30 research outputs found

    NO Disproportionation at a Mononuclear Site-Isolated Fe<sup>2+</sup> Center in Fe<sup>2+</sup>-MOF‑5

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    The weak-field ligand environments at the metal nodes of metal–organic frameworks (MOFs) mimic the electronic environment of metalloenzyme active sites, but little is known about the reactivity of MOF nodes toward small molecules of biological relevance. Here, we report that the ferrous ions in Fe<sup>2+</sup>-exchanged MOF-5 disproportionate nitric oxide to produce nitrous oxide and a ferric nitrito complex. Although mechanistic studies of N–N bond forming transformations often invoke a hyponitrite species, as in nitric oxide reductase and NO<sub><i>x</i></sub> reduction catalysis, little is known about this intermediate in its monoanionic state. Together with the first report of N–N coupling between NO molecules in a MOF, we present evidence for a species that is consistent with a ferric hyponitrite radical, whose isolation is enabled by the spatial constraints of the MOF matrix

    Solid State Collapse of a High-Spin Square-Planar Fe(II) Complex, Solution Phase Dynamics, and Electronic Structure Characterization of an Fe(II)<sub>2</sub> Dimer

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    Square-planar high-spin Fe­(II) molecular compounds are rare, and until recently, the only four examples of non-macrocyclic or sterically driven molecular compounds of this kind shared a common FeO<sub>4</sub> core. The trianionic pincer-type ligand [CF<sub>3</sub>-ONO]­H<sub>3</sub> (<b>1</b>) supports the high-spin square-planar Fe­(II) complex {[CF<sub>3</sub>-ONO]­FeCl}­{Li­(Sv)<sub>2</sub>}<sub>2</sub> (<b>2</b>). In the solid state, <b>2</b> forms the dimer complex {[CF<sub>3</sub>-ONO]­Fe}<sub>2</sub>­{(μ-Cl)<sub>2</sub>­(μ-LiTHF)<sub>4</sub>} (<b>3</b>) in 96% yield by simply applying a vacuum or stirring it with pentane for 2 h. A detailed high-frequency electron paramagnetic resonance and field-dependent <sup>57</sup>Fe Mössbauer investigation of <b>3</b> revealed a weak antiferromagnetic exchange interaction between the local iron spins which exhibit a zero-field splitting tensor characterized by negative <i>D</i> parameter. In solution, <b>2</b> is in equilibrium with the solvento complex {[CF<sub>3</sub>-ONO]­FeCl­(THF)}­{Li<sub>2</sub>(Sv)<sub>4</sub>} (<b>2·Sv</b>) and the dimer <b>3</b>. A combination of frozen solution <sup>57</sup>Fe Mössbauer spectroscopy and single crystal X-ray crystallography helped elucidate the solvent dependent equilibrium between these three species. The oxidation chemistry of <b>2·Sv</b> was investigated. Complex <b>2</b> reacts readily with the one-electron oxidizing agent CuCl<sub>2</sub> to give the Fe­(III) complex {[CF<sub>3</sub>-ONO]­FeCl<sub>2</sub>}­{Li­(THF)<sub>2</sub>}<sub>2</sub> (<b>4</b>). Also, <b>2·Sv</b> reacts with 2 equiv of TlPF<sub>6</sub> to form the Fe­(III) complex [CF<sub>3</sub>-ONO]­Fe­(THF)<sub>3</sub> (<b>5</b>)

    Spectroscopic and Theoretical Investigation of a Complex with an [OFe<sup>IV</sup>–O–Fe<sup>IV</sup>O] Core Related to Methane Monooxygenase Intermediate <b>Q</b>

