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多温度原子系综:超快电子激发后的非平衡演化

Multitemperature atomic ensemble: Nonequilibrium evolution after ultrafast electronic excitation.

作者信息

Medvedev Nikita, Volkov Alexander E

机构信息

Institute of Physics of the <a href="https://ror.org/02yhj4v17">Czech Academy of Sciences</a>, Na Slovance 1999/2, 182 21 Prague 8, Czech Republic.

Institute of Plasma Physics of the <a href="https://ror.org/053avzc18">Czech Academy of Sciences</a>, Za Slovankou 1782/3, 182 00 Prague 8, Czech Republic.

出版信息

Phys Rev E. 2024 Aug;110(2-1):024142. doi: 10.1103/PhysRevE.110.024142.

DOI:10.1103/PhysRevE.110.024142
PMID:39294952
Abstract

Ultrafast laser radiation or beams of fast charged particles primarily excite the electronic system of a solid driving the target transiently out of thermal equilibrium. Apart from the nonequilibrium between the electrons and atoms, each subsystem may be far from equilibrium. From first principles, we derive the definition of various atomic temperatures applicable to electronically excited ensembles. It is shown that the definition of the kinetic temperature of atoms in the momentum subspace is unaffected by the excitation of the electronic system. When the electronic temperature differs from the atomic one, an expression for the configurational atomic temperature is proposed, applicable to the electronic-temperature-dependent interatomic potentials (such as ab initio molecular dynamics simulations). We study how the configurational temperature behaves during nonthermal phase transition, triggered by the evolution of the interatomic potential due to the electronic excitation. It is revealed that upon the ultrafast irradiation, the atomic system of a solid exists temporarily in a multitemperature state: separate equilibria in the momentum and configurational subspaces. Complete equilibration between the various atomic temperatures takes place at longer timescales, forming the energy equipartition. Based on these results, we propose a formulation of multitemperature heat transport equations.

摘要

超快激光辐射或快速带电粒子束主要激发固体的电子系统,使靶材瞬间偏离热平衡状态。除了电子与原子之间的非平衡外,每个子系统可能都远非处于平衡状态。从第一性原理出发,我们推导出适用于电子激发系综的各种原子温度的定义。结果表明,动量子空间中原子的动力学温度定义不受电子系统激发的影响。当电子温度与原子温度不同时,提出了一种构型原子温度的表达式,适用于与电子温度相关的原子间势(如从头算分子动力学模拟)。我们研究了在由电子激发引起的原子间势演化所触发的非热相变过程中,构型温度的行为。结果表明,在超快辐照下,固体的原子系统暂时处于多温度状态:动量和构型子空间中的独立平衡态。各种原子温度之间的完全平衡在更长的时间尺度上发生,形成能量均分。基于这些结果,我们提出了多温度热传输方程的一种表述形式。

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