Ni-containing superoxide dismutase (NiSOD) is the most recently discovered member of the class of metalloenzymes that detoxify the superoxide radical in aerobic organisms. In this study, we have employed a variety of spectroscopic and computational methods to probe the electronic structure of the NiSOD active site in both its oxidized (NiSOD(ox), possessing a low-spin (S = (1)/(2)) Ni(3+) center) and reduced (NiSOD(red), containing a diamagnetic Ni(2+) center) states. Our experimentally validated computed electronic-structure description for NiSOD(ox) reveals strong sigma-bonding interactions between Ni and the equatorial S/N ligands, which give rise to intense charge-transfer transitions in the near-UV region of the absorption spectrum. Resonance Raman (rR) spectra obtained with laser excitation in this region exhibit two features at 349 and 365 cm(-)(1) that are assigned to Ni-S(Cys) stretching modes. The NiSOD(red) active site also exhibits a high degree of metal-ligand bond covalency as well as filled/filled pi-interactions between Ni and S/N orbitals, which serve to adjust the redox potential of the Ni(2+) center. Comparison of our computational results for NiSOD(red) with those obtained in parallel studies of synthetic [NiS(2)N(2)] complexes reveals that the presence of an anionic N-donor ligand is crucial for promoting metal-based (versus S-based) oxidation of the active site. The implications of our electronic-structure descriptions with respect to the function of NiSOD are discussed, and a comparison of M-S(Cys) bonding in NiSOD and other metalloenzymes with sulfur ligation is provided.

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The active sites of Fe-only hydrogenases (FeHases) feature an unusual polynuclear iron-sulfur cluster, known as the H-cluster, that consists of a [Fe4S4] cubane linked to a di-iron subunit (the [2Fe]H component) via a bridging cysteine ligand (SCys). While previous computational studies of FeHases employed H-cluster models that only included the [2Fe]H component, we have utilized density functional theory (DFT), in conjunction with the broken-symmetry (BS) approach, to explore the geometric, electronic, and magnetic properties of the entire H-cluster. These calculations have allowed us to evaluate, for the first time, the influence of the [Fe4S4] cubane on the [2Fe]H component of the H-cluster in its active (Hox) and CO-inhibited (Hox-CO) states, both of which are paramagnetic (S=1/2). Our results reveal that the presence of the cubane tunes both the position and the donor strength of the SCys ligand, which, in turn, modulates the internal geometric and electronic structures of the [2Fe]H subcluster. Importantly, the BS methodology provides an accurate description of the exchange interactions within the H-cluster, permitting insight into the electronic origin of the changes in magnetic properties observed experimentally upon conversion of Hox to Hox-CO. Specifically, while the unpaired spin density in the Hox state is localized on the distal Fe center, in the Hox-CO state, it is delocalized over the [2Fe]H component, such that the proximal Fe center acquires significant spin density (where distal and proximal refer to the positions of the Fe centers relative to the cubane). To validate our H-cluster models on the basis of experimental data, two DFT-based approaches and the semiempirical INDO/S method have been employed to compute electron paramagnetic resonance parameters for the H-cluster states. While most computations yield reasonably accurate g values and ligand hyperfine coupling constants (i.e., A values) for the Hox and Hox-CO states, they fail to reproduce the isotropic 57Fe A tensors found experimentally. Finally, extension of the computational methodology employed successfully for the Hox and Hox-CO states to the metastable Hoxphoto state, generated by irradiation of the Hox-CO state at cryogenic temperatures, has allowed us to discriminate between proposed structural models for this species.

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A high-spin Co(II) complex (3d(7), S = 3/2), Co(PPh(3))(2)Cl(2) (Ph = phenyl), has been investigated in the solid state by both high-frequency and -field electron paramagnetic resonance (HFEPR) and by variable-temperature, variable-field magnetic circular dichroism (VTVH-MCD). In HFEPR spectroscopy, the combination of variable sub-THz frequencies generated by backward wave oscillators (150-700 GHz, corresponding to energy 5-23 cm(-1)) and high magnetic fields (0-25 T) constitutes a novel experimental technique allowing accurate determination of a complete set of spin Hamiltonian parameters for this complex: D = -14.76(2) cm(-1), E = 1.141(8) cm(-1), g(x) = 2.166(4), g(y) = 2.170(4), g(z) = 2.240(5). Independent VTVH-MCD studies on multiple absorption bands of the complex yield D = -14(3) cm(-1), E = 0.96(20) cm(-1) (absolute value of E/D = 0.08(2)), g(x) = 2.15(5), g(y) = 2.16(4), and g(z) = 2.17(3). This very good agreement between HFEPR and MCD indicates that there is no inherent discrepancy between these two quite different experimental techniques. Thus, depending on the nature of the sample, either can be reliably used to determine zero-field splitting parameters in high-spin Co(II), with the HFEPR being more accurate but VTVH-MCD being more sensitive.