18 research outputs found

    Substrate-Mediated Oxygen Activation by Homoprotocatechuate 2,3-Dioxygenase: Intermediates Formed by a Tyrosine 257 Variant

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    Homoprotocatechuate (HPCA; 3,4-dihydroxyphenylacetate or 4-carboxymethyl catechol) and O<sub>2</sub> bind in adjacent ligand sites of the active site Fe<sup>II</sup> of homoprotocatechuate 2,3-dioxygenase (FeHPCD). We have proposed that electron transfer from the chelated aromatic substrate through the Fe<sup>II</sup> to O<sub>2</sub> gives both substrates radical character. This would promote reaction between the substrates to form an alkylperoxo intermediate as the first step in aromatic ring cleavage. Several active site amino acids are thought to promote these reactions through acid/base chemistry, hydrogen bonding, and electrostatic interactions. Here the role of Tyr257 is explored by using the Tyr257Phe (Y257F) variant, which decreases <i>k</i><sub>cat</sub> by about 75%. The crystal structure of the FeHPCD-HPCA complex has shown that Tyr257 hydrogen bonds to the deprotonated C2-hydroxyl of HPCA. Stopped-flow studies show that at least two reaction intermediates, termed Y257F<sub>Int1</sub><sup>HPCA</sup> and Y257F<sub>Int2</sub><sup>HPCA</sup>, accumulate during the Y257F-HPCA + O<sub>2</sub> reaction prior to formation of the ring-cleaved product. Y257F<sub>Int1</sub><sup>HPCA</sup> is colorless and is formed as O<sub>2</sub> binds reversibly to the HPCAā€“enzyme complex. Y257F<sub>Int2</sub><sup>HPCA</sup> forms spontaneously from Y257F<sub>Int1</sub><sup>HPCA</sup> and displays a chromophore at 425 nm (Īµ<sub>425</sub> = 10ā€‰500 M<sup>ā€“1</sup> cm<sup>ā€“1</sup>). MoĢˆssbauer spectra of the intermediates trapped by rapid freeze quench show that both intermediates contain Fe<sup>II</sup>. The lack of a chromophore characteristic of a quinone or semiquinone form of HPCA, the presence of Fe<sup>II</sup>, and the low O<sub>2</sub> affinity suggest that Y257F<sub>Int1</sub><sup>HPCA</sup> is an HPCA-Fe<sup>II</sup>-O<sub>2</sub> complex with little electron delocalization onto the O<sub>2</sub>. In contrast, the intense spectrum of Y257F<sub>Int2</sub><sup>HPCA</sup> suggests the intermediate is most likely an HPCA quinone-Fe<sup>II</sup>-(hydro)Ā­peroxo species. Steady-state and transient kinetic analyses show that steps of the catalytic cycle are slowed by as much as 100-fold by the mutation. These effects can be rationalized by a failure of Y257F to facilitate the observed distortion of the bound HPCA that is proposed to promote transfer of one electron to O<sub>2</sub>

    Spectroscopic and Theoretical Investigation of a Complex with an [Oī—»Fe<sup>IV</sup>ā€“Oā€“Fe<sup>IV</sup>ī—»O] Core Related to Methane Monooxygenase Intermediate <b>Q</b>

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    Previous efforts to model the diironĀ­(IV) intermediate <b>Q</b> of soluble methane monooxygenase have led to the synthesis of a diironĀ­(IV) TPA complex, <b>2</b>, with an O=Fe<sup>IV</sup>ā€“Oā€“Fe<sup>IV</sup>ā€“OH core that has two ferromagnetically coupled S<sub>loc</sub> = 1 sites. Addition of base to <b>2</b> at āˆ’85 Ā°C elicits its conjugate base <b>6</b> with a novel Oī—»Fe<sup>IV</sup>ā€“Oā€“Fe<sup>IV</sup>ī—»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 MoĢˆssbauer 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 Oī—»Feā€“Feī—»O angle of 180Ā°. MoĢˆssbauer and EPR analyses show that <b>6b</b> is a diironĀ­(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 Oī—»Feā€“Feī—»O angle of <b>6b</b> is āˆ¼90Ā°. 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>ī—»O complexes. Complex <b>6</b> represents an intriguing addition to the handful of diironĀ­(IV) complexes that have been characterized

