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耗散电子系统的精确动力学与量子输运:运动方程的层级方法。

Exact dynamics of dissipative electronic systems and quantum transport: Hierarchical equations of motion approach.

作者信息

Jin Jinshuang, Zheng Xiao, Yan YiJing

机构信息

Department of Chemistry, Hong Kong University of Science and Technology, Kowloon, Hong Kong.

出版信息

J Chem Phys. 2008 Jun 21;128(23):234703. doi: 10.1063/1.2938087.

DOI:10.1063/1.2938087
PMID:18570515
Abstract

A generalized quantum master equation theory that governs the exact, nonperturbative quantum dissipation and quantum transport is formulated in terms of hierarchically coupled equations of motion for an arbitrary electronic system in contact with electrodes under either a stationary or a nonstationary electrochemical potential bias. The theoretical construction starts with the influence functional in path integral, in which the electron creation and annihilation operators are Grassmann variables. Time derivatives on the influence functionals are then performed in a hierarchical manner. Both the multiple-frequency dispersion and the non-Markovian reservoir parametrization schemes are considered for the desired hierarchy construction. The resulting hierarchical equations of motion formalism is in principle exact and applicable to arbitrary electronic systems, including Coulomb interactions, under the influence of arbitrary time-dependent applied bias voltage and external fields. Both the conventional quantum master equation and the real-time diagrammatic formalism of Schon and co-workers can be readily obtained at well defined limits of the present theory. We also show that for a noninteracting electron system, the present hierarchical equations of motion formalism terminates at the second tier exactly, and the Landuer-Buttiker transport current expression is recovered. The present theory renders an exact and numerically tractable tool to evaluate various transient and stationary quantum transport properties of many-electron systems, together with the involving nonperturbative dissipative dynamics.

摘要

一种广义量子主方程理论被提出,它用于描述精确的、非微扰的量子耗散和量子输运。该理论基于与电极接触的任意电子系统在稳态或非稳态电化学势偏压下的层次耦合运动方程。理论构建从路径积分中的影响泛函开始,其中电子产生和湮灭算符为格拉斯曼变量。然后以层次方式对影响泛函进行时间导数运算。为了构建所需的层次结构,考虑了多频色散和非马尔可夫库仑参数化方案。所得的层次运动方程形式原则上是精确的,适用于任意电子系统,包括库仑相互作用,在任意随时间变化的外加偏置电压和外场影响下。在本理论定义明确的极限情况下,可以很容易地得到传统量子主方程以及舍恩及其同事的实时图解形式。我们还表明,对于非相互作用电子系统,当前的层次运动方程形式在第二层恰好终止,并恢复了兰道尔 - 布蒂克尔输运电流表达式。本理论提供了一个精确且数值上易于处理的工具,用于评估多电子系统的各种瞬态和稳态量子输运性质,以及涉及的非微扰耗散动力学。

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