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聚对苯撑乙烯链内激子迁移的第一性原理描述。II. 扭转缺陷处激子动力学的多组态含时密度泛函理论模拟

First-principles description of intra-chain exciton migration in an oligo(para-phenylene vinylene) chain. II. ML-MCTDH simulations of exciton dynamics at a torsional defect.

作者信息

Binder Robert, Burghardt Irene

机构信息

Institute for Physical and Theoretical Chemistry, Goethe University, Max-von-Laue-Str. 7, 60438 Frankfurt/Main, Germany.

出版信息

J Chem Phys. 2020 May 29;152(20):204120. doi: 10.1063/5.0004511.

Abstract

The first-principles parameterized Frenkel-Holstein Hamiltonian developed in Paper I [R. Binder et al., J. Chem. Phys. 152, 204119 (2020)] is employed to carry out full quantum-dynamical simulations of an elementary exciton migration event in an oligo-(para-phenylene vinylene) chain with 20 repeat units (OPV-20). We consider a dynamic scenario where an initial torsional defect, creating a conjugation break, relaxes on a time scale of about 500 fs toward a planarized structure and triggers the spatial displacement of the photogenerated exciton. Accurate quantum dynamical simulations are performed using the multi-layer multi-configuration time-dependent Hartree method as applied to an OPV-20 system comprising 20 electronic states of Frenkel type and 60 vibrational modes. These include site-local quinoid-distortion modes, site-correlated bond-length alternation (BLA) modes, and an active ring torsional mode at the central junction. The simulations fully account for correlations between the ring torsional mode and the anharmonically coupled BLA coordinate located at the same junction. In accordance with our earlier studies of a related oligothiophene (OT) system [R. Binder, D. Lauvergnat, and I. Burghardt, Phys. Rev. Lett. 120, 227401 (2018)], these simulation results highlight that exciton migration is a coherent process driven by the fluctuations of "soft" modes, exemplified by the ring torsions. Conversely, these results also show that trapping due to high-frequency modes, leading to energetic stabilization of the exciton-polaron species, is weaker in OPV than in the OT system. This underscores not only the generic features of exciton dynamics in conjugated polymer systems, but also the role of molecular specificities.

摘要

我们采用在论文I [R. Binder等人,《化学物理杂志》152, 204119 (2020)] 中开发的第一性原理参数化弗伦克尔 - 霍尔斯坦哈密顿量,对具有20个重复单元的寡聚(对亚苯基乙烯基)链(OPV - 20)中的基本激子迁移事件进行全量子动力学模拟。我们考虑一种动态场景,即初始的扭转缺陷会导致共轭中断,该缺陷在约500飞秒的时间尺度上弛豫到平面化结构,并触发光生激子的空间位移。使用多层多组态含时哈特里方法对包含20个弗伦克尔型电子态和60个振动模式的OPV - 20系统进行精确的量子动力学模拟。这些模式包括位点局部醌式畸变模式、位点相关的键长交替(BLA)模式以及中心连接处的活性环扭转模式。模拟充分考虑了环扭转模式与位于同一连接处的非谐耦合BLA坐标之间的相关性。与我们早期对相关寡聚噻吩(OT)系统的研究 [R. Binder, D. Lauvergnat, and I. Burghardt, 《物理评论快报》120, 227401 (2018)] 一致,这些模拟结果突出表明,激子迁移是一个由“软”模式(如环扭转)的涨落驱动的相干过程。相反,这些结果还表明,在OPV中,由高频模式导致的捕获(从而使激子 - 极化子物种能量稳定)比在OT系统中更弱。这不仅强调了共轭聚合物系统中激子动力学的一般特征,也突出了分子特异性的作用。

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