    Sc<sup>3+</sup>-Triggered Oxoiron(IV) Formation from O<sub>2</sub> and its Non-Heme Iron(II) Precursor via a Sc<sup>3+</sup>ā€“Peroxoā€“Fe<sup>3+</sup> Intermediate

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    We report that redox-inactive Sc<sup>3+</sup> can trigger O<sub>2</sub> activation by the Fe<sup>II</sup>(TMC) center (TMC = tetramethylcyclam) to generate the corresponding oxoironĀ­(IV) complex in the presence of BPh<sub>4</sub><sup>ā€“</sup> as an electron donor. To model a possible intermediate in the above reaction, we generated an unprecedented Sc<sup>3+</sup> adduct of [Fe<sup>III</sup>(Ī·<sup>2</sup>-O<sub>2</sub>)Ā­(TMC)]<sup>+</sup> by an alternative route, which was found to have an Fe<sup>3+</sup>ā€“(Ī¼-Ī·<sup>2</sup>:Ī·<sup>2</sup>-peroxo)ā€“Sc<sup>3+</sup> core and to convert to the oxoironĀ­(IV) complex. These results have important implications for the role a Lewis acid can play in facilitating Oā€“O bond cleavage during the course of O<sub>2</sub> activation at non-heme iron centers

    Upside Down! Crystallographic and Spectroscopic Characterization of an [Fe<sup>IV</sup>(O<sub>syn</sub>)(TMC)]<sup>2+</sup> Complex

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    Fe<sup>II</sup>(TMC)Ā­(OTf)<sub>2</sub> reacts with 2-<sup>t</sup>BuSO<sub>2</sub>ā€“C<sub>6</sub>H<sub>4</sub>IO to afford an oxoironĀ­(IV) product, <b>2</b>, distinct from the previously reported [Fe<sup>IV</sup>(O<sub>anti</sub>)Ā­(TMC)Ā­(NCMe)]<sup>2+</sup>. In MeCN, <b>2</b> has a blue-shifted near-IR band, a higher Ī½Ā­(Feī—»O), a larger MoĢˆssbauer quadrupole splitting, and quite a distinct <sup>1</sup>H NMR spectrum. Structural analysis of crystals grown from CH<sub>2</sub>Cl<sub>2</sub> reveals a complex with the formulation of [Fe<sup>IV</sup>(O<sub>syn</sub>)Ā­(TMC)Ā­(OTf)]Ā­(OTf) and the shortest Fe<sup>IV</sup>ī—»O bond [1.625(4) ƅ] found to date

    Structural, EPR, and MoĢˆssbauer Characterization of (Ī¼-Alkoxo)(Ī¼-Carboxylato)Diiron(II,III) Model Complexes for the Active Sites of Mixed-Valent Diiron Enzymes

