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双核铂(II)A 型炔基二膦配合物的光物理性质和 NMR 流动性的计算研究。

Computational studies on the photophysical properties and NMR fluxionality of dinuclear platinum(II) A-frame alkynyl diphosphine complexes.

机构信息

Institute of Molecular Functional Materials and Department of Chemistry, The University of Hong Kong, Pokfulam Road, Hong Kong, People's Republic of China.

出版信息

Inorg Chem. 2010 Dec 6;49(23):10930-9. doi: 10.1021/ic101271d. Epub 2010 Nov 9.

Abstract

The structural geometry, electronic structure, photophysical properties, and the fluxional behavior of a series of A-frame diplatinum alkynyl complexes, Pt(2)(μ-dppm)(2)(μ-C≡CR)(C≡CR)(2) [R = (t)Bu (1), C(6)H(5) (2), C(6)H(4)Ph-p (3), C(6)H(4)Et-p (4), C(6)H(4)OMe-p (5); dppm = bis(diphenylphosphino)methane], have been studied by density functional theory (DFT) and time-dependent TD-DFT associated with conductor-like polarizable continuum model (CPCM) calculations. The results show that the Pt···Pt distance strongly depends on the binding mode of the alkynyl ligands. A significantly shorter Pt···Pt distance is found in the symmetrical form, in which the bridging alkynyl ligand is σ-bound to the two metal centers, than in the unsymmetrical form where the alkynyl ligand is σ-bound to one metal and π-bound to another. For the two structural forms in 1-5, both the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) energy levels show a dependence on the nature of the substituents attached to the alkynyl ligand. The energies of the HOMO and LUMO are found to increase and decrease, respectively, from R = (t)Bu to R = Ph and to R = C(6)H(4)Ph-p, because of the increase of the π- conjugation of the alkynyl ligand. On the basis of the TDDFT/CPCM calculations, the low-energy absorption band consists of two types of transitions, which are ligand-to-ligand charge-transfer (LLCT) [π(alkynyl) → σ*(dppm)]/metal-centered MC [dσ*(Pt(2)) → pσ(Pt(2))] transitions as well as interligand π → π* transition from the terminal alkynyl ligands to the bridging alkynyl ligand mixed with metal-metal-to-ligand charge transfer MMLCT [dσ*(Pt(2)) → π*(bridging alkynyl)] transition. The latter transition is lower in energy than the former. The calculation also indicates that the emission for the complexes originates from the triplet interligand π(terminal alkynyls) → π*(bridging alkynyl)/MMLCT [dσ*(Pt(2)) → π*(bridging alkynyl)] excited state. In terms of the fluxional behavior, calculations have been performed to study the details of the mechanisms for the three fluxional processes, which are the σ,π-alkynyl exchange, the ring-flipping, and the bridging-to-terminal alkynyl exchange processes.

摘要

已通过密度泛函理论(DFT)和与导体相似的极化连续模型(CPCM)相关的时间相关 TD-DFT 对一系列 A 型二价铂炔基配合物Pt(2)(μ-dppm)(2)(μ-C≡CR)(C≡CR)(2) [R = (t)Bu(1), C(6)H(5)(2), C(6)H(4)Ph-p(3), C(6)H(4)Et-p(4), C(6)H(4)OMe-p(5); dppm = 双(二苯基膦)甲烷]的结构几何形状、电子结构、光物理性质和动态行为进行了研究。结果表明,Pt···Pt 距离强烈依赖于炔基配体的结合模式。在对称形式中发现 Pt···Pt 距离明显较短,其中桥接炔基配体与两个金属中心形成σ键,而在不对称形式中,炔基配体与一个金属形成σ键,与另一个形成π键。对于 1-5 中的两种结构形式,最高占据分子轨道(HOMO)和最低未占据分子轨道(LUMO)能级都表现出对炔基配体上所连接取代基性质的依赖性。由于炔基配体的π共轭增加,HOMO 和 LUMO 的能量分别增加和减少。基于 TDDFT/CPCM 计算,低能量吸收带由两种类型的跃迁组成,即配体到配体电荷转移(LLCT)[π(炔基)→σ*(dppm)]/金属中心 MC [dσ*(Pt(2)) → pσ(Pt(2))]跃迁以及来自末端炔基配体到桥接炔基配体的配体间π→π跃迁,混合金属-金属到配体电荷转移 MMLCT [dσ(Pt(2)) → π*(桥接炔基)]跃迁。后一种跃迁的能量低于前一种跃迁。该计算还表明,配合物的发射源自三重态配体间π(末端炔基)→π*(桥接炔基)/MMLCT [dσ*(Pt(2)) → π*(桥接炔基)]激发态。就动态行为而言,已经进行了计算以研究三种动态过程(σ,π-炔基交换、环翻转和桥接到末端炔基交换过程)的机制细节。

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