Root David E., Mahroof-Tahir Mohammed, Karlin Kenneth D., Solomon Edward I.
Departments of Chemistry, Stanford University, Stanford, California 94305, and The Johns Hopkins University, Baltimore, Maryland 21218.
Inorg Chem. 1998 Sep 21;37(19):4838-4848. doi: 10.1021/ic980606c.
Spectroscopic studies of a &mgr;-1,1-hydroperoxo-bridged copper dimer are combined with SCF-Xalpha-SW molecular orbital calculations to describe the vibrational and electronic structure of the hydroperoxo-copper complex and compare it to that of previously studied peroxo-copper species. Four vibrational modes of the Cu(2)OOH unit in the resonance Raman and infrared spectra are assigned on the basis of isotope shifts: nu(O-O) = 892 cm(-)(1), nu(as)(Cu-O) = 506 cm(-)(1), nu(s)(Cu-O) = 322 cm(-)(1), and nu(O-H) = 3495 cm(-)(1). The 892 cm(-)(1) O-O stretch of the &mgr;-1,1-hydroperoxo-bridged copper dimer is 89 cm(-)(1) higher than that of the unprotonated complex. Resonance Raman profiles of the 892 cm(-)(1) O-O stretch are used to assign an electronic absorption band at 25 200 cm(-)(1) (epsilon = 6700 M(-)(1) cm(-)(1)) to a hydroperoxide pi-to-Cu charge transfer (CT) transition. This band is approximately 5000 cm(-)(1) higher in energy than the corresponding transition in the unprotonated complex. The pi-to-Cu CT transition intensity defines the degree of hydroperoxide-to-copper charge donation, which is lower than in the unprotonated complex due to the increased electronegativity of the peroxide with protonation. The lower Cu-O covalency of this hydroperoxo-copper complex shows that the high O-O stretching frequency is not due to increased pi-to-Cu charge donation but rather reflects the direct effect of protonation on intra-peroxide bonding. Density functional calculations are used to describe changes in intra-peroxide and Cu-O bonding upon protonation of the peroxo-copper complex and to relate these changes to changes in reactivity.
对一个μ-1,1-氢过氧桥联铜二聚体进行光谱研究,并结合SCF-Xα-SW分子轨道计算,以描述氢过氧-铜配合物的振动和电子结构,并将其与先前研究的过氧-铜物种进行比较。基于同位素位移,在共振拉曼光谱和红外光谱中确定了Cu(2)OOH单元的四种振动模式:ν(O-O)=892 cm⁻¹,ν(as)(Cu-O)=506 cm⁻¹,ν(s)(Cu-O)=322 cm⁻¹,ν(O-H)=3495 cm⁻¹。μ-1,1-氢过氧桥联铜二聚体的892 cm⁻¹ O-O伸缩振动比未质子化配合物的高89 cm⁻¹。892 cm⁻¹ O-O伸缩振动的共振拉曼光谱用于将25200 cm⁻¹(ε=6700 M⁻¹ cm⁻¹)处的电子吸收带归属于氢过氧化物π到铜的电荷转移(CT)跃迁。该谱带的能量比未质子化配合物中的相应跃迁高约5000 cm⁻¹。π到铜的CT跃迁强度定义了氢过氧化物到铜的电荷给予程度,由于质子化使过氧化物的电负性增加,该程度低于未质子化配合物。这种氢过氧-铜配合物较低的Cu-O共价性表明高O-O伸缩频率不是由于π到铜的电荷给予增加,而是反映了质子化对过氧化物内键合的直接影响。密度泛函计算用于描述过氧-铜配合物质子化时过氧化物内和Cu-O键合的变化,并将这些变化与反应性变化联系起来。