NRW Graduate School of Chemistry, University of Münster , D-48149 Münster, Germany.
Inorg Chem. 2013 Oct 7;52(19):10756-65. doi: 10.1021/ic302695q. Epub 2013 Sep 9.
We report on the photophysical studies of two cationic near-UV emitters based on bis-pincer Ir(III) carbene complexes: [Ir(nBu)(C(NHC)(Me)CC(NHC))2]X, where Ir(nBu)(C(NHC)(Me)CC(NHC)) is (4,6-dimethyl-1,3-phenylene-κC(2))bis(1-butylimidazol-2-ylidene) and X = I(-) or PF6(-)). The compounds are highly emitting in deaerated CH3CN solution with emission maxima at 384 and 406 nm, and photoluminescence quantum yields of 0.41 and 0.38, for [Ir(nBu)(C(NHC)(Me)CC(NHC))2]I and Ir(nBu)(C(NHC)(Me)CC(NHC))2]PF6, respectively. In order to gain deeper understandings into their structural and electronic features, as well as to ascertain the nature of the excited states involved into the electronic absorption processes, density functional theory (DFT) and time-dependent DFT (TD-DFT) calculations have been performed on the ground and excited states of the closely related complex Ir(Me)(C(NHC)(Me)CC(NHC))2. In the solid state, an emission at low energy is observed (λ(max) = 500 nm) for both complexes. However, the intensity of the emission at high energy versus the intensity of the new emission at low energy is dependent on the nature of counterions. The origin of this emission is not completely clear, but the experimental data point to the formation of trapping sites induced by aggregation processes involving the interaction between the cationic emitter and the counterion.
我们报告了基于双膦 Ir(III)卡宾配合物的两种阳离子近紫外发射体的光物理研究:[Ir(nBu)(C(NHC)(Me)CC(NHC))2]X,其中 Ir(nBu)(C(NHC)(Me)CC(NHC))是(4,6-二甲基-1,3-亚苯基-κC(2))双(1-丁基咪唑-2-亚基),X = I(-)或 PF6(-)。这些化合物在无氧 CH3CN 溶液中高度发光,发射最大值为 384nm 和 406nm,光致发光量子产率分别为 0.41 和 0.38,对于[Ir(nBu)(C(NHC)(Me)CC(NHC))2]I 和 Ir(nBu)(C(NHC)(Me)CC(NHC))2]PF6。为了更深入地了解它们的结构和电子特性,并确定参与电子吸收过程的激发态的性质,对密切相关的配合物Ir(Me)(C(NHC)(Me)CC(NHC))2的基态和激发态进行了密度泛函理论(DFT)和时间相关 DFT(TD-DFT)计算。在固态中,两种配合物都观察到低能发射(λ(max)=500nm)。然而,高能发射的强度与低能新发射的强度之比取决于抗衡离子的性质。这种发射的起源尚不完全清楚,但实验数据表明,阳离子发射体与抗衡离子之间的相互作用引起的聚集过程形成了陷阱位。