Self-interstitial atom properties in Nb–Mo–Ta–W alloys

扩散 合金 Atom(片上系统) 不对称 材料科学 金属 格子(音乐) 化学物理 八面体 间质缺损 辐照 分子物理学 结晶学 凝聚态物理 化学 晶体结构 热力学 冶金 物理 光电子学 兴奋剂 量子力学 计算机科学 声学 核物理学 嵌入式系统
作者
Xinran Zhou,Annie K. Barnett,Emily H. Mang,Michael L. Falk,Mitra L. Taheri,Jaime Marian
出处
期刊:Computational Materials Science [Elsevier BV]
卷期号:234: 112765-112765
标识
DOI:10.1016/j.commatsci.2023.112765
摘要

Self-interstitial atoms (SIA) are generated in collision cascades during high-energy particle irradiation of crystalline materials. In pure metals, SIA generally adopt split configurations and display fast mobilities along one-dimensional trajectories. This differentiates them from vacancies, which move in confined three-dimensional paths. This asymmetry is one of the pillars of irradiation damage theories that have been successful in explaining a number features of the irradiation response of pure metals and dilute alloys. However, in complex concentrated alloys consisting of several metallic elements in equal or near equal proportions, lattice distortions associated with compositional fluctuations change the potential energy landscape on atomic scales, leading to SIA structures not seen in their pure metal counterparts. In this paper, we use atomistic simulations to study the properties of self-interstitial atoms in the quaternary equiatomic Nb–Mo–Ta–W refractory alloy. Chemically, these SIA defects adopt a variety of structures involving all pairs of atoms. We find the 〈111〉 orientation to be the most common among all split configurations, but we also observe – surprisingly – a relatively high occurrence of octahedral SIA. In terms of their diffusivities, we find two clearly distinguished regimes below and above 600 K, where the SIA diffusion changes dimensionality from 1D to 3D. We calculate the migration energies and diffusion pre-factors in both regions, from which we extract the translational and rotational components of the defect migration. We find values of 0.25 eV and pre-factors of ∼10−11 m2 s−1 in the low temperature regime, and 0.57 eV and ∼10−8 m2 s−1 in the high temperature one. From this, we estimate a rotational energy barrier of 0.37 eV.
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