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    To obtain structural and spectroscopic models for the diironĀ­(II,III) centers in the active sites of diiron enzymes, the (Ī¼-alkoxo)Ā­(Ī¼-carboxylato)Ā­diironĀ­(II,III) complexes [Fe<sup>II</sup>Fe<sup>III</sup>(<i>N</i>-Et-HPTB)Ā­(O<sub>2</sub>CPh)Ā­(NCCH<sub>3</sub>)<sub>2</sub>]Ā­(ClO<sub>4</sub>)<sub>3</sub> (<b>1</b>) and [Fe<sup>II</sup>Fe<sup>III</sup>(<i>N</i>-Et-HPTB)Ā­(O<sub>2</sub>CPh)Ā­(Cl)Ā­(HOCH<sub>3</sub>)]Ā­(ClO<sub>4</sub>)<sub>2</sub> (<b>2</b>) (<i>N</i>-Et-HPTB = <i>N,N,N</i>ā€²<i>,N</i>ā€²-tetrakisĀ­(2-(1-ethyl-benzimidazolylmethyl))-2-hydroxy-1,3-diaminopropane) have been prepared and characterized by X-ray crystallography, UVā€“visible absorption, EPR, and MoĢˆssbauer spectroscopies. Fe1ā€“Fe2 separations are 3.60 and 3.63 ƅ, and Fe1ā€“O1ā€“Fe2 bond angles are 128.0Ā° and 129.4Ā° for <b>1</b> and <b>2</b>, respectively. MoĢˆssbauer and EPR studies of <b>1</b> show that the Fe<sup>III</sup> (<i>S</i><sub>A</sub> = 5/2) and Fe<sup>II</sup> (<i>S</i><sub>B</sub> = 2) sites are antiferromagnetically coupled to yield a ground state with <i>S</i> = 1/2 (<i>g</i> <b>=</b> 1.75, 1.88, 1.96); MoĢˆssbauer analysis of solid <b>1</b> yields <i>J</i> = 22.5 Ā± 2 cm<sup>ā€“1</sup> for the exchange coupling constant (H = <i>J</i><b>S</b><sub>A</sub>Ā·<b>S</b><sub>B</sub> convention). In addition to the <i>S</i> = 1/2 ground-state spectrum of <b>1</b>, the EPR signal for the <i>S</i> = 3/2 excited state of the spin ladder can also be observed, the first time such a signal has been detected for an antiferromagnetically coupled diironĀ­(II,III) complex. The anisotropy of the <sup>57</sup>Fe magnetic hyperfine interactions at the Fe<sup>III</sup> site is larger than normally observed in mononuclear complexes and arises from admixing <i>S</i> > 1/2 excited states into the <i>S</i> = 1/2 ground state by zero-field splittings at the two Fe sites. Analysis of the ā€œ<i>D</i>/<i>J</i>ā€ mixing has allowed us to extract the zero-field splitting parameters, local <i>g</i> values, and magnetic hyperfine structural parameters for the individual Fe sites. The methodology developed and followed in this analysis is presented in detail. The spin Hamiltonian parameters of <b>1</b> are related to the molecular structure with the help of DFT calculations. Contrary to what was assumed in previous studies, our analysis demonstrates that the deviations of the <i>g</i> values from the free electron value (<i>g</i> = 2) for the antiferromagnetically coupled diironĀ­(II,III) core in complex <b>1</b> are predominantly determined by the anisotropy of the effective <i>g</i> values of the ferrous ion and only to a lesser extent by the admixture of excited states into ground-state ZFS terms (<i>D</i>/<i>J</i> mixing). The results for <b>1</b> are discussed in the context of the data available for diironĀ­(II,III) clusters in proteins and synthetic diironĀ­(II,III) complexes

    Structural, EPR, and MoĢˆssbauer Characterization of (Ī¼-Alkoxo)(Ī¼-Carboxylato)Diiron(II,III) Model Complexes for the Active Sites of Mixed-Valent Diiron Enzymes

