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含杂环芳基乙炔配体的发光金(I)和金(III)配合物中荧光与磷光之间的相互作用

The interplay between fluorescence and phosphorescence with luminescent gold(i) and gold(iii) complexes bearing heterocyclic arylacetylide ligands.

作者信息

Chan Kaai Tung, Tong Glenna So Ming, To Wai-Pong, Yang Chen, Du Lili, Phillips David Lee, Che Chi-Ming

机构信息

State Key Laboratory of Synthetic Chemistry , Institute of Molecular Functional Materials , Department of Chemistry , The University of Hong Kong , Pokfulam Road , Hong Kong SAR , China . Email:

Department of Chemistry , The University of Hong Kong , Hong Kong , China.

出版信息

Chem Sci. 2017 Mar 1;8(3):2352-2364. doi: 10.1039/c6sc03775e. Epub 2016 Dec 5.

Abstract

The photophysical properties of a series of gold(i) [LAu(C[triple bond, length as m-dash]CR)] (L = PCy (), RNC (), NHC ()) and gold(iii) complexes [Au(C^N^C)(C[triple bond, length as m-dash]CR)] () bearing heterocyclic arylacetylide ligands with narrow band-gap are compared. The luminescence of both series are derived from an intraligand transition localized on the arylacetylide ligand (ππ*(C[triple bond, length as m-dash]CR)) but displayed prompt fluorescence ( = 2.7-12.0 ns) while showed mainly phosphorescence ( = 104-205 μs). The experimentally determined intersystem crossing (ISC) rate constants ( ) are on the order of 10 to 10 s for the gold(i) series () but 10 to 10 s for the gold(iii) analogues (). DFT/TDDFT calculations have been performed to help understand the difference in the between the two series of complexes. Owing to the different oxidation states of the gold ion, the Au(i) complexes have linear coordination geometry while the Au(iii) complexes are square planar. It was found from DFT/TDDFT calculations that due to this difference in coordination geometries, the energy gap between the singlet and triplet excited states (Δ ) with effective spin-orbit coupling (SOC) for Au(i) systems is much larger than that for the Au(iii) counterparts, thus resulting in the poor ISC efficiency for the former. Time-resolved spectroscopies revealed a minor contribution (<2.9%) of a long-lived delayed fluorescence (DF) ( = 4.6-12.5 μs) to the total fluorescence in . Attempts have been made to elucidate the mechanism for the origins of the DF: the dependence of the DF intensity with the power of excitation light reveals that triplet-triplet annihilation (TTA) is the most probable mechanism for the DF of while germinate electron-hole pair (GP) recombination accounts for the DF of in 77 K glassy solution (MeOH/EtOH = 4 : 1). Both and contain a BODIPY moiety at the acetylide ligand and display only IL(ππ*) fluorescence with negligible phosphorescence being observed. Computational analyses attributed this observation to the lack of low-lying triplet excited states that could have effective SOC with the S excited state.

摘要

比较了一系列带有窄带隙杂环芳基乙炔配体的金(I)[LAu(C≡CR)](L = PCy(),RNC(),NHC())和金(III)配合物[Au(C^N^C)(C≡CR)]()的光物理性质。这两个系列的发光均源自芳基乙炔配体(ππ*(C≡CR))上的配体内跃迁,但显示出即时荧光(τ = 2.7 - 12.0 ns),而显示出主要为磷光(τ = 104 - 205 μs)。实验测定的金(I)系列()的系间窜越(ISC)速率常数()在10⁶至10⁷ s⁻¹的范围内,而金(III)类似物()的ISC速率常数在10¹²至10¹³ s⁻¹的范围内。进行了DFT/TDDFT计算以帮助理解这两个系列配合物之间ISC的差异。由于金离子的氧化态不同,金(I)配合物具有线性配位几何结构,而金(III)配合物为平面正方形。从DFT/TDDFT计算中发现,由于这种配位几何结构的差异,对于具有有效自旋 - 轨道耦合(SOC)的金(I)体系,单重态和三重态激发态之间的能隙(ΔEST)比金(III)对应物的能隙大得多,因此导致前者的ISC效率较低。时间分辨光谱揭示了长寿命延迟荧光(DF)(τ = 4.6 - 12.5 μs)对中总荧光的贡献较小(<2.9%)。已尝试阐明DF起源的机制:DF强度对激发光功率的依赖性表明,三重态 - 三重态湮灭(TTA)是中DF最可能的机制,而在77 K玻璃态溶液(MeOH/EtOH = 4∶1)中,萌芽电子 - 空穴对(GP)复合是中DF的原因。和在乙炔配体处均含有一个BODIPY部分,并且仅显示IL(ππ*)荧光,观察到的磷光可忽略不计。计算分析将此观察结果归因于缺乏能够与S激发态具有有效SOC的低能三重态激发态。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f75c/5365001/86f9bbc495df/c6sc03775e-f1.jpg

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