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    Previous efforts to model the diiron­(IV) intermediate <b>Q</b> of soluble methane monooxygenase have led to the synthesis of a diiron­(IV) TPA complex, <b>2</b>, with an O=Fe<sup>IV</sup>–O–Fe<sup>IV</sup>–OH core that has two ferromagnetically coupled S<sub>loc</sub> = 1 sites. Addition of base to <b>2</b> at −85 °C elicits its conjugate base <b>6</b> with a novel OFe<sup>IV</sup>–O–Fe<sup>IV</sup>O core. In frozen solution, <b>6</b> exists in two forms, <b>6a</b> and <b>6b</b>, that we have characterized extensively using Mössbauer and parallel mode EPR spectroscopy. The conversion between <b>2</b> and <b>6</b> is quantitative, but the relative proportions of <b>6a</b> and <b>6b</b> are solvent dependent. <b>6a</b> has two equivalent high-spin (<i>S</i><sub>loc</sub> = 2) sites, which are antiferromagnetically coupled; its quadrupole splitting (0.52 mm/s) and isomer shift (0.14 mm/s) match those of intermediate <b>Q</b>. DFT calculations suggest that <b>6a</b> assumes an anti conformation with a dihedral OFe–FeO angle of 180°. Mössbauer and EPR analyses show that <b>6b</b> is a diiron­(IV) complex with ferromagnetically coupled <i>S</i><sub>loc</sub> = 1 and <i>S</i><sub>loc</sub> = 2 sites to give total spin <i>S</i><sub>t</sub> = 3. Analysis of the zero-field splittings and magnetic hyperfine tensors suggests that the dihedral OFe–FeO angle of <b>6b</b> is ∼90°. DFT calculations indicate that this angle is enforced by hydrogen bonding to both terminal oxo groups from a shared water molecule. The water molecule preorganizes <b>6b</b>, facilitating protonation of one oxo group to regenerate <b>2</b>, a protonation step difficult to achieve for mononuclear Fe<sup>IV</sup>O complexes. Complex <b>6</b> represents an intriguing addition to the handful of diiron­(IV) complexes that have been characterized

    Solid State Collapse of a High-Spin Square-Planar Fe(II) Complex, Solution Phase Dynamics, and Electronic Structure Characterization of an Fe(II)<sub>2</sub> Dimer

    No full text
    Square-planar high-spin Fe­(II) molecular compounds are rare, and until recently, the only four examples of non-macrocyclic or sterically driven molecular compounds of this kind shared a common FeO<sub>4</sub> core. The trianionic pincer-type ligand [CF<sub>3</sub>-ONO]­H<sub>3</sub> (<b>1</b>) supports the high-spin square-planar Fe­(II) complex {[CF<sub>3</sub>-ONO]­FeCl}­{Li­(Sv)<sub>2</sub>}<sub>2</sub> (<b>2</b>). In the solid state, <b>2</b> forms the dimer complex {[CF<sub>3</sub>-ONO]­Fe}<sub>2</sub>­{(μ-Cl)<sub>2</sub>­(μ-LiTHF)<sub>4</sub>} (<b>3</b>) in 96% yield by simply applying a vacuum or stirring it with pentane for 2 h. A detailed high-frequency electron paramagnetic resonance and field-dependent <sup>57</sup>Fe Mössbauer investigation of <b>3</b> revealed a weak antiferromagnetic exchange interaction between the local iron spins which exhibit a zero-field splitting tensor characterized by negative <i>D</i> parameter. In solution, <b>2</b> is in equilibrium with the solvento complex {[CF<sub>3</sub>-ONO]­FeCl­(THF)}­{Li<sub>2</sub>(Sv)<sub>4</sub>} (<b>2·Sv</b>) and the dimer <b>3</b>. A combination of frozen solution <sup>57</sup>Fe Mössbauer spectroscopy and single crystal X-ray crystallography helped elucidate the solvent dependent equilibrium between these three species. The oxidation chemistry of <b>2·Sv</b> was investigated. Complex <b>2</b> reacts readily with the one-electron oxidizing agent CuCl<sub>2</sub> to give the Fe­(III) complex {[CF<sub>3</sub>-ONO]­FeCl<sub>2</sub>}­{Li­(THF)<sub>2</sub>}<sub>2</sub> (<b>4</b>). Also, <b>2·Sv</b> reacts with 2 equiv of TlPF<sub>6</sub> to form the Fe­(III) complex [CF<sub>3</sub>-ONO]­Fe­(THF)<sub>3</sub> (<b>5</b>)

