Liu Tao, Zhang Hong-Xing, Xia Bao-Hui
State Key Laboratory of Theoretical and Computational Chemistry, Institute of Theoretical Chemistry, and College of Chemistry, Jilin University, Changchun 130023, People's Republic of China.
J Phys Chem A. 2007 Sep 6;111(35):8724-30. doi: 10.1021/jp072802n. Epub 2007 Aug 16.
The geometries, electronic structures, and spectroscopic properties of a series of novel cationic iridium(III) complexes [trans-(C/N)(2)Ir(PH(3))(2)]+ (C/N = 2-phenylpyridine, 1; benzoquinoline, 2; 1-phenylpytazolato, 3; 2-(4,6-difluorophenyl)pyridimato, 4) were investigated theoretically. The ground- and excited-state geometries were optimized at the B3LYP/LANL2DZ and CIS/LANL2DZ levels, respectively. The optimized geometry structural parameters agree well with the corresponding experimental results. The unoccupied molecular orbitals are dominantly localized on the C/N ligand, while the occupied molecular orbitals are composed of Ir atom and C/N ligand. Under the time-dependent density functional theory (TDDFT) level with the polarized continuum model (PCM) model, the absorption and phosphorescence in acetonitrile (MeCN) media were calculated based on the optimized ground- and excited-state geometries, respectively. The calculated results showed that the lowest-lying absorptions at 364 nm (1), 389 nm (2), 317 nm (3), and 344 nm (4) are all attributed to a {[d(yz)(Ir) + pi(C/N)] --> [pi*(C/N)]} transition with metal-to-ligand and intraligand charge transfer (MLCT/ILCT) characters; moreover, the phosphorescence at 460 (1) and 442 nm (4) originates from the 3{[d(yz)(Ir) + pi(C/N)] [pi*(C/N)]} (3)MLCT/(3)ILCT excited state, while that at 505 (2) and 399 nm (3) can be described as originating from different types of (3)MLCT/(3)ILCT excited state (3){[d(xy)(Ir) + pi(C/N)] [pi*(C/N)]}. The calculated results also revealed that the absorption and emission transition character can be altered by adjusting the pi electron-withdrawing groups and, furthermore, suggested that the phosphorescent color can be tuned by changing the pi-conjugation effect of the C/N ligand.
理论上研究了一系列新型阳离子铱(III)配合物[反式-(C/N)(2)Ir(PH(3))(2)]⁺(C/N = 2-苯基吡啶,1;苯并喹啉,2;1-苯基吡唑啉,3;2-(4,6-二氟苯基)吡啶,4)的几何结构、电子结构和光谱性质。基态和激发态几何结构分别在B3LYP/LANL2DZ和CIS/LANL2DZ水平上进行了优化。优化后的几何结构参数与相应的实验结果吻合良好。未占据分子轨道主要定域在C/N配体上,而占据分子轨道由Ir原子和C/N配体组成。在含极化连续介质模型(PCM)模型的含时密度泛函理论(TDDFT)水平下,分别基于优化后的基态和激发态几何结构计算了乙腈(MeCN)介质中的吸收和磷光。计算结果表明,在364 nm(1)、389 nm(2)、317 nm(3)和344 nm(4)处的最低吸收均归因于{[d(yz)(Ir) + π(C/N)]→[π*(C/N)]}跃迁,具有金属-配体和配体内电荷转移(MLCT/ILCT)特征;此外,460(1)和442 nm(4)处的磷光源于³{[d(yz)(Ir) + π(C/N)] [π*(C/N)]} (³)MLCT/(³)ILCT激发态,而505(2)和399 nm(3)处的磷光可描述为源于不同类型的(³)MLCT/(³)ILCT激发态³{[d(xy)(Ir) + π(C/N)] [π*(C/N)]}。计算结果还表明,通过调整π吸电子基团可以改变吸收和发射跃迁特征,此外,还表明通过改变C/N配体的π共轭效应可以调节磷光颜色。