedmolecular dynamics (MD) is used to find numerically the diffusion coefficient of liquid gallium at different temperatures, and numerical theory results well agree with the experimental findings at temperatures below 500 K. Machine learning force fields derived frommolecular dynamics (AIMD) overestimate within a small 6% error the diffusion coefficient of pure gallium within the genuine AIMD. However, they better agree with experiment for pure gallium and enable the numerical finding of the diffusion coefficient of nickel in the considered melted alloy along with the diffusion coefficient of gallium and integral diffusion coefficient, that agrees with the corresponding experimental values within the error bars. The temperature dependence of the gallium diffusion coefficientDGa(T)follows the Arrhenius law experimentally for all studied temperatures and below 500 K also in the numerical simulations. However,DGa(T)can be well described alternatively by an Einstein-Stokes dependence with the metallic liquid viscosity following the Arrhenius law, especially for the MD simulation results at all studied temperatures. Moreover, a novel variant of the excess entropy scaling theory rationalized our findings for gallium diffusion. Obtained values of the Arrhenius activation energies are profoundly different in the competing theoretical descriptions, which is explained by different temperature-dependent prefactors in the corresponding theories. The diffusion coefficient of gallium is significantly reduced (at the same temperature) in a melted alloy with natural nickel, even at a tiny 2 at% concentration of nickel, as compared with its pure gallium value. This highly surprising behavior contradicts the existing excess entropy scaling theories and opens a venue for further research.

摘要

通过非相干准弹性中子散射实验研究了液态纯镓和含2原子百分比镍的镓镍合金中的原子迁移率。从不同温度下的实验数据推导出全原子扩散的积分扩散系数。基于密度泛函理论(DFT)的分子动力学(MD)用于数值求解不同温度下液态镓的扩散系数,数值理论结果与500 K以下温度的实验结果吻合良好。从分子动力学(AIMD)导出的机器学习力场在真实AIMD范围内对纯镓的扩散系数高估了6%的小误差。然而,它们与纯镓的实验结果更吻合,并能够数值求解所考虑的熔融合金中镍的扩散系数以及镓的扩散系数和积分扩散系数,在误差范围内与相应的实验值一致。对于所有研究温度以及数值模拟中500 K以下的温度,镓扩散系数DGa(T)的温度依赖性实验上遵循阿仑尼乌斯定律。然而,DGa(T)也可以用爱因斯坦-斯托克斯依赖性很好地描述,其中金属液体粘度遵循阿仑尼乌斯定律,特别是对于所有研究温度下的MD模拟结果。此外,过量熵标度理论的一个新变体使我们对镓扩散的研究结果合理化。在相互竞争的理论描述中,阿仑尼乌斯活化能的获得值有很大差异,这是由相应理论中不同的温度依赖前置因子解释的。与纯镓值相比,即使在镍浓度仅为2原子百分比的情况下,含天然镍的熔融合金中镓的扩散系数(在相同温度下)也显著降低。这种非常令人惊讶的行为与现有的过量熵标度理论相矛盾,并为进一步研究开辟了道路。

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