33 research outputs found

    Magnetic Properties and Electronic Structure of Manganese-Based Blue Pigments: A High-Frequency and -Field EPR Study

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    A variety of new oxide-based materials based on hexagonal phase of YInO<sub>3</sub> have been recently described. In some of these materials, the InĀ­(III) ions are substituted by MnĀ­(III), which finds itself in a trigonal-bipyramidal (TBP) coordination environment. While YInO<sub>3</sub> is colorless and YMnO<sub>3</sub> is black, mixed systems YIn<sub>1ā€“<i>x</i></sub>Mn<sub><i>x</i></sub>O<sub>3</sub> (0.02 < <i>x</i> < 0.25) display intense blue color and have been proposed as novel blue pigments. Since the MnĀ­(III) ion is paramagnetic, its presence imparts distinct magnetic properties to the whole class of materials. These properties were investigated by electron paramagnetic resonance (EPR) in its high-frequency and -field version (HFEPR), a technique ideally suited for transition metal ions such as MnĀ­(III) that, in contrast to, for example, MnĀ­(II), are difficult to study by EPR at (conventional) low frequency and field. YIn<sub>1ā€“<i>x</i></sub>Mn<sub><i>x</i></sub>O<sub>3</sub> with 0.02 < <i>x</i> < 0.2 exhibited high-quality HFEPR spectra up to room temperature that could be interpreted as arising from isolated <i>S</i> = 2 paramagnets. A simple ligand-field model, based on the structure and optical spectra, explains the spin Hamiltonian parameters provided by HFEPR, which were <i>D</i> = +3.0 cm<sup>ā€“1</sup>, <i>E</i> = 0; <i>g</i><sub>āŠ„</sub> = 1.99, <i>g</i><sub>āˆ„</sub> = 2.0. This study demonstrates the general applicability of a combined spectroscopic and classical theoretical approach to understanding the electronic structure of novel materials containing paramagnetic dopants. Moreover, HFEPR complements optical and other experimental methods as being a sensitive probe of dopant level

    Observation of a Photogenerated Rh<sub>2</sub> Nitrenoid Intermediate in Cā€“H Amination

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    Rh<sub>2</sub>-catalyzed Cā€“H amination is a powerful method for nitrogenating organic molecules. While Rh<sub>2</sub> nitrenoids are often invoked as reactive intermediates in these reactions, the exquisite reactivity and fleeting lifetime of these species has precluded their observation. Here, we report the photogeneration of a transient Rh<sub>2</sub> nitrenoid that participates in Cā€“H amination. The developed approach to Rh<sub>2</sub> nitrenoids, based on photochemical cleavage of Nā€“Cl bonds in <i>N</i>-chloroamido ligands, has enabled characterization of a reactive Rh<sub>2</sub> nitrenoid by mass spectrometry and transient absorption spectroscopy. We anticipate that photogeneration of metal nitrenoids will contribute to the development of Cā€“H amination catalysis by providing tools to directly study the structures of these critical intermediates

    High Spin Co(I): High-Frequency and -Field EPR Spectroscopy of CoX(PPh<sub>3</sub>)<sub>3</sub> (X = Cl, Br)

