Palmer Joshua H, Lancaster Kyle M
Beckman Institute , California Institute of Technology, Pasadena, California 91125, United States.
Inorg Chem. 2012 Nov 19;51(22):12473-82. doi: 10.1021/ic3018826. Epub 2012 Nov 1.
The electronic structures of monocationic tris[(5,10,15-pentafluorophenyl)-corrolato]iridium compounds, Ir(tpfc)L2, where L = 4-cyanopyridine 1, pyridine 2, 4-methoxypyridine 3, or 4-(N,N'-dimethylamino)pyridine 4, have been probed by electron paramagnetic resonance (EPR) spectroscopy, Ir L3,2-edge X-ray absorption spectroscopy (XAS), UV/visible (UV-vis) spectroelectrochemistry, and density functional theoretical (DFT) calculations. The data demonstrate that these complexes, which have been previously formulated as either of the limiting cases Ir(III)(tpfc(•))L2 or Ir(IV)(tpfc)L2, are best described as possessing a singly occupied molecular orbital (SOMO) dominated by tpfc with small but significant Ir admixture. EPR g-values and electronic absorption spectra are reproduced well using a simple DFT approach. These quantities depend profoundly upon Ir orbital contribution to the SOMO. To wit, the calculated Ir spin population ranges from 10.6% for 1 to 16.3% for 4, reflecting increased Ir d mixing into the SOMO with increasingly electron-rich axial ligation. This gives rise to experimentally measured gz values ranging from 2.335 to 2.533, metal-to-ligand charge transfer (MLCT) bands ranging from 14730 and 14330 cm(-1), and Ir(tpfc)L2 reduction potentials ranging from 0.305 to 0.035 V vs Fc(+/0). In addition, the calculated Ir character in the SOMO tracks with estimated Ir L3,2 XAS branching ratios (EBR), reflecting the increasing degree of Ir d orbital character upon proceeding from 1 to 4.
单阳离子三[(5,10,15-五氟苯基)-卟吩合]铱化合物Ir(tpfc)L2(其中L = 4-氰基吡啶1、吡啶2、4-甲氧基吡啶3或4-(N,N'-二甲基氨基)吡啶4)的电子结构已通过电子顺磁共振(EPR)光谱、Ir L3,2边X射线吸收光谱(XAS)、紫外/可见(UV-vis)光谱电化学以及密度泛函理论(DFT)计算进行了探究。数据表明,这些配合物先前被表述为极限情况Ir(III)(tpfc(•))L2或Ir(IV)(tpfc)L2中的一种,而实际上最好描述为具有一个以tpfc为主导且有少量但显著的Ir混合的单占据分子轨道(SOMO)。使用简单的DFT方法能很好地重现EPR g值和电子吸收光谱。这些量极大地取决于Ir轨道对SOMO的贡献。具体而言,计算得到的Ir自旋布居从1的10.6%到4的16.3%不等,这反映出随着轴向配体电子云密度的增加,Ir d轨道混入SOMO的程度增大。这导致实验测得的gz值在2.335至2.533之间、金属到配体的电荷转移(MLCT)带在14730和14330 cm(-1)之间,以及Ir(tpfc)L2的还原电位相对于Fc(+/0)在0.305至0.035 V之间。此外,计算得到的SOMO中Ir的特征与估计的Ir L3,2 XAS分支比(EBR)相符,反映出从1到4过程中Ir d轨道特征程度的增加。