Sarangi Ritimukta, Aboelella Nermeen, Fujisawa Kiyoshi, Tolman William B, Hedman Britt, Hodgson Keith O, Solomon Edward I
Department of Chemistry, Stanford University, Stanford, California 94305, USA.
J Am Chem Soc. 2006 Jun 28;128(25):8286-96. doi: 10.1021/ja0615223.
The geometric and electronic structures of two mononuclear CuO2 complexes, [Cu(O2){HB(3-Ad-5-(i)Prpz)3}] (1) and [Cu(O2)(beta-diketiminate)] (2), have been evaluated using Cu K- and L-edge X-ray absorption spectroscopy (XAS) studies in combination with valence bond configuration interaction (VBCI) simulations and spin-unrestricted broken symmetry density functional theory (DFT) calculations. Cu K- and L-edge XAS data indicate the Cu(II) and Cu(III) nature of 1 and 2, respectively. The total integrated intensity under the L-edges shows that the 's in 1 and 2 contain 20% and 28% Cu character, respectively, indicative of very covalent ground states in both complexes, although more so in 1. Two-state VBCI simulations also indicate that the ground state in 2 has more Cu (/3d8) character. DFT calculations show that the in both complexes is dominated by O2(n-) character, although the O2(n-) character is higher in 1. It is shown that the ligand L plays an important role in modulating Cu-O2 bonding in these LCuO2 systems and tunes the ground states of 1 and 2 to have dominant Cu(II)-superoxide-like and Cu(III)-peroxide-like character, respectively. The contributions of ligand field (LF) and the charge on the absorbing atom in the molecule (Q(mol)M) to L- and K-edge energy shifts are evaluated using DFT and time-dependent DFT calculations. It is found that LF makes a dominant contribution to the edge energy shift, while the effect of Q(mol)M is minor. The charge on the Cu in the Cu(III) complex is found to be similar to that in Cu(II) complexes, which indicates a much stronger interaction with the ligand, leading to extensive charge transfer.
利用铜K边和L边X射线吸收光谱(XAS)研究,并结合价键组态相互作用(VBCI)模拟以及自旋非限制破缺对称性密度泛函理论(DFT)计算,对两种单核CuO₂配合物[Cu(O₂){HB(3 - Ad - 5 - (i)Prpz)₃}](1)和[Cu(O₂)(β - 二酮亚胺)](2)的几何结构和电子结构进行了评估。铜K边和L边XAS数据分别表明1和2具有Cu(II)和Cu(III)的性质。L边下方的总积分强度表明,1和2中的“s”分别含有20%和28%的Cu特征,这表明两种配合物都具有非常共价的基态,尽管1中更为明显。双态VBCI模拟还表明,2中的基态具有更多的Cu(³d⁸)特征。DFT计算表明,两种配合物中的“”主要由O₂(ⁿ⁻)特征主导,尽管1中的O₂(ⁿ⁻)特征更高。结果表明,配体L在调节这些LCuO₂体系中的Cu - O₂键合方面起着重要作用,并将1和2的基态分别调整为具有主要的类Cu(II)超氧化物和类Cu(III)过氧化物特征。利用DFT和含时DFT计算评估了配体场(LF)和分子中吸收原子上的电荷(Q(mol)M)对L边和K边能量位移的贡献。发现LF对边能量位移起主要作用,而Q(mol)M的影响较小。发现Cu(III)配合物中Cu上的电荷与Cu(II)配合物中的电荷相似,这表明与配体的相互作用更强,导致广泛的电荷转移。