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    The previously reported pseudotetrahedral CoĀ­(I) complexes, CoXĀ­(PR<sub>3</sub>)<sub>3</sub>, where R = Me, Ph, and chelating analogues, and X = Cl, Br, I exhibit a spin triplet ground state, which is uncommon for CoĀ­(I), although expected for this geometry. Described here are studies using electronic absorption and high-frequency and -field electron paramagnetic resonance (HFEPR) spectroscopy on two members of this class of complexes: CoXĀ­(PR<sub>3</sub>)<sub>3</sub>, where R = Ph and X = Cl and Br. In both cases, well-defined spectra corresponding to axial spin triplets were observed, with signals assignable to three distinct triplet species, and with perfectly axial zero-field splitting (zfs) given by the parameter <i>D</i> = +4.46, +5.52, +8.04 cm<sup>ā€“1</sup>, respectively, for CoClĀ­(PPh<sub>3</sub>)<sub>3</sub>. The crystal structure reported for CoClĀ­(PPh<sub>3</sub>)<sub>3</sub> shows crystallographic 3-fold symmetry, but with three structurally distinct molecules per unit cell. Both of these facts thus correlate with the HFEPR data. The investigated complexes, along with a number of structurally characterized CoĀ­(I) trisphosphine analogues, were analyzed by quantum chemistry calculations (both density functional theory (DFT) and unrestricted Hartreeā€“Fock (UHF) methods). These methods, along with ligand-field theory (LFT) analysis of CoClĀ­(PPh<sub>3</sub>)<sub>3</sub>, give reasonable agreement with the salient features of the electronic structure of these complexes. A spin triplet ground state is strongly favored over a singlet state and a positive, axial <i>D</i> value is predicted, in agreement with experiment. Quantitative agreement between theory and experiment is less than ideal with LFT overestimating the zfs, while DFT underestimates these effects. Despite these shortcomings, this study demonstrates the ability of advanced paramagnetic resonance techniques, in combination with other experimental techniques, and with theory, to shed light on the electronic structure of an unusual transition metal ion, paramagnetic CoĀ­(I)

    Synthesis, Characterization, and Electrochemical Analyses of Vanadocene Tetrametaphosphate and Phosphinate Derivatives

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    The synthesis and characterization of a series of new vanadocene-derived tetrametaphosphate or diphenylphosphinate complexes, [PPN]<sub>2</sub>[CpVĀ­(P<sub>4</sub>O<sub>12</sub>)] (<b>1</b>), [Cp<sub>2</sub>VOPĀ­(O)Ā­Ph<sub>2</sub>] (<b>2</b>), [CpVĀ­(Ī¼<sup>2</sup>-O<sub>2</sub>PPh<sub>2</sub>)<sub>4</sub>VCp] (<b>3</b>), and [Cp<sub>2</sub>VĀ­(Ī¼<sup>2</sup>-O<sub>2</sub>PPh<sub>2</sub>)<sub>2</sub>VCp<sub>2</sub>]Ā­[PF<sub>6</sub>]<sub>2</sub> (<b>4</b>), is reported ([PPN]<sup>+</sup> = bisĀ­(triphenylphosphoranylidene)Ā­ammonium; Cp = Ī·<sup>5</sup>-cyclopentadienyl). The complexes were synthesized from the methyl vanadocene (Cp<sub>2</sub>VMe) precursor, through protonation of the Me or Cp linkages using the tetrametaphosphate or phosphinate acid precursors [PPN]<sub>2</sub>[P<sub>4</sub>O<sub>12</sub>H<sub>2</sub>] (for <b>1</b>) and Ph<sub>2</sub>PĀ­(O)Ā­OH (for <b>2</b> and <b>3</b>). Oxidation of <b>2</b> with [Fc]Ā­[PF<sub>6</sub>] resulted in dimerization, yielding the bimetallic <b>4</b> ([Fc]<sup>+</sup> = ferrocenium). Electrochemical analysis of this reaction revealed a possible ECE mechanism that includes prior and subsequent electron transfer to this dimerization. The electronic structure of the dimer <b>4</b> was probed by SQUID magnetommetry and X-band EPR spectroscopy (100 and 4 K). The dimer was found to contain two antiferromagnetically coupled V<sup>IV</sup> centers, as well as a small portion of monomeric V<sup>IV</sup> species, <b>2</b><sup><b>+</b></sup>. In contrast to <b>2</b>, oxidation of <b>1</b> resulted in an EC mechanism, the product of which remains unknown. Preliminary reactions with compounds <b>1</b> and <b>2</b> bearing free Pī—»O groups were performed using H atom donors to test their ability to undergo H atom transfer in the context of the proposed ā€œreduction-coupled oxo activationā€ mechanism; however, no clear reaction pathway supporting this mechanism has yet been observed

