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激子耦合硼二吡咯二聚体中的受激共振拉曼和激发态动力学:对含时密度泛函理论和极化连续介质模型的检验

Stimulated Resonance Raman and Excited-State Dynamics in an Excitonically Coupled Bodipy Dimer: A Test for TD-DFT and the Polarizable Continuum Model.

作者信息

Sandoval Juan S, Gong Qingbao, Jiao Lijuan, McCamant David W

机构信息

Department of Chemistry, University of Rochester, 120 Trustee Road, Rochester, New York 14627, United States.

School of Chemistry and Materials Science, Anhui Normal University, Wuhu 241002, China.

出版信息

J Phys Chem A. 2023 Aug 31;127(34):7156-7167. doi: 10.1021/acs.jpca.3c02978. Epub 2023 Aug 18.

Abstract

Bodipy is one of the most versatile and studied functional dyes due to its myriad applications and tunable spectral properties. One of the strategies to adjust their properties is the formation of Bodipy dimers and oligomers whose properties differ significantly from the corresponding monomer. Recently, we have developed a novel strategy for synthesizing α,α-ethylene-bridged Bodipy dimers; however, their excited-state dynamics was heretofore unknown. This work presents the ultrafast excited-state dynamics of a novel α,α-ethylene-bridge Bodipy dimer and its monomeric parent. The dimer's steady-state absorption and fluorescence suggest a Coulombic interaction between the monomeric units' transition dipole moments (TDMs), forming what is often termed a "J-dimer". The excited-state properties of the dimer were studied using molecular excitonic theory and time-dependent density functional theory (TD-DFT). We chose the M06 exchange-correlation functional (XCF) based on its ability to reproduce the experimental oscillator strength and resonance Raman spectra. Ultrafast laser spectroscopy reveals symmetry-breaking charge separation (SB-CS) in the dimer in polar solvents and the subsequent population of the charge-separated ion-pair state. The charge separation rate falls into the normal regime, while the charge recombination is in the inverted regime. Conversely, in nonpolar solvents, the charge separation is thermodynamically not feasible. In contrast, the monomer's excited-state dynamics shows no dependence on the solvent polarity. Furthermore, we found no evidence of significant structural rearrangement upon photoexcitation, regardless of the deactivation pathway. After an extensive analysis of the electronic transitions, we concluded that the solvent fluctuations in the local environment around the dimer create an asymmetry that drives and stabilizes the charge separation. This work sheds light on the charge-transfer process in this new set of molecular systems and how excited-state dynamics can be modeled by combining the experiment and theory.

摘要

由于其众多的应用和可调节的光谱特性,Bodipy是用途最广泛且研究最多的功能性染料之一。调整其性质的策略之一是形成Bodipy二聚体和寡聚体,它们的性质与相应的单体有显著差异。最近,我们开发了一种合成α,α-乙烯桥连Bodipy二聚体的新策略;然而,其激发态动力学此前尚不清楚。这项工作展示了一种新型α,α-乙烯桥连Bodipy二聚体及其单体母体的超快激发态动力学。二聚体的稳态吸收和荧光表明单体单元的跃迁偶极矩(TDM)之间存在库仑相互作用,形成了通常所说的“J-二聚体”。使用分子激子理论和含时密度泛函理论(TD-DFT)研究了二聚体的激发态性质。我们基于其再现实验振子强度和共振拉曼光谱的能力选择了M06交换相关泛函(XCF)。超快激光光谱揭示了在极性溶剂中,二聚体中存在对称性破缺的电荷分离(SB-CS)以及随后电荷分离离子对态的布居。电荷分离速率处于正常范围,而电荷复合处于反转范围。相反,在非极性溶剂中,电荷分离在热力学上是不可行的。相比之下,单体的激发态动力学不依赖于溶剂极性。此外,无论失活途径如何,我们都没有发现光激发后发生显著结构重排的证据。在对电子跃迁进行广泛分析之后,我们得出结论,二聚体周围局部环境中的溶剂波动产生了一种不对称性,这种不对称性驱动并稳定了电荷分离。这项工作揭示了这组新分子系统中的电荷转移过程,以及如何通过结合实验和理论对激发态动力学进行建模。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ef4f/10476205/e4033b0dfff9/jp3c02978_0002.jpg

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