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分子组装体中的强激子 - 振动耦合。在热场动力学(HEOM)空间中使用极化子变换的动力学

Strong Exciton-Vibrational Coupling in Molecular Assemblies. Dynamics Using the Polaron Transformation in HEOM Space.

作者信息

Seibt Joachim, Kühn Oliver

机构信息

Institute of Physics, University of Rostock, Albert-Einstein-Str. 23-24, 18059 Rostock, Germany.

Institute for Theoretical Physics, Johannes Kepler University Linz, Altenberger Str. 69, 4040 Linz, Austria.

出版信息

J Phys Chem A. 2021 Aug 19;125(32):7052-7065. doi: 10.1021/acs.jpca.1c02684. Epub 2021 Aug 5.

DOI:10.1021/acs.jpca.1c02684
PMID:34353023
Abstract

In Frenkel exciton dynamics of aggregated molecules, the polaron transformation (PT) technique leads to decoupling of diagonal elements in the subspace of excited electronic states from vibrations. In this article we describe for the first time how PT becomes applicable in the framework of the "Hierarchical Equations of Motion" (HEOM) approach for treatment of open quantum systems. We extend the concept of formulating operators in HEOM space by deriving hierarchical equations of PT which lead to a shift in the excited state potential energy surface to compensate its displacement. While the assumption of thermal equilibration of the vibrational oscillators, introduced by PT, results in a stationary state in a monomer, in a dimer under the same assumption nonequilibrium dynamics appears because of the interplay of the transfer process and vibrational equilibration. Both vertical transitions generating a vibrationally hot state and initially equilibrated vibrational oscillators evolve toward the same stationary asymptotic state associated with polaron formation. The effect of PT on the dynamics of this process depends on initial excitation and basis representation of the electronic system. The developed approach facilitates a generic formulation of quantum master equations involving perturbative treatment of polaron dynamics.

摘要

在聚集分子的弗伦克尔激子动力学中,极化子变换(PT)技术使得激发电子态子空间中的对角元素与振动解耦。在本文中,我们首次描述了PT如何在用于处理开放量子系统的“运动分层方程”(HEOM)方法框架中适用。我们通过推导PT的分层方程扩展了在HEOM空间中制定算符的概念,该方程导致激发态势能面发生位移以补偿其偏移。虽然PT引入的振动振荡器热平衡假设在单体中导致稳态,但在二聚体中,由于转移过程和振动平衡的相互作用,在相同假设下会出现非平衡动力学。产生振动热态的垂直跃迁和初始平衡的振动振荡器都朝着与极化子形成相关的相同稳态渐近态演化。PT对该过程动力学的影响取决于电子系统的初始激发和基表示。所开发的方法有助于涉及极化子动力学微扰处理的量子主方程的通用表述。

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