Institute of Molecular Functional Materials and Department of Chemistry, The University of Hong Kong, Pokfulam Road, Hong Kong, People's Republic of China.
Inorg Chem. 2010 Dec 6;49(23):10930-9. doi: 10.1021/ic101271d. Epub 2010 Nov 9.
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.
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。