Kender William T, Turro Claudia
Department of Chemistry and Biochemistry , The Ohio State University , Columbus , Ohio 43210 , United States.
J Phys Chem A. 2019 Apr 4;123(13):2650-2660. doi: 10.1021/acs.jpca.9b00858. Epub 2019 Mar 21.
A series of six [Ru(bpy)(NHC-R)] complexes were synthesized and characterized, where bpy = 2,2'-bipyridine and NHC-R is an N-heterocyclic carbene covalently linked to a carbanion with a number of substituents, R = -OMe (1), -Me (2), -H (3), -Cl (4), -COEt (5), and -NO (6). The effects of these strongly σ-donating NHC-R ligands on the ground-state electronic structure and on the excited-state character and dynamics were probed using electrochemistry, TD-DFT calculations, and steady-state absorption and emission spectroscopies, along with ultrafast transient absorption and time-resolved IR measurements. The excitation of 1-5 with a 400 nm pulse (irf = 85 fs) results in the population of a high energy singlet state, S, that rapidly intersystem crosses into a high-lying triplet state, T. Over the course of 7-22 ps, T relaxes to the lowest lying triplet state, T, which is metal/ligand-to-ligand charge transfer, Ru(d)/NHC(π) → bpy(π*) in character. These ML-LCT states decay to regenerate the ground state with lifetimes, τ, that range from <8 to 15 ns at 298 K and from 10 to 23 ns at 77 K in CHCN. Both the excited-state lifetime at 77 K and the T → T rate of internal conversion of 1-5 are dependent on the substituent R, and the latter correlates with the Hammett parameter (σ) of the NHC-R ligand. Excitation of 1-5 with low energy light, 550-670 nm, does not result in the population of T, as only T is observed. In the case of 6, excitation is expected to populate a Ru(d)/NHC(π) → NHC(π*) state localized on the NHC-NO ligand, which decays to a higher energy Ru(d)/NHC(π) → NHC(π*) state followed by internal conversion to the Ru(d)/NHC(π) → bpy(π*) T state with τ = 250 ps; the population of both states is independent of excitation wavelength in 6. This work demonstrates that the introduction of one NHC-R ligand in these complexes permits the population of a higher energy triplet state that decays to T in the picosecond time range. The relatively slow T → T internal conversion in these complexes makes the population of the higher-energy state potentially useful for more efficient charge injection into semiconductors for solar energy conversion or to aid in accessing dissociative metal-centered states for drug delivery. Overall, this work shows the ability to synthetically access valuable excited-state dynamics using the two different Ru-C bonds of the asymmetric NHC-R ligands.
合成并表征了一系列六种[Ru(bpy)(NHC-R)]配合物,其中bpy = 2,2'-联吡啶,NHC-R是一种与带有多个取代基的碳负离子共价连接的N-杂环卡宾,R = -OMe(1)、-Me(2)、-H(3)、-Cl(4)、-COEt(5)和-NO(6)。使用电化学、TD-DFT计算、稳态吸收和发射光谱,以及超快瞬态吸收和时间分辨红外测量,探究了这些强σ供体NHC-R配体对基态电子结构、激发态性质和动力学的影响。用400 nm脉冲(irf = 85 fs)激发1-5会导致高能单重态S的布居,该单重态迅速通过系间窜越进入高位三重态T。在7-22 ps的过程中,T弛豫到最低位三重态T,其特征是金属/配体到配体的电荷转移,即Ru(d)/NHC(π) → bpy(π*)。这些ML-LCT态衰变以再生基态,其寿命τ在298 K时范围为<8至15 ns,在77 K时在CHCN中为10至23 ns。77 K时的激发态寿命以及1-5的T → T内转换速率均取决于取代基R,且后者与NHC-R配体的哈米特参数(σ)相关。用低能光550-670 nm激发1-5不会导致T的布居,因为仅观察到了T。对于6,预计激发会使位于NHC-NO配体上的Ru(d)/NHC(π) → NHC(π*)态布居,该态衰变为更高能量的Ru(d)/NHC(π) → NHC(π*)态,随后通过内转换变为Ru(d)/NHC(π) → bpy(π*) T态,τ = 250 ps;在6中,这两种态的布居均与激发波长无关。这项工作表明,在这些配合物中引入一个NHC-R配体可使更高能量的三重态布居,该三重态在皮秒时间范围内衰变为T。这些配合物中相对较慢的T → T内转换使得更高能态的布居对于更有效地向用于太阳能转换的半导体中注入电荷或有助于进入用于药物递送的离解性金属中心态可能是有用的。总体而言,这项工作展示了利用不对称NHC-R配体的两种不同Ru-C键合成获得有价值的激发态动力学的能力。