    Secondary Coordination Sphere Effects in Ruthenium(III) Tetraammine Complexes: Role of the Coordinated Water Molecule

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    The complexes <i>trans</i>-[Ru<sup>III</sup>(NH<sub>3</sub>)<sub>4</sub>(4-pic)Ā­(H<sub>2</sub>O)]Ā­(CF<sub>3</sub>SO<sub>3</sub>)<sub>3</sub> (<b>1</b>) and [Ru<sup>III</sup>(NH<sub>3</sub>)<sub>5</sub>(4-pic)]Ā­(CF<sub>3</sub>SO<sub>3</sub>)<sub>3</sub> (<b>2</b>) were isolated and studied experimentally by electron paramagnetic resonance (EPR) and UVā€“vis spectroscopies, cyclic voltammetry, and X-ray crystallography and theoretically by ligand-field theory (LFT) and density functional theory (DFT) calculations. Complex <b>1</b> is reported in two different crystal forms, <b>1a</b> (100 K) and <b>1b</b> (room temperature). EPR and UVā€“vis spectroscopies suggest that aqua ligand interaction in this low-spin rutheniumĀ­(III) complex changes as a function of hydrogen bonding with solvent molecules. This explicit water solvent effect was explained theoretically by DFT calculations, which demonstrated the effect of rotation of the aqua ligand about the N<sub>pic</sub>ā€“Ruā€“O<sub>aq</sub> axis. The UVā€“vis spectrum of <b>1</b> shows in an aqueous acid solution a broad- and low-intensity absorption band around 28ā€Æ500 cm<sup>ā€“1</sup> (Īµ ā‰ˆ 500 M<sup>ā€“1</sup> cm<sup>ā€“1</sup>) that is assigned mainly to a charge-transfer (CT) transition from the equatorial ligands to the Ru Ī²-4d<sub><i>xy</i></sub> orbital (Ī²-LUMO) using DFT calculations. The electronic reflectance spectrum of <b>1</b> shows a broad and intense absorption band around 25ā€Æ500 cm<sup>ā€“1</sup> that is assigned to a CT transition from 4-picoline to the Ru Ī²-4d<sub><i>xz</i></sub> orbital (Ī²-LUMO) using DFT calculations. The t<sub>2g</sub><sup>5</sup> set of orbitals had its energy splitting investigated by LFT. LFT analysis shows that a rhombic component arises from <i>C</i><sub>2<i>v</i></sub> symmetry by a simple Ļ€-bonding ligand (H<sub>2</sub>O in our case) twisting about the trans (<i>C</i><sub>2</sub>) axis. This twist was manifested in the EPR spectra, which were recorded for <b>1</b> as a function of the solvent in comparison with [RuĀ­(NH<sub>3</sub>)<sub>5</sub>(4-pic)]<sup>3+</sup> and [RuĀ­(NH<sub>3</sub>)<sub>5</sub>(H<sub>2</sub>O)]<sup>3+</sup>. Only <b>1</b> shows an evident change in the <b>g</b>-tensor values, wherein an increased rhombic component is correlated with a higher nucleophilicity (donor) solvent feature, as parametrized by the Abraham system

    Secondary Coordination Sphere Effects in Ruthenium(III) Tetraammine Complexes: Role of the Coordinated Water Molecule