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    To obtain structural and spectroscopic models for the diironĀ­(II,III) centers in the active sites of diiron enzymes, the (Ī¼-alkoxo)Ā­(Ī¼-carboxylato)Ā­diironĀ­(II,III) complexes [Fe<sup>II</sup>Fe<sup>III</sup>(<i>N</i>-Et-HPTB)Ā­(O<sub>2</sub>CPh)Ā­(NCCH<sub>3</sub>)<sub>2</sub>]Ā­(ClO<sub>4</sub>)<sub>3</sub> (<b>1</b>) and [Fe<sup>II</sup>Fe<sup>III</sup>(<i>N</i>-Et-HPTB)Ā­(O<sub>2</sub>CPh)Ā­(Cl)Ā­(HOCH<sub>3</sub>)]Ā­(ClO<sub>4</sub>)<sub>2</sub> (<b>2</b>) (<i>N</i>-Et-HPTB = <i>N,N,N</i>ā€²<i>,N</i>ā€²-tetrakisĀ­(2-(1-ethyl-benzimidazolylmethyl))-2-hydroxy-1,3-diaminopropane) have been prepared and characterized by X-ray crystallography, UVā€“visible absorption, EPR, and MoĢˆssbauer spectroscopies. Fe1ā€“Fe2 separations are 3.60 and 3.63 ƅ, and Fe1ā€“O1ā€“Fe2 bond angles are 128.0Ā° and 129.4Ā° for <b>1</b> and <b>2</b>, respectively. MoĢˆssbauer and EPR studies of <b>1</b> show that the Fe<sup>III</sup> (<i>S</i><sub>A</sub> = 5/2) and Fe<sup>II</sup> (<i>S</i><sub>B</sub> = 2) sites are antiferromagnetically coupled to yield a ground state with <i>S</i> = 1/2 (<i>g</i> <b>=</b> 1.75, 1.88, 1.96); MoĢˆssbauer analysis of solid <b>1</b> yields <i>J</i> = 22.5 Ā± 2 cm<sup>ā€“1</sup> for the exchange coupling constant (H = <i>J</i><b>S</b><sub>A</sub>Ā·<b>S</b><sub>B</sub> convention). In addition to the <i>S</i> = 1/2 ground-state spectrum of <b>1</b>, the EPR signal for the <i>S</i> = 3/2 excited state of the spin ladder can also be observed, the first time such a signal has been detected for an antiferromagnetically coupled diironĀ­(II,III) complex. The anisotropy of the <sup>57</sup>Fe magnetic hyperfine interactions at the Fe<sup>III</sup> site is larger than normally observed in mononuclear complexes and arises from admixing <i>S</i> > 1/2 excited states into the <i>S</i> = 1/2 ground state by zero-field splittings at the two Fe sites. Analysis of the ā€œ<i>D</i>/<i>J</i>ā€ mixing has allowed us to extract the zero-field splitting parameters, local <i>g</i> values, and magnetic hyperfine structural parameters for the individual Fe sites. The methodology developed and followed in this analysis is presented in detail. The spin Hamiltonian parameters of <b>1</b> are related to the molecular structure with the help of DFT calculations. Contrary to what was assumed in previous studies, our analysis demonstrates that the deviations of the <i>g</i> values from the free electron value (<i>g</i> = 2) for the antiferromagnetically coupled diironĀ­(II,III) core in complex <b>1</b> are predominantly determined by the anisotropy of the effective <i>g</i> values of the ferrous ion and only to a lesser extent by the admixture of excited states into ground-state ZFS terms (<i>D</i>/<i>J</i> mixing). The results for <b>1</b> are discussed in the context of the data available for diironĀ­(II,III) clusters in proteins and synthetic diironĀ­(II,III) complexes

    Enzyme Substrate Complex of the H200C Variant of Homoprotocatechuate 2,3-Dioxygenase: MoĢˆssbauer and Computational Studies

