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Time-dependent exchange-correlation current density functionals with memory

机译:带存储器的时间相关交换相关电流密度函数

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Most present applications of time-dependent density functional theory use adiabatic functionals, i.e., the effective potential at time t is determined solely by the density at the same time. This paper discusses a method that aims to go beyond this approximation, by incorporating "memory" effects: the derived exchange-correlation potential will depend not only on present densities but also on the past. In order to ensure the potentials are causal, we formulate the action on the Keldysh contour for electrons in electromagnetic fields, from which we derive suitable Kohn-Sham equations. The exchange-correlation action is now a functional of the electron density and velocity field. A specific action functional is constructed which is Galilean invariant and yields a causal exchange-correlation vector potential for the Kohn-Sham equations incorporating memory effects. We show explicitly that the net exchange-correlation Lorentz force is zero. The potential is consistent with known dynamical properties of the homogeneous electron gas (in the linear response limit). (C) 2004 American Institute of Physics.
机译:随时间变化的密度泛函理论的大多数当前应用使用绝热泛函,即,在时刻t的有效电势仅由同时的密度决定。本文讨论了一种方法,该方法旨在通过结合“内存”效应来超越此近似值:导出的交换相关势将不仅取决于当前的密度,还取决于过去的密度。为了确保电势具有因果关系,我们对电磁场中电子对Keldysh轮廓的作用进行了公式化,由此得出了合适的Kohn-Sham方程。现在,交换相关作用是电子密度和速度场的函数。构造了一个特定的动作函数,它是伽利略不变式,并为包含记忆效应的Kohn-Sham方程产生了因果交换相关矢量势。我们明确表明,净交换相关洛伦兹力为零。该电势与均匀电子气的已知动力学特性(在线性响应极限内)一致。 (C)2004年美国物理研究所。

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