    No full text
    The complexes <i>trans</i>-[Ru<sup>III</sup>(NH<sub>3</sub>)<sub>4</sub>(4-pic)Ā­(H<sub>2</sub>O)]Ā­(CF<sub>3</sub>SO<sub>3</sub>)<sub>3</sub> (<b>1</b>) and [Ru<sup>III</sup>(NH<sub>3</sub>)<sub>5</sub>(4-pic)]Ā­(CF<sub>3</sub>SO<sub>3</sub>)<sub>3</sub> (<b>2</b>) were isolated and studied experimentally by electron paramagnetic resonance (EPR) and UVā€“vis spectroscopies, cyclic voltammetry, and X-ray crystallography and theoretically by ligand-field theory (LFT) and density functional theory (DFT) calculations. Complex <b>1</b> is reported in two different crystal forms, <b>1a</b> (100 K) and <b>1b</b> (room temperature). EPR and UVā€“vis spectroscopies suggest that aqua ligand interaction in this low-spin rutheniumĀ­(III) complex changes as a function of hydrogen bonding with solvent molecules. This explicit water solvent effect was explained theoretically by DFT calculations, which demonstrated the effect of rotation of the aqua ligand about the N<sub>pic</sub>ā€“Ruā€“O<sub>aq</sub> axis. The UVā€“vis spectrum of <b>1</b> shows in an aqueous acid solution a broad- and low-intensity absorption band around 28ā€Æ500 cm<sup>ā€“1</sup> (Īµ ā‰ˆ 500 M<sup>ā€“1</sup> cm<sup>ā€“1</sup>) that is assigned mainly to a charge-transfer (CT) transition from the equatorial ligands to the Ru Ī²-4d<sub><i>xy</i></sub> orbital (Ī²-LUMO) using DFT calculations. The electronic reflectance spectrum of <b>1</b> shows a broad and intense absorption band around 25ā€Æ500 cm<sup>ā€“1</sup> that is assigned to a CT transition from 4-picoline to the Ru Ī²-4d<sub><i>xz</i></sub> orbital (Ī²-LUMO) using DFT calculations. The t<sub>2g</sub><sup>5</sup> set of orbitals had its energy splitting investigated by LFT. LFT analysis shows that a rhombic component arises from <i>C</i><sub>2<i>v</i></sub> symmetry by a simple Ļ€-bonding ligand (H<sub>2</sub>O in our case) twisting about the trans (<i>C</i><sub>2</sub>) axis. This twist was manifested in the EPR spectra, which were recorded for <b>1</b> as a function of the solvent in comparison with [RuĀ­(NH<sub>3</sub>)<sub>5</sub>(4-pic)]<sup>3+</sup> and [RuĀ­(NH<sub>3</sub>)<sub>5</sub>(H<sub>2</sub>O)]<sup>3+</sup>. Only <b>1</b> shows an evident change in the <b>g</b>-tensor values, wherein an increased rhombic component is correlated with a higher nucleophilicity (donor) solvent feature, as parametrized by the Abraham system

    Mechanistic Studies of the Spore Photoproduct Lyase via a Single Cysteine Mutation

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    5-Thyminyl-5,6-dihydrothymine (also called spore photoproduct or SP) is the exclusive DNA photodamage product in bacterial endospores. It is repaired by a radical SAM (<i>S</i>-adenosylmethionine) enzyme, the spore photoproduct lyase (SPL), at the bacterial early germination phase. Our previous studies proved that SPL utilizes the 5ā€²-dAā€¢ generated by the SAM cleavage reaction to abstract the H<sub>6pro<i>R</i></sub> atom to initiate the SP repair process. The resulting thymine allylic radical was suggested to take an H atom from an unknown protein source, most likely cysteine 141. Here we show that C141 can be readily alkylated in the native SPL by an iodoacetamide treatment, suggesting that it is accessible to the TpT radical. SP repair by the SPL C141A mutant yields TpTSO<sub>2</sub><sup>ā€“</sup> and TpT simultaneously from the very beginning of the reaction; no lag phase is observed for TpTSO<sub>2</sub><sup>ā€“</sup> formation. Should any other protein residue serve as the H donor, its presence would result in TpT being the major product at least for the first enzyme turnover. These observations provide strong evidence to support C141 as the direct H atom donor. Moreover, because of the lack of this intrinsic H donor, the C141A mutant produces TpT via an unprecedented thymine cation radical reduction (proton-coupled electron transfer) process, contrasting to the H atom transfer mechanism in the wild-type (WT) SPL reaction. The C141A mutant repairs SP at a rate that is āˆ¼3-fold slower than that of the WT enzyme. Formation of TpTSO<sub>2</sub><sup>ā€“</sup> and TpT exhibits a <i>V</i><sub>max</sub> deuterium kinetic isotope effect (KIE) of 1.7 Ā± 0.2, which is smaller than the <sup>D</sup><i>V</i><sub>max</sub> KIE of 2.8 Ā± 0.3 determined for the WT SPL reaction. These findings suggest that removing the intrinsic H atom donor disturbs the rate-limiting process during enzyme catalysis. As expected, the prereduced C141A mutant supports only āˆ¼0.4 turnover, which is in sharp contrast to the >5 turnovers exhibited by the WT SPL reaction, suggesting that the enzyme catalytic cycle (SAM regeneration) is disrupted by this single mutation

