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量子随机轨迹:由约化密度矩阵驱动的福克-普朗克-玻姆方程

Quantum Stochastic Trajectories: The Fokker-Planck-Bohm Equation Driven by the Reduced Density Matrix.

作者信息

Avanzini Francesco, Moro Giorgio J

机构信息

Dipartimento di Scienze Chimiche , Università di Padova , via Marzolo 1 , 35131 Padova , Italy.

出版信息

J Phys Chem A. 2018 Mar 15;122(10):2751-2763. doi: 10.1021/acs.jpca.7b11943. Epub 2018 Mar 6.

Abstract

The quantum molecular trajectory is the deterministic trajectory, arising from the Bohm theory, that describes the instantaneous positions of the nuclei of molecules by assuring the agreement with the predictions of quantum mechanics. Therefore, it provides the suitable framework for representing the geometry and the motions of molecules without neglecting their quantum nature. However, the quantum molecular trajectory is extremely demanding from the computational point of view, and this strongly limits its applications. To overcome such a drawback, we derive a stochastic representation of the quantum molecular trajectory, through projection operator techniques, for the degrees of freedom of an open quantum system. The resulting Fokker-Planck operator is parametrically dependent upon the reduced density matrix of the open system. Because of the pilot role played by the reduced density matrix, this stochastic approach is able to represent accurately the main features of the open system motions both at equilibrium and out of equilibrium with the environment. To verify this procedure, the predictions of the stochastic and deterministic representation are compared for a model system of six interacting harmonic oscillators, where one oscillator is taken as the open quantum system of interest. The undeniable advantage of the stochastic approach is that of providing a simplified and self-contained representation of the dynamics of the open system coordinates. Furthermore, it can be employed to study the out of equilibrium dynamics and the relaxation of quantum molecular motions during photoinduced processes, like photoinduced conformational changes and proton transfers.

摘要

量子分子轨迹是源自玻姆理论的确定性轨迹,它通过确保与量子力学的预测一致来描述分子原子核的瞬时位置。因此,它为表示分子的几何形状和运动提供了合适的框架,而不会忽略其量子性质。然而,从计算的角度来看,量子分子轨迹的要求极高,这严重限制了它的应用。为了克服这一缺点,我们通过投影算符技术,为开放量子系统的自由度推导了量子分子轨迹的随机表示。由此产生的福克 - 普朗克算符参数化地依赖于开放系统的约化密度矩阵。由于约化密度矩阵所起的引导作用,这种随机方法能够准确地表示开放系统在与环境处于平衡和非平衡状态下运动的主要特征。为了验证这一过程,我们对一个由六个相互作用的谐振子组成的模型系统进行了比较,其中一个振子被视为感兴趣的开放量子系统,比较了随机表示和确定性表示的预测结果。随机方法的一个不可否认的优点是,它为开放系统坐标的动力学提供了一种简化且自成体系的表示。此外,它可用于研究光诱导过程中量子分子运动的非平衡动力学和弛豫,如光诱导构象变化和质子转移。

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