Optical Determination of Electron Transfer Dynamics and Kinetics for Asymmetrical [Mo2]–ph–[Mo2] Systems
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We report the study, in terms of electronic coupling (EC) and electron transfer (ET), on three asymmetrical Mo2 dimers [Mo2(DAniF)3]2[μ-(NH)OCC6H4CO2] ([NO–ph–OO]) (DAniF = N,N′-di(p-anisyl)formamidinate), [Mo2(DAniF)3]2[μ-(NH)2CC6H4CO2] ([NN–ph–OO]), and [Mo2(DAniF)3]2[μ-(NH)2CC6H4C(NH)O] ([NN–ph–NO]), which are closely related to the three symmetrical analogues [OO–ph–OO], [NO–ph–NO], and [NN–ph–NN] reported earlier. The mixed-valence (MV) complexes [NO–ph–OO]+, [NN–ph–OO]+, and [NN–ph–NO]+ exhibit metal to ligand and ligand to metal charge transfer bands, along with an intervalence (IV) transition absorption in the Near-IR region. The free energy change (ΔG°) for ET is determined by comparing the redox potential splitting (ΔE1/2) and IV transition energy (EIT) with the data for the symmetrical species. The reorganization energy (λ) is estimated from the Hush model (Δν1/2 = [16ln(2)λRT]1/2). Significantly, electrochemical and optical analyses verify EIT = ΔG° + λ, the core energetic relationship underlying the semiclassical theories. With the electronic coupling parameters calculated from the method suggested by Creutz, Newton and Sutin (HMM′ = ∼ 500 cm–1), the adiabatic ET rate constants ket (f) are determined to be ∼1010 s–1 for [NO–ph–OO]+ and [NN–ph–NO]+, smaller than ket (r) for the backward reaction and ket for the symmetrical analogues by 1 order of magnitude, and ∼109 s–1 for [NN–ph–OO]+. This work illustrates that the redox asymmetry in D–B–A systems controls the ET rate and direction.

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