Lind Samuel J, Walsh Timothy J, Blackman Allan G, Polson Matthew I J, Irwin Garth I S, Gordon Keith C
MacDiarmid Institute for Advanced Materials and Nanotechnology, Department of Chemistry, University of Otago, Dunedin, New Zealand.
J Phys Chem A. 2009 Apr 16;113(15):3566-75. doi: 10.1021/jp808179m.
The compound (Cu(PPh(3))(2))(3)(HATNMe(6))(3) has been synthesized and characterized by X-ray crystallography, resonance Raman spectroscopy, and density functional theory (DFT) calculations. The X-ray structure of solvated (Cu(PPh(3))(2))(3)(HATNMe(6))(3) [rhombohedral, R3, a = b = 21.6404(4) A, c = 53.188(3) A, alpha = beta = 90 degrees, gamma = 120 degrees] shows that the HATNMe(6) ligand is very slightly twisted. The electronic absorption spectrum of the complex in chloroform shows two bands in the visible region attributed to ligand-centered (LC) and metal-to-ligand charge-transfer (MLCT) transitions, respectively. Time-dependent DFT calculations show good agreement with experiment, with two MLCT and one LC transition predicted in the visible region (641, 540, and 500 nm). Resonance Raman spectra of the complex using discrete excitation energies between 647 and 406 nm showed a variation in enhancement patterns consistent with at least two distinct transitions. The absolute Raman cross sections have been evaluated and, through a wavepacket analysis, the amount of distortion along each vibrational mode across the Franck-Condon surface is established from the calculated dimensionless displacement (Delta) values as well as other electronic parameters. The pattern of Delta values shows good agreement with the observed calculated modes, with the MLCT transition, showing much larger Delta values for outer ring modes such as nu(93) and nu(205) than in the LC transition. This is consistent with the molecular orbitals involved in the two transitions; the donor orbitals for the LC transition have similar outer-ring bonding characteristics compared to the MLCT transition, which has no donor orbital bonding characteristics on the ligand because the donor molecular orbitals are dpi orbitals.
化合物(Cu(PPh(3))(2))(3)(HATNMe(6))(3)已通过X射线晶体学、共振拉曼光谱和密度泛函理论(DFT)计算进行了合成和表征。溶剂化的(Cu(PPh(3))(2))(3)(HATNMe(6))(3)的X射线结构[菱面体,R3,a = b = 21.6404(4) Å,c = 53.188(3) Å,α = β = 90°,γ = 120°]表明HATNMe(6)配体略有扭曲。该配合物在氯仿中的电子吸收光谱在可见光区域显示出两个谱带,分别归因于配体中心(LC)和金属到配体的电荷转移(MLCT)跃迁。含时DFT计算与实验结果吻合良好,在可见光区域(641、540和500 nm)预测有两个MLCT跃迁和一个LC跃迁。使用647至406 nm之间的离散激发能量对该配合物进行的共振拉曼光谱显示,增强模式的变化与至少两个不同的跃迁一致。已评估了绝对拉曼截面,并通过波包分析,根据计算出的无量纲位移(Δ)值以及其他电子参数确定了沿弗兰克-康登表面上每个振动模式的畸变程度。Δ值的模式与观察到的计算模式吻合良好,对于MLCT跃迁,外环模式如ν(93)和ν(205)的Δ值比LC跃迁中的大得多。这与两个跃迁中涉及的分子轨道一致;与MLCT跃迁相比,LC跃迁的供体轨道具有相似的外环键合特征,MLCT跃迁在配体上没有供体轨道键合特征,因为供体分子轨道是dpi轨道。