Fujimoto Yushi, Mochiduki Yoshifumi, Sotome Hikaru, Shimada Rintaro, Okajima Hajime, Toda Yasunori, Sakamoto Akira, Miyasaka Hiroshi, Ito Fuyuki
Department of Chemistry, Graduate School of Science and Technology, Shinshu University, 3-1-1, Asahi, Matsumoto, Nagano 390-8621, Japan.
Department of Chemistry, Institute of Education, Shinshu University, 6-Ro, Nishinagano, Nagano 380-8544, Japan.
J Am Chem Soc. 2024 Nov 27;146(47):32529-32538. doi: 10.1021/jacs.4c10277. Epub 2024 Nov 17.
Organic molecules with an aggregation-induced emission (AIE) property have been attracting much attention from the viewpoint of application to solid state emissive materials. For the AIE mechanism, quantum mechanical studies proposed the restriction of the intramolecular motion (RIM) model with the contribution of the conical intersection (CI) and deduced the importance of the restricted access to a conical intersection (RACI) in the potential energy surface (PES). Although these theoretical studies have contributed to the elucidation of AIE phenomena, direct detection of the reaction dynamics is indispensable to clarify the actual PES and the deactivation mechanism. Along this line, we investigated excited state dynamics of the AIE molecule with dibenzoylmethanatoboron difluoride complexes using time-resolved absorption spectroscopies in both visible and infrared (IR) regions. While the reference system of 1,3-bis(4-methoxyphenyl)methanatoboron difluoride (2aBF) showed strong emission in solution, the methyl-substituted derivative at the α-position of the dioxaborine ring (2amBF) led to the very weak fluorescence in solution but strong emission in the solid state. Time-resolved visible absorption measurements revealed a peak shift and broadening of the stimulated emission in the solution of 2amBF, owing to the rapid change of the molecular geometry. With the temporal evolution of time-resolved IR absorption signals and density functional theory (DFT) calculation of these systems, it was deduced that 2amBF has two stable geometries, namely, planar and bending, in the S state and the bending geometry in the S state led to rapid conversion to the S state. These results support the RACI model in the aggregated states, leading to the AIE properties.
从应用于固态发光材料的角度来看,具有聚集诱导发光(AIE)特性的有机分子一直备受关注。对于AIE机制,量子力学研究提出了分子内运动受限(RIM)模型,并考虑了锥形交叉(CI)的贡献,还推导出了势能面(PES)中受限进入锥形交叉(RACI)的重要性。尽管这些理论研究有助于阐明AIE现象,但直接检测反应动力学对于明确实际的PES和失活机制是必不可少的。沿着这条线,我们使用可见和红外(IR)区域的时间分辨吸收光谱研究了二苯甲酰甲烷合硼二氟配合物的AIE分子的激发态动力学。虽然1,3-双(4-甲氧基苯基)甲烷合硼二氟(2aBF)的参考体系在溶液中表现出强烈的发射,但二氧硼杂环α位的甲基取代衍生物(2amBF)在溶液中导致非常弱的荧光,但在固态中发射很强。时间分辨可见吸收测量表明,由于分子几何形状的快速变化,2amBF溶液中受激发射出现峰移和展宽。随着时间分辨红外吸收信号的时间演化以及这些体系的密度泛函理论(DFT)计算,推断出2amBF在S态有两种稳定的几何形状,即平面和弯曲形状,并且S态的弯曲几何形状导致快速转换为S态。这些结果支持了聚集态下的RACI模型,从而导致了AIE特性。