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部分量子分子动力学的流体力学表示。

Partial hydrodynamic representation of quantum molecular dynamics.

机构信息

Department of Chemistry, University of Rochester, Rochester, New York 14627, USA.

出版信息

J Chem Phys. 2017 May 21;146(19):194104. doi: 10.1063/1.4983495.

Abstract

A hybrid method is proposed to propagate system-bath quantum dynamics that use both basis functions and coupled quantum trajectories. In it, the bath is represented with an ensemble of Bohmian trajectories while the system degrees of freedom are accounted through reduced density matrices. By retaining the Hilbert space structure for the system, the method is able to capture interference processes that are challenging to describe in Bohmian dynamics due to singularities that these processes introduce in the quantum potential. By adopting quantum trajectories to represent the bath, the method beats the exponential scaling of the computational cost with the bath size. This combination makes the method suitable for large-scale ground and excited state fully quantum molecular dynamics simulations. Equations of motion for the quantum trajectories and reduced density matrices are derived from the Schrödinger equation and a computational algorithm to solve these equations is proposed. Through computations in two-dimensional model systems, the method is shown to offer an accurate description of subsystem observables and of quantum decoherence, which is difficult to obtain when the quantum nature of the bath is ignored. The scaling of the method is demonstrated using a model with 21 degrees of freedom. The limit of independent trajectories is recovered when the mass of bath degrees of freedom is much larger than the one of the system, in agreement with mixed quantum-classical descriptions.

摘要

提出了一种混合方法来传播使用基函数和耦合量子轨迹的系统-浴量子动力学。在这种方法中,浴被表示为一组玻姆轨迹,而系统自由度则通过约化密度矩阵来描述。通过保留系统的希尔伯特空间结构,该方法能够捕捉到由于这些过程在量子势中引入的奇点而使得玻姆动力学难以描述的干涉过程。通过采用量子轨迹来表示浴,该方法克服了由于浴尺寸的增加而导致计算成本呈指数级增长的问题。这种组合使得该方法适用于大规模的基态和激发态全量子分子动力学模拟。从薛定谔方程推导出了量子轨迹和约化密度矩阵的运动方程,并提出了一种求解这些方程的计算算法。通过在二维模型系统中的计算,该方法被证明能够准确描述子系统可观测量和量子退相干,而忽略浴的量子性质时很难获得这些性质。使用具有 21 个自由度的模型演示了该方法的缩放性。当浴自由度的质量远大于系统的质量时,会恢复独立轨迹的极限,这与混合量子-经典描述一致。

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