Threshold displacement energies in refractory high-entropy alloys

Jesper Byggmästar, Flyura Djurabekova, Kai Nordlund
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Abstract

Refractory high-entropy alloys show promising resistance to irradiation, yet little is known about the fundamental nature of radiation-induced defect formation. Here, we simulate threshold displacement energies in equiatomic MoNbTaVW using an accurate machine-learned interatomic potential, covering the full angular space of crystal directions. The effects of local chemical ordering is assessed by comparing results in randomly ordered and short-range-ordered MoNbTaVW. The average threshold displacement energy in the random alloy is $44.3 \pm 0.15$ eV and slightly higher, $48.6 \pm 0.15$ eV, in the short-range-ordered alloy. Both are significantly lower than in any of the constituent pure metals. We identify the mechanisms of defect creation and find that they are mainly dependent on the masses of the recoiling and colliding elements. Low thresholds are generally found when heavy atoms (W, Ta) displace and replace the lightest atoms (V). The average threshold energies when separated by recoiling element are consequently ordered inversely according to their mass, opposite to the trend in the pure metals where W has by far the highest thresholds. However, the trend in the alloy is reversed when considering the cross sections for defect formation in electron irradiation, due to the mass-dependent recoil energies from the electrons.
难熔高熵合金的阈值位移能
难熔高熵合金显示出良好的抗辐照性能,但人们对辐照诱导缺陷形成的基本性质知之甚少。在这里,我们使用精确的机器学习原子间位势模拟了等原子铌钽钒的阈值位移能,涵盖了晶体方向的全部角空间。通过比较随机有序和短程有序铌钽钨的结果,评估了局部化学排序的影响。随机合金的平均阈值位移能为 44.3 \pm 0.15$ eV,而短程有序合金的平均阈值位移能稍高,为 48.6 \pm 0.15$ eV。两者都明显低于任何一种纯金属成分。我们确定了缺陷产生的机制,发现它们主要取决于反冲和碰撞元素的质量。当重原子(W、Ta)置换和取代最轻原子(V)时,通常会发现低阈值。因此,按再沸元素分离时的平均阈值能与它们的质量成反比,这与纯金属中的趋势相反,在纯金属中 W 的阈值最高。然而,在考虑电子辐照下缺陷形成的截面时,由于电子的反冲能量与质量有关,合金中的趋势则相反。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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