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内笼胺功能化双膦基 Pt(II) 配合物的光物理性质作为发射金属环的模型。

Photophysical properties of endohedral amine-functionalized bis(phosphine) Pt(II) complexes as models for emissive metallacycles.

机构信息

Department of Chemistry, University of Utah, 315 South 1400 East, RM 2020, Salt Lake City, Utah 84412, United States.

出版信息

Inorg Chem. 2013 Aug 19;52(16):9254-65. doi: 10.1021/ic400491q. Epub 2013 Aug 2.

Abstract

The photophysical properties of bis(phosphine) Pt(II) complexes constructed from 2,6-bis(pyrid-3-ylethynyl) aniline and 2,6-bis(pyrid-4-ylethynyl) aniline vary significantly, even though the complexes differ only in the position of the coordinating nitrogen. By capping the ligands with an aryl bis(phosphine) Pt(II) metal acceptor, the photophysical properties of the two isomeric systems were directly compared, revealing that the low-energy absorption and emission bands of the two systems were separated by 30 nm (1804 cm(-1)) and 39 nm (1692 cm(-1)), respectively. From the analysis of time-dependent density functional (TD-DFT) calculations and excited-state lifetime measurements, it was determined that the nature of the Pt-N bond in the HOMO and the sums of the radiative (k(rad)) and nonradiative (k(nr)) rate constants were significantly different in the two systems. As the dominant nonradiative decay pathway in aniline systems is relaxation from the triplet state through intersystem crossing (ISC), the difference in k(nr) can be ascribed to changes in ISC between isomers of the bis(phosphine) Pt(II)-capped 2,6-bis(pyrid-3-ylethynyl) aniline system. It was also determined that the photophysical properties of these capped systems can be altered by functionalizing the aryl capping ligand on the bis(phosphine) Pt(II) metal center, which perturbs the molecular orbitals involved in the observed optical transitions. In addition, an isoelectronic bis(phosphine) Pd(II)-capped system was prepared for comparison with the bis(phosphine) Pt(II) suite of complexes. The Pd(II) system showed significant changes in its low-energy absorption band, but preserved the characteristic emissive properties of its Pt(II) analogue with an even higher quantum yield.

摘要

由 2,6-双(吡啶-3-乙炔基)苯胺和 2,6-双(吡啶-4-乙炔基)苯胺构建的双(膦)Pt(II)配合物的光物理性质有很大差异,尽管这些配合物仅在配位氮原子的位置上有所不同。通过用芳基双(膦)Pt(II)金属受体封端配体,可以直接比较两个异构体系的光物理性质,结果表明,两个体系的低能吸收带和发射带分别分离 30nm(1804cm(-1))和 39nm(1692cm(-1))。通过时间依赖密度泛函(TD-DFT)计算和激发态寿命测量的分析,确定在两个体系中,HOMO 中的 Pt-N 键的性质以及辐射(k(rad))和非辐射(k(nr))速率常数之和有很大差异。由于苯胺体系中主要的非辐射衰减途径是通过系间窜越(ISC)从三重态弛豫,因此 k(nr)的差异可以归因于双(膦)Pt(II)封端的 2,6-双(吡啶-3-乙炔基)苯胺体系异构体之间的 ISC 变化。还确定了这些封端体系的光物理性质可以通过官能化双(膦)Pt(II)金属中心上的芳基封端配体来改变,这会干扰参与观察到的光学跃迁的分子轨道。此外,还制备了等电子双(膦)Pd(II)封端体系以与双(膦)Pt(II)配合物系列进行比较。Pd(II)体系在其低能吸收带中显示出显著变化,但保留了与其 Pt(II)类似物的特征发光性质,量子产率更高。

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