Kaufmann Martin, Müller Carolin, Cullen Aoibhin A, Brandon Michael P, Dietzek Benjamin, Pryce Mary T
School of Chemical Sciences, National Centre for Sensor Research, Dublin City University, Dublin 9, Ireland.
Institute of Physical Chemistry and Abbe Center of Photonics, Friedrich Schiller University Jena, Helmholtzweg 4, Jena 07743, Germany.
Inorg Chem. 2021 Jan 18;60(2):760-773. doi: 10.1021/acs.inorgchem.0c02765. Epub 2020 Dec 23.
Transition-metal-based donor-acceptor systems can produce long-lived excited charge-transfer states by visible-light irradiation. The novel ruthenium(II) polypyridyl type complexes and based on the dipyridophenazine ligand () directly linked to 4-hydroxythiazoles of different donor strengths were synthesized and photophysically characterized. The excited-state dynamics were investigated by femtosecond-to-nanosecond transient absorption and nanosecond emission spectroscopy complemented by time-dependent density functional theory calculations. These results indicate that photoexcitation in the visible region leads to the population of both metal-to-ligand charge-transfer (MLCT) and thiazole (tz)-induced intraligand charge-transfer (ILCT) states. Thus, the excited-state dynamics is described by two excited-state branches, namely, the population of (i) a comparably short-lived phenazine-centered MLCT state (τ ≈ 150-400 ps) and (ii) a long-lived ILCT state (τ ≈ 40-300 ns) with excess charge density localized on the phenazine and tz moieties. Notably, the ruthenium(II) complexes feature long-lived dual emission with lifetimes in the ranges τ ≈ 40-300 ns and τ ≈ 100-200 ns, which are attributed to emission from the ILCT and MLCT manifolds, respectively.
基于过渡金属的供体-受体体系通过可见光照射可产生长寿命的激发电荷转移态。合成了基于与不同供体强度的4-羟基噻唑直接相连的二吡啶并菲嗪配体()的新型钌(II)多吡啶型配合物和,并对其进行了光物理表征。通过飞秒到纳秒瞬态吸收和纳秒发射光谱,并结合含时密度泛函理论计算,研究了激发态动力学。这些结果表明,可见光区域的光激发导致金属到配体电荷转移(MLCT)和噻唑(tz)诱导的配体内电荷转移(ILCT)态的形成。因此,激发态动力学由两个激发态分支描述,即(i)寿命相对较短的以二吡啶并菲嗪为中心的MLCT态(τ≈150 - 400 ps)和(ii)寿命较长的ILCT态(τ≈40 - 300 ns),其多余电荷密度定域在二吡啶并菲嗪和tz部分。值得注意的是,钌(II)配合物具有长寿命的双重发射,寿命范围分别为τ≈40 - 300 ns和τ≈100 - 200 ns,分别归因于ILCT和MLCT流形的发射。