Exploring Potential Energy Surfaces for Aggregation-Induced Emission-From Solution to Crystal

被引:131
作者
Crespo-Otero, Rachel [3 ]
Li, Quansong [4 ]
Blancafort, Lluis [1 ,2 ]
机构
[1] Univ Girona, Fac Ciencies, IQCC, CM A Capmany 69, Girona 17003, Spain
[2] Univ Girona, Fac Ciencies, Dept Quim, CM A Capmany 69, Girona 17003, Spain
[3] Queen Mary Univ London, Sch Biol & Chem Sci, Mile End Rd, London E1 4NS, England
[4] Beijing Inst Technol, Sch Chem & Chem Engn, South Zhongguancun St 5, Beijing 100081, Peoples R China
基金
英国工程与自然科学研究理事会;
关键词
aggregation-induced emission; conical intersections; fluorescence; intermolecular interactions; potential energy surfaces; ROOM-TEMPERATURE PHOSPHORESCENCE; INTRAMOLECULAR PROTON-TRANSFER; STATE DEACTIVATION MECHANISMS; DENSITY-FUNCTIONAL THEORY; CONICAL INTERSECTION; EXCITED-STATES; QUANTUM EFFICIENCY; AB-INITIO; PHOTOPHYSICS; DERIVATIVES;
D O I
10.1002/asia.201801649
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
Aggregation-induced emission (AIE) is a phenomenon where non-luminescent compounds in solution become strongly luminescent in aggregate and solid phase. It provides a fertile ground for luminescent applications that has rapidly developed in the last 15 years. In this review, we focus on the contributions of theory and computations to understanding the molecular mechanism behind it. Starting from initial models, such as restriction of intramolecular rotations (RIR), and the calculation of non-radiative rates with Fermi's golden rule (FGR), we center on studies of the global excited-state potential energy surfaces that have provided the basis for the restricted access to a conical intersection (RACI) model. In this model, which has been shown to apply for a diverse group of AIEgens, the lack of fluorescence in solution comes from radiationless decay at a CI in solution that is hindered in the aggregate state. We also highlight how intermolecular interactions modulate the photophysics in the aggregate phase, in terms of fluorescence quantum yield and emission color.
引用
收藏
页码:700 / 714
页数:15
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