室温下金属原子尺度模拟中的非局域电子-声子耦合。

Maxime Malingre, Laurent Proville, Jean-Paul Crocombette
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引用次数: 0

摘要

双温度模型(TTM)通常用于金属晶体在辐照下建立超出玻恩-奥本海默近似的预测。在正常条件下,对热非均质材料的热峰衰减进行了研究,发现当热非均质材料尺寸小于电子平均自由程时,热峰衰减速率与电子导电性无关,而当热非均质材料尺寸大于电子平均自由程时,热峰衰减速率主要由电子导电性驱动。发现需要额外的非局部耦合来恢复弛豫时间,这取决于所有尺寸的电子电导率,正如对金属的期望一样。提出了一种将非局部贡献转化为分子动力学模拟的方法。我们通过研究Au和Ni的电子性质有显著差异来检验我们方法的可转移性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Non-local electron-phonon coupling in atomic scale simulations at room temperature in metals.

The two temperature model (TTM) is commonly used in metallic crystals under irradiation to establish predictions beyond the Born-Oppenheimer approximation. Examining in normal conditions, the heat spike decrease in TTM we remarked that oddly the decrease rate is independent from electron conductivity when the thermal heterogeneity has size inferior to electron mean free path whilst for larger sizes the decrease is essentially driven by electron conductivity. An additional non-local coupling was found to be necessary to recover a relaxation time depending on the electron conductivity at all sizes, as expected for metals. A method is proposed to transfer the non-local contribution into molecular dynamics simulations. We check transferability of our method through the study of Au and Ni of which electronic properties differ significantly.

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