首页> 外文期刊>Inorganic Chemistry: A Research Journal that Includes Bioinorganic, Catalytic, Organometallic, Solid-State, and Synthetic Chemistry and Reaction Dynamics >Computational modeling of the triplet metal-to-ligand charge-transfer excited-state structures of mono-bipyridine-ruthenium(II) complexes and comparisons to their 77 K emission band shapes
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Computational modeling of the triplet metal-to-ligand charge-transfer excited-state structures of mono-bipyridine-ruthenium(II) complexes and comparisons to their 77 K emission band shapes

机译:双联吡啶-钌(II)配合物的三重态金属-配体电荷转移激发态结构的计算模型及其与77 K发射带形状的比较

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摘要

A computational approach for calculating the distortions in the lowest energy triplet metal to ligand charge-transfer (~3MLCT = T _0) excited states of ruthenium(II)-bipyridine (Ru-bpy) complexes is used to account for the patterns of large variations in vibronic sideband amplitudes found in the experimental 77 K emission spectra of complexes with different ancillary ligands (L). Monobipyridine, [Ru(L)_4bpy] ~(m+) complexes are targeted to simplify analysis. The range of known emission energies for this class of complexes is expanded with the 77 K spectra of the complexes with (L)_4 = bis-acetonylacetonate (emission onset at about 12 000 cm~(-1)) and 1,4,8,11-tetrathiacyclotetradecane and tetrakis-acetonitrile (emission onsets at about 21 000 cm~(-1)); no vibronic sidebands are resolved for the first of these, but they dominate the spectra of the last two. The computational modeling of excited-state distortions within a Franck-Condon approximation indicates that there are more than a dozen important distortion modes including metal-ligand modes (low frequency; lf) as well as predominately bpy modes (medium frequency; mf), and it simulates the observed 77 K emission spectral band shapes of selected complexes very well. This modeling shows that the relative importance of the mf modes increases very strongly as the T_0 energy increases. Furthermore, the calculated metal-centered SOMOs show a substantial bpy-π-orbital contribution for the complexes with the highest energy T0. These features are attributed to configurational mixing between the diabatic MLCT and the bpy ~3ππ* excited states at the highest T_0 energies.
机译:一种用于计算钌(II)-联吡啶(Ru-bpy)配合物的最低能级三重态金属向配体电荷转移(〜3MLCT = T _0)激发态的畸变的计算方法来解释大变化的模式在具有不同辅助配体的配合物的实验77 K发射光谱中发现的电子振动边带振幅(L)。单联吡啶,[Ru(L)_4bpy]〜(m +)配合物可简化分析。这类配合物的已知发射能范围随着配合物的77 K光谱而扩大,其中(L)_4 =双-丙酮基丙酮酸酯(在约12000 cm〜(-1)处开始发射)和1,4,8 ,11-四硫代环十四烷和四-乙腈(发射开始于约21 000 cm〜(-1));对于其中的第一个,没有解决任何振动边带,但它们主导了后两个的光谱。 Franck-Condon近似内的激发态畸变的计算模型表明,有十多种重要的畸变模式,包括金属配体模式(低频; lf​​)以及主要为bpy模式(中频; mf),以及它很好地模拟了所选配合物的77 K发射光谱带形状。该模型表明,随着T_0能量的增加,mf模式的相对重要性非常强烈地增加。此外,计算得出的以金属为中心的SOMOs对具有最高能量T0的配合物表现出重要的bpy-π-轨道贡献。这些特征归因于非绝热MLCT和最高T_0能量下的bpy〜3ππ*激发态之间的结构混合。

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