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首页> 外文期刊>Polyhedron: The International Journal for Inorganic and Organometallic Chemistry >X-ray structure and DFT study of neutral mixed phosphine azoimine complexes of ruthenium
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X-ray structure and DFT study of neutral mixed phosphine azoimine complexes of ruthenium

机译:钌中性混合膦偶氮亚胺配合物的X射线结构和DFT研究

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Geometry optimization for a cis-[Ru~(II)(dppe)LCl_2] (1-8) {L = C_6H_5NNC(COCH_3)NAr, Ar = 2,4,6-trimethylphenyl (L_1), 2,5-dimethylphenyl (L_2), 4-tolyl (L_3), phenyl (L_4), 4-methoxyphenyl (L _5), 4-chlorophenyl (L_6), 4-nitrophenyl (L_7), 2,5-dichlorophenyl (L_8); dppe = Ph_2P(CH_2) _2PPh_2} was effected using the gaussian 03 protocol at density functional theory (DFT) B3LYP level with 6-31G/lanl2dz mixed basis. In addition, the complex cis-[Ru~(II)(dppe)L_3Cl_2] (3) has been further characterized by X-ray diffraction analysis. It was found that the optimized structure using 6-31G/lanl2dz has a large agreement with the X-ray data. DFT calculations show that upon solvation both Highest Occupied Molecular Orbital (HOMO) and Lowest Unoccupied Molecular Orbital (LUMO) molecular orbitals are stabilized and their energy gap is increased. TD-DFT calculations show that the intense broad band centered at λ_(max) ~ 506 nm is assigned to "mixed metal-ligand-to-ligand charge-transfer" (MMLLCT) while the weak low energy band centered on ~840 nm is assigned to the pure MLCT transition. The low intensity for the low energy MLCT transition can be explained by the large mixing between the azoimine (L) and (Ru(dπ)) orbital.
机译:顺式-[Ru〜(II)(dppe)LCl_2](1-8)的几何优化{L = C_6H_5NNC(COCH_3)NAr,Ar = 2,4,6-三甲基苯基(L_1),2,5-二甲基苯基( L_2),4-甲苯基(L_3),苯基(L_4),4-甲氧基苯基(L_5),4-氯苯基(L_6),4-硝基苯基(L_7),2,5-二氯苯基(L_8); dppe = Ph_2P(CH_2)_2PPh_2}是在密度泛函理论(DFT)B3LYP级别上以6-31G / lanl2dz混合基础使用高斯03协议实现的。另外,通过X射线衍射分析进一步表征了复杂的顺式[[Ru〜(II)(dppe)L_3Cl_2](3)。发现使用6-31G / lanl2dz的优化结构与X射线数据有很大的一致性。 DFT计算表明,溶剂化后,最高占据分子轨道(HOMO)和最低未占据分子轨道(LUMO)分子轨道都稳定了,并且它们的能隙增大了。 TD-DFT计算表明,以λ_(max)〜506 nm为中心的强宽带分配给“混合金属-配体-配体电荷转移”(MMLLCT),而以〜840 nm为中心的弱低能带为分配给纯MLCT过渡。低能量MLCT过渡的低强度可以通过偶氮亚胺(L)和(Ru(dπ))轨道之间的大量混合来解释。

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