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The dynamics of highly excited electronic systems: Applications of the electron force field

机译:高激发电子系统的动力学:电子力场的应用

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Highly excited heterogeneous complex materials are essential elements of important processes, ranging from inertial confinement fusion to semiconductor device fabrication. Understanding the dynamics of these systems has been challenging because of the difficulty in extracting mechanistic information from either experiment or theory. We describe here the electron force field (eFF) approximation to quantum mechanics which provides a practical approach to simulating the dynamics of such systems. eFF includes all the normal electrostatic interactions between electrons nd nuclei and the normal quantum mechanical description of kinetic energy for the electrons, but contains two severe approximations: first, the individual electrons are represented as floating Gaussian wave packets whose position and size respond instantaneously to various forces during the dynamics; and second, these wave packets are combined into a many-body wave function as a Hartree product without explicit antisymmetrization. The Pauli principle is accounted for by adding an extra spin-dependent term to the Hamiltonian. These approximations are a logical extension of existing approaches to simulate the dynamics of fermions, which we review. In this paper, we discuss the details of the equations of motion and potentials that form eFF, and evaluate the ability of eFF to describe ground-state systems containing covalent, ionic, multicenter, and/or metallic bonds. We also summarize two eFF calculations previously reported on electronically excited systems: (1) the thermodynamics of hydrogen compressed up to ten times liquid density and heated up to 200 000 K; and (2) the dynamics of Auger fragmentation in a diamond nanoparticle, where hundreds of electron volts of excitation energy are dissipated over tens of femtoseconds. These cases represent the first steps toward using eFF to model highly excited electronic processes in complex materials.
机译:从惯性约束融合到半导体器件制造,高激发的异质复杂材料是重要过程的基本要素。由于难以从实验或理论中提取机械信息,因此了解这些系统的动态一直具有挑战性。我们在这里描述了量子力学的电子力场(eFF)近似值,它提供了一种模拟此类系统动力学的实用方法。 eFF包括电子与原子核之间的所有正常静电相互作用以及电子的动能的正常量子力学描述,但包含两个严格的近似值:首先,单个电子表示为浮动高斯波包,其位置和大小对各种瞬时响应动态过程中的力量;其次,这些波包被组合成一个多体波函数,作为Hartree乘积,而没有明确的反对称化。通过向哈密顿量添加一个额外的自旋相关项来说明保利原理。这些近似值是模拟费米子动力学的现有方法的逻辑扩展,我们将对其进行回顾。在本文中,我们讨论了形成eFF的运动方程和电位方程的详细信息,并评估了eFF描述包含共价键,离子键,多中心键和/或金属键的基态系统的能力。我们还总结了先前在电子激发系统上报告的两种eFF计算:(1)氢的热力学压缩至液体密度的十倍,并加热至200 000 K; (2)金刚石纳米粒子中俄歇碎片的动力学,其中数百电子伏特的激发能在数十飞秒内耗散。这些情况代表了使用eFF建模复杂材料中的高激发电子过程的第一步。

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