Osawa Masahisa, Soma Sakie, Hoshino Mikio, Tanaka Yuya, Akita Munetaka
Department of Applied Chemistry, Nippon Institute of Technology, Gakuendai 4-1, Miyashiro-Machi, Saitama 345-8501, Japan.
Laboratory for Chemistry and Life Science Institute of Innovative Research, Tokyo Institute of Technology R1-27, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan.
Dalton Trans. 2020 Nov 10;49(43):15204-15212. doi: 10.1039/d0dt03144e.
The gold(i) complexes [μ-LiPr(AuX)2] {X = Cl (1D), Br (2D), and I (3D); LiPr = 1,2-bis[bis(2-isopropylphenyl)phosphino]benzene} were synthesised to investigate the photoluminescence properties of dinuclear Au complexes comprising weak Au(i)-Au(i) bonds. Single crystals of the tetrahydrofuran (THF) adducts 1DOR, 2DOR, and 3DOR were obtained by recrystallisation of 1D, 2D, and 3D from a mixed solution of THF and n-hexane. These THF adducts afford orange emission, with peak wavelengths ranging from 597 to 630 nm, in the crystalline state at 293 K. Recrystallisation of 3D from a mixed solution of acetone and n-hexane afforded single crystals of the acetone adduct 3DGR, which exhibits blue-green emission at 293 K. No crystals of the acetone adduct were obtained from 1D and 2D. The emission spectra and lifetimes of 1DOR, 2DOR, 3DOR, and 3DGR measured in the temperature range 77-293 K indicate that emission from these complexes in the solid state is due to phosphorescence. Notably, although the molecular structure of 3D in the 3DOR crystal is near-similar to that of 3DGR, the phosphorescence spectrum of 3DOR differs markedly from that of 3DGR, with peak wavelengths at 597 and 506 nm, respectively. Theoretical studies revealed that (1) phosphorescence occurs via the electronic transition from the excited triplet state, which is mainly composed of halogen-to-metal-metal charge transfer and metal-centered transitions and (2) the T1-optimised structure of 3D in the 3DGR crystals differs markedly from that in 3DOR, and the differences in the phosphorescence colour observed between 3DGR and 3DOR are ascribed to the differences in their stabilised structures in the excited triplet state.
合成了金(I)配合物[μ-LiPr(AuX)₂] {X = Cl(1D)、Br(2D)和I(3D);LiPr = 1,2-双[双(2-异丙基苯基)膦基]苯},以研究包含弱金(I)-金(I)键的双核金配合物的光致发光性质。通过将1D、2D和3D从四氢呋喃(THF)和正己烷的混合溶液中重结晶,得到了四氢呋喃加合物1DOR、2DOR和3DOR的单晶。这些四氢呋喃加合物在293 K的晶体状态下发出橙色光,峰值波长范围为597至630 nm。将3D从丙酮和正己烷的混合溶液中重结晶,得到丙酮加合物3DGR的单晶,其在293 K时发出蓝绿色光。从1D和2D未得到丙酮加合物的晶体。在77 - 293 K温度范围内测量的1DOR、2DOR、3DOR和3DGR的发射光谱和寿命表明,这些配合物在固态下的发射是由于磷光。值得注意的是,尽管3DOR晶体中3D的分子结构与3DGR的近乎相似,但3DOR的磷光光谱与3DGR的明显不同,峰值波长分别为597和506 nm。理论研究表明:(1)磷光通过从激发三重态的电子跃迁发生,激发三重态主要由卤素到金属-金属电荷转移和金属中心跃迁组成;(2)3DGR晶体中3D的T1优化结构与3DOR中的明显不同,3DGR和3DOR之间观察到的磷光颜色差异归因于它们在激发三重态下稳定结构的差异。