    Evolution of Bonding and Magnetism via Changes in Valence Electron Count in CuFe2–xCoxGe2

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    A series of solid solutions, CuFe2–xCoxGe2 (x = 0, 0.2, 0.4, 0.8, and 1.0), have been synthesized by arc-melting and characterized by powder X-ray and neutron diffraction, magnetic measurements, Mössbauer spectroscopy, and electronic band structure calculations. All compounds crystallize in the CuFe2Ge2 structure type, which can be considered as a three-dimensional framework built of fused MGe6 octahedra and MGe5 trigonal bipyramids (M = Fe and Co), with channels filled by rows of Cu atoms. As the Co content (x) increases, the unit cell volume decreases in an anisotropic fashion: the b and c lattice parameters decrease while the a parameter increases. The changes in all the parameters are nearly linear, thus following Vegard’s law. CuFe2Ge2 exhibits two successive antiferromagnetic (AFM) orderings, corresponding to the formation of a commensurate AFM structure, followed by an incommensurate AFM structure observed at lower temperatures. Additionally, as the Co content increases, the AFM ordering temperature (TN) gradually decreases, and only one AFM transition is observed for x ≥ 0.2. The magnetic behavior of unsubstituted CuFe2Ge2 was found to be sensitive to the preparation method. The temperature-dependent zero-field 57Fe Mössbauer spectra reveal two hyperfine split components that evolve in agreement with the two consecutive AFM orderings observed in magnetic measurements. In contrast, the field-dependent spectra obtained for fields ≥ 2 T reveal a parallel arrangement of the moments associated with the two crystallographically unique metal sites. Electronic band structure calculations and chemical bonding analysis reveal a mix of strong M–M antibonding and non-bonding states at the Fermi level, in support of the overall AFM ordering observed in zero field. The substitution of Co for Fe reduces the population of the M–M antibonding states and the overall density of states at the Fermi level, thus suppressing the TN value.This is a manuscript of an article published as Tener, Zachary P., Vincent Yannello, V. Ovidiu Garlea, Saul H. Lapidus, Philip Yox, Kirill Kovnir, Sebastian A. Stoian, and Michael Shatruk. "Evolution of Bonding and Magnetism via Changes in Valence Electron Count in CuFe2–x Co x Ge2." Inorganic Chemistry 61, no. 10 (2022): 4257-4269. DOI: 10.1021/acs.inorgchem.1c02997. Copyright 2022 American Chemical Society Posted with permission. DOE Contract Number(s): AC05-00OR22725; DMR-1905499; DMR-1644779; AC02–07CH11358; AC02-06CH11357

    Synthesis and Characterization of a Stable High-Valent Cobalt Carbene Complex

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    The formally Co<sup>IV</sup> carbene Co­(OR)<sub>2</sub>(CPh<sub>2</sub>) is formed upon the reaction of diphenyl­diazo­methane with the cobalt bis­(alkoxide) precursor Co­(OR)<sub>2</sub>(THF)<sub>2</sub>. Structural, spectroscopic, and theoretical studies demonstrate that Co­(OR)<sub>2</sub>(CPh<sub>2</sub>) has significant high-valent Co<sup>IV</sup>CPh<sub>2</sub> character with non-negligible spin density on the carbene moiety

    Synthesis and Characterization of a Stable High-Valent Cobalt Carbene Complex

    No full text
    The formally Co<sup>IV</sup> carbene Co­(OR)<sub>2</sub>(CPh<sub>2</sub>) is formed upon the reaction of diphenyl­diazo­methane with the cobalt bis­(alkoxide) precursor Co­(OR)<sub>2</sub>(THF)<sub>2</sub>. Structural, spectroscopic, and theoretical studies demonstrate that Co­(OR)<sub>2</sub>(CPh<sub>2</sub>) has significant high-valent Co<sup>IV</sup>CPh<sub>2</sub> character with non-negligible spin density on the carbene moiety
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