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    The extradiol, aromatic ring-cleaving enzyme homoprotocatechuate 2,3-dioxygenase (HPCD) catalyzes a complex chain of reactions that involve second sphere residues of the active site. The importance of the second-sphere residue His200 was demonstrated in studies of HPCD variants, such as His200Cys (H200C), which revealed significant retardations of certain steps in the catalytic process as a result of the substitution, allowing novel reaction cycle intermediates to be trapped for spectroscopic characterization. As the H200C variant largely retains the wild-type active site structure and produces the correct ring-cleaved product, this variant presents a valuable target for mechanistic HPCD studies. Here, the high-spin Fe<sup>II</sup> states of resting H200C and the H200Cā€“homoprotocatechuate enzymeā€“substrate (ES) complex have been characterized with MoĢˆssbauer spectroscopy to assess the electronic structures of the active site in these states. The analysis reveals a high-spin Fe<sup>II</sup> center in a low symmetry environment that is reflected in the values of the zero-field splitting (ZFS) (<i>D</i> ā‰ˆ ā€“ 8 cm<sup>ā€“1</sup>, <i>E</i>/<i>D</i> ā‰ˆ 1/3 in ES), as well as the relative orientations of the principal axes of the <sup>57</sup>Fe magnetic hyperfine (<b>A</b>) and electric field gradient (EFG) tensors relative to the ZFS tensor axes. A spin Hamiltonian analysis of the spectra for the ES complex indicates that the magnetization axis of the integer-spin <i>S</i> = 2 Fe<sup>II</sup> system is nearly parallel to the symmetry axis, <i>z</i>, of the doubly occupied d<sub><i>xy</i></sub> ground orbital deduced from the EFG and <b>A</b>-values, an observation, which cannot be rationalized by DFT assisted crystal-field theory. In contrast, ORCA/CASSCF calculations for the ZFS tensor in combination with DFT calculations for the EFG- and <b>A</b>-tensors describe the experimental data remarkably well

    Spectroscopic and Theoretical Study of Spin-Dependent Electron Transfer in an Iron(III) Superoxo Complex

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    It was shown previously (<i>J. Am. Chem. Soc.</i> <b>2014</b>, <i>136</i>, 10846) that bubbling of O<sub>2</sub> into a solution of Fe<sup>II</sup>(BDPP) (H<sub>2</sub>BDPP = 2,6-bisĀ­[[(<i>S</i>)-2-(diphenylhydroxymethyl)-1-pyrrolidinyl]Ā­methyl]Ā­pyridine) in tetrahydrofuran at āˆ’80 Ā°C generates a high-spin (<i>S</i><sub>Fe</sub> = <sup>5</sup>/<sub>2</sub>) ironĀ­(III) superoxo adduct, <b>1</b>. MoĢˆssbauer studies revealed that <b>1</b> is an exchange-coupled system, HĢ‚ex=JSĢ‚FeĀ·SĢ‚R, where <i>S</i><sub>R</sub> = <sup>1</sup>/<sub>2</sub> is the spin of the superoxo radical, of which the spectra were not well enough resolved to determine whether the coupling was ferromagnetic (<i>S</i> = 3 ground state) or antiferromagnetic (<i>S</i> = 2). The glass-forming 2-methyltetrahydrofuran solvent yields highly resolved MoĢˆssbauer spectra from which the following data have been extracted: (i) the ground state of <b>1</b> has <i>S</i> = 3 (<i>J</i> < 0); (ii) |<i>J</i>| > 15 cm<sup>ā€“1</sup>; (iii) the zero-field-splitting parameters are <i>D</i> = āˆ’1.1 cm<sup>ā€“1</sup> and <i>E</i>/<i>D</i> = 0.02; (iv) the major component of the electric-field-gradient tensor is tilted ā‰ˆ7Ā° relative to the easy axis of magnetization determined by the <i>M</i><sub><i>S</i></sub> = Ā±3 and Ā±2 doublets. The excited-state <i>M</i><sub><i>S</i></sub> = Ā±2 doublet yields a narrow parallel-mode electron paramagnetic resonance signal at <i>g</i> = 8.03, which was used to probe the magnetic hyperfine splitting of <sup>17</sup>O-enriched O<sub>2</sub>. A theoretical model that considers spin-dependent electron transfer for the cases where the doubly occupied Ļ€* orbital of the superoxo ligand is either ā€œinā€ or ā€œoutā€ of the plane defined by the bent Feā€“OO moiety correctly predicts that <b>1</b> has an <i>S</i> = 3 ground state, in contrast to the density functional theory calculations for <b>1</b>, which give a ground state with both the wrong spin and orbital configuration. This failure has been traced to a basis set superposition error in the interactions between the superoxo moiety and the adjacent five-membered rings of the BDPP ligand and signals a fundamental problem in the quantum chemistry of O<sub>2</sub> activation

