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用于等离子体系统中热载流子动力学的随机薛定谔方程。

Stochastic Schrödinger equation for hot-carrier dynamics in plasmonic systems.

作者信息

Dall'Osto Giulia, Vanzan Mirko, Corni Stefano, Marsili Margherita, Coccia Emanuele

机构信息

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

Dipartimento di Fisica, Università di Milano, Via Giovanni Celoria 16, 20133 Milano, Italy.

出版信息

J Chem Phys. 2024 Sep 28;161(12). doi: 10.1063/5.0221179.

Abstract

We present a multiscale method coupling the theory of open quantum systems with real-time ab initio treatment of electronic structure to study hot-carrier dynamics in photoexcited plasmonic systems. We combine the Markovian Stochastic Schrödinger equation with an ab initio GW coupled to the Bethe-Salpeter (BSE) equation description of the electronic degrees of freedom, interacting with a metallic nanoparticle modeled classically according to the polarizable continuum model. We apply this methodology to study the effect of relaxation (T1) and pure dephasing (T2) times on the hot-carrier dynamics in a system composed of a quantum portion described at GW/BSE level, i.e., a CHO fragment adsorbed on a vertex of a rhodium nanocube, and of the rest of the nanocube, treated classically, when irradiated with a 2.7 eV light pulse, inspired by the experimental results on plasmon-driven CO2 photoreduction. A net hole injection from rhodium to CHO is observed, with and without the classical portion of the nanocube. The nanocube effect is to enhance the generated charge population by two orders of magnitude. The nonradiative decay, via a relaxation time T1 based on the energy-gap law, produces a rapid decrease of the charge population. Results with T2 only show that a charge injection retarded with respect to the pulse, which is present in the coherent dynamics, disappears when coherence is erased.

摘要

我们提出了一种多尺度方法,将开放量子系统理论与电子结构的实时从头算处理相结合,以研究光激发等离子体系统中的热载流子动力学。我们将马尔可夫随机薛定谔方程与从头算GW相结合,并耦合到电子自由度的贝叶斯-萨尔皮特(BSE)方程描述,该电子自由度与根据可极化连续介质模型经典建模的金属纳米颗粒相互作用。我们应用这种方法来研究弛豫时间(T1)和纯退相时间(T2)对由GW/BSE水平描述的量子部分(即吸附在铑纳米立方体顶点上的CHO片段)和经典处理的纳米立方体其余部分组成的系统中热载流子动力学的影响,该系统在2.7 eV光脉冲照射下,灵感来自等离子体驱动的CO2光还原的实验结果。无论有无纳米立方体的经典部分,都观察到从铑到CHO的净空穴注入。纳米立方体的作用是将产生的电荷数量提高两个数量级。基于能隙定律的弛豫时间T1导致的非辐射衰变会使电荷数量迅速减少。仅考虑T2时的结果表明,相干动力学中存在的相对于脉冲延迟的电荷注入,在相干消除时消失。

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