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极性染料聚集体:超越激子模型

Aggregates of polar dyes: beyond the exciton model.

作者信息

Anzola Mattia, Painelli Anna

机构信息

Department of Chemistry, Life Science and Environmental Sustainability, University of Parma, 43124 Parma, Italy.

出版信息

Phys Chem Chem Phys. 2021 Apr 14;23(14):8282-8291. doi: 10.1039/d1cp00335f. Epub 2021 Mar 29.

Abstract

The physics of aggregates of polar and polarizable donor-acceptor dyes is discussed, extending a previous model to account for the coupling of electronic and vibrational degrees of freedom. Fully exploiting translational symmetry, exact absorption and fluorescence spectra are calculated for aggregates with up to 6 molecules. A two-step procedure is presented: in the first step, a mean-field solution of the problem is proposed to define the excitonic basis via a rotation of the electronic basis. The rotation is also accompanied by a Lang-Firsov transformation of the vibrational basis. In the second step, the aggregate Hamiltonian, written on the exciton basis, is diagonalized towards exact results. The procedure leads to a reduction of the dimension of the problem, since, at least for weak coupling, only states with up to 3 excitons are needed to obtain reliable results. More interestingly, the mean-field solution represents the proper reference state to discuss excitonic and ultraexcitonic effects. The emerging picture demonstrates that the exciton model offers a reliable description of aggregates of polar and polarizable dyes in the weak coupling regime, while ultraexcitonic effects are important in the medium-strong coupling regimes, and particularly so for J-aggregates where ultraexcitonic effects show up most clearly with multistability and multiexciton generation.

摘要

本文讨论了极性和可极化供体 - 受体染料聚集体的物理性质,扩展了先前的模型以考虑电子和振动自由度的耦合。充分利用平移对称性,计算了多达6个分子的聚集体的精确吸收光谱和荧光光谱。本文提出了一个两步过程:第一步,提出问题的平均场解,通过电子基的旋转来定义激子基。这种旋转还伴随着振动基的朗 - 菲尔索夫变换。第二步,在激子基上写出的聚集体哈密顿量被对角化以得到精确结果。该过程导致问题维度的降低,因为至少对于弱耦合,只需要考虑最多3个激子的状态就能得到可靠结果。更有趣的是,平均场解代表了讨论激子和超激子效应的合适参考态。新出现的情况表明,激子模型在弱耦合 regime 中为极性和可极化染料的聚集体提供了可靠的描述,而超激子效应在中强耦合 regime 中很重要,特别是对于J - 聚集体,其中超激子效应在多稳定性和多激子产生中表现得最为明显。

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