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非常小的发射量子产率是钌(II)-(受体配体)发色团纯金属到配体电荷转移激发态的特征吗?

Are Very Small Emission Quantum Yields Characteristic of Pure Metal-to-Ligand Charge-Transfer Excited States of Ruthenium(II)-(Acceptor Ligand) Chromophores?

作者信息

Tsai Chia Nung, Mazumder Shivnath, Zhang Xiu Zhu, Schlegel H Bernhard, Chen Yuan Jang, Endicott John F

机构信息

Department of Chemistry, Fu-Jen Catholic University , New Taipei City 24205, Taiwan, Republic of China.

Department of Chemistry, Wayne State University , Detroit, Michigan 48202, United States.

出版信息

Inorg Chem. 2016 Aug 1;55(15):7341-55. doi: 10.1021/acs.inorgchem.6b00374. Epub 2016 Jul 20.

Abstract

Metal to ligand charge-transfer (MLCT) excited state emission quantum yields, ϕem, are reported in 77 K glasses for a series of pentaammine and tetraammine ruthenium(II) complexes with monodentate aromatic acceptor ligands (Ru-MDA) such as pyridine and pyrazine. These quantum yields are only about 0.2-1% of those found for their Ru-bpy (bpy = 2,2'-bipyridine) analogs in similar excited state energy ranges (hνem). The excited state energy dependencies of the emission intensity are characterized by mean radiative decay rate constants, kRAD, resolved from ϕem/τobs = kRAD (τobs = the observed emission decay lifetime; τobs(-1) = kRAD + kNRD; kNRD = nonradiative decay rate constant). Except for the Ru-pz chromophores in alcohol glasses, the values of kNRD for the Ru-MDA chromophores are slightly smaller, and their dependences on excited state energies are very similar to those of related Ru-bpy chromophores. In principle, one expects kRAD to be proportional to the product of (hνem)(3) and the square of the transition dipole moment (Me,g).(2) However, from experimental studies of Ru-bpy chromophores, an additional hνem dependence has been found that originates in an intensity stealing from a higher energy excited state with a much larger value of Me,g. This additional hνem dependence is not present in the kRAD energy dependence for Ru-MDA chromophores in the same energy regime. Intensity stealing in the phosphorescence of these complexes is necessary since the triplet-to-singlet transition is only allowed through spin-orbit coupling and since the density functional theory modeling implicates configurational mixing between states in the triplet spin manifold; this is treated by setting Me,g equal to the product of a mixing coefficient and the difference between the molecular dipole moments of the states involved, which implicates an experimental first order dependence of kRAD on hνem. The failure to observe intensity stealing for the Ru-MDA complexes suggests that their weak emissions are more typical of "pure" (or unmixed) (3)MLCT excited states.

摘要

在77K玻璃中,报道了一系列含有单齿芳族受体配体(Ru-MDA)(如吡啶和吡嗪)的五氨和四氨钌(II)配合物的金属到配体电荷转移(MLCT)激发态发射量子产率ϕem。这些量子产率仅约为在相似激发态能量范围(hνem)中其Ru-bpy(bpy = 2,2'-联吡啶)类似物的量子产率的0.2 - 1%。发射强度的激发态能量依赖性由平均辐射衰减速率常数kRAD表征,kRAD由ϕem/τobs = kRAD解析得出(τobs = 观测到的发射衰减寿命;τobs(-1) = kRAD + kNRD;kNRD = 非辐射衰减速率常数)。除了醇玻璃中的Ru-pz发色团外,Ru-MDA发色团的kNRD值略小,并且它们对激发态能量的依赖性与相关Ru-bpy发色团的依赖性非常相似。原则上,人们预期kRAD与(hνem)(3)和跃迁偶极矩(Me,g)(2)的平方的乘积成正比。然而,从Ru-bpy发色团的实验研究中发现了一种额外的hνem依赖性,其源于从具有大得多的Me,g值的更高能量激发态的强度窃取。在相同能量范围内,Ru-MDA发色团的kRAD能量依赖性中不存在这种额外的hνem依赖性。这些配合物磷光中的强度窃取是必要的,因为三重态到单重态的跃迁仅通过自旋 - 轨道耦合才被允许,并且因为密度泛函理论建模暗示了三重态自旋流形中态之间的构型混合;这通过将Me,g设定为混合系数与所涉及态的分子偶极矩之差的乘积来处理,这暗示了kRAD对hνem的实验一级依赖性。未观察到Ru-MDA配合物的强度窃取表明它们的弱发射更典型地代表“纯”(或未混合)的(3)MLCT激发态。

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