Brooks Jason, Babayan Yelizaveta, Lamansky Sergey, Djurovich Peter I, Tsyba Irina, Bau Robert, Thompson Mark E
Department of Chemistry, University of Southern California, Los Angeles, California 90089-0744, USA.
Inorg Chem. 2002 Jun 17;41(12):3055-66. doi: 10.1021/ic0255508.
The synthesis, electrochemistry, and photophysics of a series of square planar Pt(II) complexes are reported. The complexes have the general structure C(wedge)NPt(O(wedge)O),where C(wedge)N is a monoanionic cyclometalating ligand (e.g., 2-phenylpyridyl, 2-(2'-thienyl)pyridyl, 2-(4,6-difluorophenyl)pyridyl, etc.) and O(wedge)O is a beta-diketonato ligand. Reaction of K(2)PtCl(4) with a HC(wedge)N ligand precursor forms the chloride-bridged dimer, C(wedge)NPt(mu-Cl)(2)PtC(wedge)N, which is cleaved with beta-diketones such as acetyl acetone (acacH) and dipivaloylmethane (dpmH) to give the corresponding monomeric C(wedge)NPt(O(wedge)O) complex. The thpyPt(dpm) (thpy = 2-(2'-thienyl)pyridyl) complex has been characterized using X-ray crystallography. The bond lengths and angles for this complex are similar to those of related cyclometalated Pt complexes. There are two independent molecular dimers in the asymmetric unit, with intermolecular spacings of 3.45 and 3.56 A, consistent with moderate pi-pi interactions and no evident Pt-Pt interactions. Most of the C(wedge)NPt(O(wedge)O) complexes display a single reversible reduction wave between -1.9 and -2.6 V (vs Cp(2)Fe/Cp(2)Fe(+)), assigned to largely C(wedge)N ligand based reduction, and an irreversible oxidation, assigned to predominantly Pt based oxidation. DFT calculations were carried out on both the ground (singlet) and excited (triplet) states of these complexes. The HOMO levels are a mixture of Pt and ligand orbitals, while the LUMO is predominantly C(wedge)N ligand based. The emission characteristics of these complexes are governed by the nature of the organometallic cyclometalating ligand allowing the emission to be tuned throughout the visible spectrum. Twenty-three different C(wedge)N ligands have been examined, which gave emission lambda(max) values ranging from 456 to 600 nm. Well-resolved vibronic fine structure is observed in all of the emission spectra (room temperature and 77 K). Strong spin-orbit coupling of the platinum atom allows for the formally forbidden mixing of the (1)MLCT with the (3)MCLT and (3)pi-pi states. This mixing leads to high emission quantum efficiencies (0.02-0.25) and lifetimes on the order of microseconds for the platinum complexes.
报道了一系列平面正方形Pt(II)配合物的合成、电化学和光物理性质。这些配合物具有通式C(楔)NPt(O(楔)O),其中C(楔)N是单阴离子环金属化配体(例如2-苯基吡啶基、2-(2'-噻吩基)吡啶基、2-(4,6-二氟苯基)吡啶基等),O(楔)O是β-二酮配体。K₂PtCl₄与HC(楔)N配体前体反应形成氯桥联二聚体C(楔)NPt(μ-Cl)₂PtC(楔)N,该二聚体用乙酰丙酮(acacH)和二苯甲酰甲烷(dpmH)等β-二酮裂解,得到相应的单体C(楔)NPt(O(楔)O)配合物。thpyPt(dpm)(thpy = 2-(2'-噻吩基)吡啶基)配合物已通过X射线晶体学表征。该配合物的键长和键角与相关环金属化Pt配合物的相似。不对称单元中有两个独立的分子二聚体,分子间间距为3.45和3.56 Å,符合适度的π-π相互作用且无明显的Pt-Pt相互作用。大多数C(楔)NPt(O(楔)O)配合物在-1.9至-2.6 V(相对于Cp₂Fe/Cp₂Fe⁺)之间显示出一个单一的可逆还原波,主要归因于基于C(楔)N配体的还原,以及一个不可逆氧化波,主要归因于基于Pt的氧化。对这些配合物的基态(单重态)和激发态(三重态)进行了密度泛函理论计算。最高占据分子轨道(HOMO)能级是Pt和配体轨道的混合,而最低未占据分子轨道(LUMO)主要基于C(楔)N配体。这些配合物的发射特性由有机金属环金属化配体的性质决定,使得发射能够在整个可见光谱范围内进行调节。已经研究了23种不同的C(楔)N配体,其发射λ(max)值范围为456至600 nm。在所有发射光谱(室温及77 K)中均观察到分辨率良好的振动精细结构。铂原子的强自旋-轨道耦合使得形式上禁阻的(¹MLCT)与(³MCLT)和(³π-π)态发生混合。这种混合导致铂配合物具有高发射量子效率(0.02 - 0.25)和微秒级的寿命。