    A Long-Lived Fe<sup>III</sup>-(Hydroperoxo) Intermediate in the Active H200C Variant of Homoprotocatechuate 2,3-Dioxygenase: Characterization by MoĢˆssbauer, Electron Paramagnetic Resonance, and Density Functional Theory Methods

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    The extradiol-cleaving dioxygenase homoprotocatechuate 2,3-dioxygenase (HPCD) binds substrate homoprotocatechuate (HPCA) and O<sub>2</sub> sequentially in adjacent ligand sites of the active site Fe<sup>II</sup>. Kinetic and spectroscopic studies of HPCD have elucidated catalytic roles of several active site residues, including the crucial acidā€“base chemistry of His200. In the present study, reaction of the His200Cys (H200C) variant with native substrate HPCA resulted in a decrease in both <i>k</i><sub>cat</sub> and the rate constants for the activation steps following O<sub>2</sub> binding by >400 fold. The reaction proceeds to form the correct extradiol product. This slow reaction allowed a long-lived (<i>t</i><sub>1/2</sub> = 1.5 min) intermediate, H200C-HPCA<sub>Int1</sub> (<i>Int1</i>), to be trapped. MoĢˆssbauer and parallel mode electron paramagnetic resonance (EPR) studies show that <i>Int1</i> contains an <i>S</i><sub>1</sub> = 5/2 Fe<sup>III</sup> center coupled to an <i>S</i><sub>R</sub> = 1/2 radical to give a ground state with total spin <i>S</i> = 2 (<i>J</i> > 40 cm<sup>ā€“1</sup>) in Hexch=JSĢ‚1Ā·SĢ‚R. Density functional theory (DFT) property calculations for structural models suggest that <i>Int1</i> is a (HPCA semiquinone<sup>ā€¢</sup>)Ā­Fe<sup>III</sup>(OOH) complex, in which OOH is protonated at the distal O and the substrate hydroxyls are deprotonated. By combining MoĢˆssbauer and EPR data of <i>Int1</i> with DFT calculations, the orientations of the principal axes of the <sup>57</sup>Fe electric field gradient and the zero-field splitting tensors (<i>D</i> = 1.6 cm<sup>ā€“1</sup>, <i>E</i>/<i>D</i> = 0.05) were determined. This information was used to predict hyperfine splittings from bound <sup>17</sup>OOH. DFT reactivity analysis suggests that <i>Int1</i> can evolve from a ferromagnetically coupled Fe<sup>III</sup>-superoxo precursor by an inner-sphere proton-coupled-electron-transfer process. Our spectroscopic and DFT results suggest that a ferric hydroperoxo species is capable of extradiol catalysis

    Spectroscopic Identification of an Fe<sup>III</sup> Center, not Fe<sup>IV</sup>, in the Crystalline Scā€“Oā€“Fe Adduct Derived from [Fe<sup>IV</sup>(O)(TMC)]<sup>2+</sup>

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    The apparent Sc<sup>3+</sup> adduct of [Fe<sup>IV</sup>(O)Ā­(TMC)]<sup>2+</sup> (<b>1</b>, TMC = 1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclotetradecane) has been synthesized in amounts sufficient to allow its characterization by various spectroscopic techniques. Contrary to the earlier assignment of a +4 oxidation state for the iron center of <b>1</b>, we establish that <b>1</b> has a high-spin ironĀ­(III) center based on its MoĢˆssbauer and EPR spectra and its quantitative reduction by 1 equiv of ferrocene to [Fe<sup>II</sup>(TMC)]<sup>2+</sup>. Thus, <b>1</b> is best described as a Sc<sup>III</sup>ā€“Oā€“Fe<sup>III</sup> complex, in agreement with previous DFT calculations (Swart, M. Chem. Commun. 2013, 49, 6650.). These results shed light on the interaction of Lewis acids with high-valent metal-oxo species
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