Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan.
Inorg Chem. 2010 Jan 18;49(2):531-40. doi: 10.1021/ic9015788.
New sulfide-capped octahedral hexarhenium(III) complexes containing 4-phenylpyridine (ppy) or 1,2-bis(4-pyridyl)ethane (bpe) ((n-C(4)H(9))(4)N)[mer-{Re(6)S(8)Cl(3)(ppy)(3)}] ((Bu(4)N)[1]), ((n-C(4)H(9))(4)N)(2)[trans-{Re(6)S(8)Cl(4)(ppy)(2)}] ((Bu(4)N)(2)[2a]), ((n-C(4)H(9))(4)N)(2)[cis-{Re(6)S(8)Cl(4)(ppy)(2)}] ((Bu(4)N)(2)[2b]), ((n-C(4)H(9))(4)N)(2)[trans-{Re(6)S(8)Cl(4)(bpe)(2)}] ((Bu(4)N)(2)[3a]), and ((n-C(4)H(9))(4)N)(2)[cis-{Re(6)S(8)Cl(4)(bpe)(2)}] ((Bu(4)N)(2)[3b]) were prepared, and X-ray single-crystal structure determination was carried out for (Bu(4)N)(2)[2a] and (Bu(4)N)(2)[3a]. The photophysical properties of these complexes were studied both in acetonitrile at 298 K and in the solid state at 298 and 80 K, along with those of the known 4,4'-bipyridine (bpy) analogues ((n-C(4)H(9))(4)N)[mer-{Re(6)S(8)Cl(3)(bpy)(3)}] ((Bu(4)N)[4]), ((n-C(4)H(9))(4)N)(2)[trans-{Re(6)S(8)Cl(4)(bpy)(2)}] ((Bu(4)N)(2)[5a]), and ((n-C(4)H(9))(4)N)(2)[cis-{Re(6)S(8)Cl(4)(bpy)(2)}] ((Bu(4)N)(2)[5b]). The photophysical data of 5a and 5b in solution and in the solid state were significantly different from those of other complexes. On the basis of experimental observations of 2a and 5a and density-functional theory (DFT) calculations, it was concluded that 5a and 5b exhibited metal (Re(6)S(8) core)-to-ligand (bpy) charge transfer (MLCT) type emission. This is the first unambiguous demonstration of MLCT type emissions for the hexarhenium complexes. The MLCT components, where present, are only minor in the case of the emissions of 1, 2a, 2b, and 4; these can be explained primarily as the contributions of the intracore electronic transitions. The emissions of 3a and 3b can be assigned almost completely to the electronic transitions within the Re(6)S(8) core. The different emission characteristics of the bis(bpy) complexes (5a and 5b) from the tris(bpy) complex (4) are a result of the increase in the number of nitrogen donors on the Re(6)S(8) core, which stabilizes the Re(6)S(8) core energy to a lower level than the energy of the bpy ligand pi* orbital. On the other hand, it has been shown that the emissions of the bis(ppy) (2a and 2b) and bis(bpe) complexes (3a and 3b) are best characterized by the higher pi* energy level of each N-heteroaromatic ligand, which lead to a stronger metal character in the emissive excited state of the complex.
新的含 4-苯基吡啶 (ppy) 或 1,2-双(4-吡啶基)乙烷 (bpe) 的八面体六铼(III)配合物 ((n-C(4)H(9))(4)N)[mer-{Re(6)S(8)Cl(3)(ppy)(3)}] ((Bu(4)N)[1])、((n-C(4)H(9))(4)N)(2)[trans-{Re(6)S(8)Cl(4)(ppy)(2)}] ((Bu(4)N)(2)[2a])、((n-C(4)H(9))(4)N)(2)[cis-{Re(6)S(8)Cl(4)(ppy)(2)}] ((Bu(4)N)(2)[2b])、((n-C(4)H(9))(4)N)(2)[trans-{Re(6)S(8)Cl(4)(bpe)(2)}] ((Bu(4)N)(2)[3a]) 和 ((n-C(4)H(9))(4)N)(2)[cis-{Re(6)S(8)Cl(4)(bpe)(2)}] ((Bu(4)N)(2)[3b]) 被制备出来,并对 (Bu(4)N)(2)[2a] 和 (Bu(4)N)(2)[3a] 进行了 X 射线单晶结构测定。研究了这些配合物在乙腈中的光物理性质,在 298 K 和在 298 和 80 K 下的固态光物理性质,以及已知的 4,4'-联吡啶 (bpy) 类似物 ((n-C(4)H(9))(4)N)[mer-{Re(6)S(8)Cl(3)(bpy)(3)}] ((Bu(4)N)[4])、((n-C(4)H(9))(4)N)(2)[trans-{Re(6)S(8)Cl(4)(bpy)(2)}] ((Bu(4)N)(2)[5a]) 和 ((n-C(4)H(9))(4)N)(2)[cis-{Re(6)S(8)Cl(4)(bpy)(2)}] ((Bu(4)N)(2)[5b]) 的光物理性质。5a 和 5b 在溶液和固态中的光物理数据与其他配合物明显不同。根据 2a 和 5a 的实验观察和密度泛函理论 (DFT) 计算,得出 5a 和 5b 表现出金属 (Re(6)S(8) 核)到配体 (bpy) 电荷转移 (MLCT) 类型发射。这是首次对六铼配合物的 MLCT 型发射进行明确的证明。对于 1、2a、2b 和 4 的发射,其中存在的 MLCT 成分只是次要的,这些可以主要解释为内核电子跃迁的贡献。3a 和 3b 的发射几乎可以完全归因于 Re(6)S(8) 核内的电子跃迁。双(bpy)配合物 (5a 和 5b) 的发射特征与三(bpy)配合物 (4) 不同,这是由于 Re(6)S(8) 核上氮供体数量的增加,从而稳定了 Re(6)S(8) 核的能量,使其低于 bpy 配体 pi轨道的能量。另一方面,已经表明,双(ppy) (2a 和 2b) 和双(bpe) 配合物 (3a 和 3b) 的发射特征最好用每个 N-杂芳烃配体的较高 pi能级来描述,这导致配合物激发态中金属的特征更强。