    HFEPR and Computational Studies on the Electronic Structure of a High-Spin Oxidoiron(IV) Complex in Solution

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    Nonheme iron enzymes perform diverse and important functions in biochemistry. The active form of these enzymes comprises the ferryl, oxidoironĀ­(IV), [FeO]<sup>2+</sup> unit. In enzymes, this unit is in the high-spin, quintet, <i>S</i> = 2, ground state, while many synthetic model compounds exist in the spin triplet, <i>S</i> = 1, ground state. Recently, however, Que and co-workers reported an oxidoironĀ­(IV) complex with a quintet ground state, [FeOĀ­(TMG<sub>3</sub>tren)]Ā­(OTf)<sub>2</sub>, where TMG<sub>3</sub>tren = 1,1,1-trisĀ­{2-[<i>N</i>2-(1,1,3,3-tetramethylguanidino)]Ā­ethyl}Ā­amine and OTf = CF<sub>3</sub>SO<sub>3</sub><sup>ā€“</sup>. The trigonal geometry imposed by this ligand, as opposed to the tetragonal geometry of earlier model complexes, favors the high-spin ground state. Although [FeOĀ­(TMG<sub>3</sub>tren)]<sup>2+</sup> has been earlier probed by magnetic circular dichroism (MCD) and MoĢˆssbauer spectroscopies, the technique of high-frequency and -field electron paramagnetic resonance (HFEPR) is superior for describing the electronic structure of the ironĀ­(IV) center because of its ability to establish directly the spin-Hamiltonian parameters of high-spin metal centers with high precision. Herein we describe HFEPR studies on [FeOĀ­(TMG<sub>3</sub>tren)]Ā­(OTf)<sub>2</sub> generated in situ and confirm the <i>S</i> = 2 ground state with the following parameters: <i>D</i> = +4.940(5) cm<sup>ā€“1</sup>, <i>E</i> = 0.000(5), <i>B</i><sub>4</sub><sup>0</sup> = āˆ’14(1) Ɨ 10<sup>ā€“4</sup> cm<sup>ā€“1</sup>, <i>g</i><sub>āŠ„</sub> = 2.006(2), and <i>g</i><sub>āˆ„</sub> = 2.03(2). Extraction of a fourth-order spin-Hamiltonian parameter is unusual for HFEPR and impossible by other techniques. These experimental results are combined with state-of-the-art computational studies along with previous structural and spectroscopic results to provide a complete picture of the electronic structure of this biomimetic complex. Specifically, the calculations reproduce well the spin-Hamiltonian parameters of the complex, provide a satisfying geometrical picture of the <i>S</i> = 2 oxidoironĀ­(IV) moiety, and demonstrate that the TMG<sub>3</sub>tren is an ā€œinnocentā€ ligand

    A Neutrally Charged Trimethylmanganese(III) Complex: Synthesis, Characterization, and Disproportionation Chemistry

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    The synthesis and properties of an unusual, neutrally charged and volatile <i>N</i>,<i>N</i>,<i>N</i>ā€²,<i>N</i>ā€²-tetramethylethylenediamine trimethyl manganeseĀ­(III) complex, (TMEDA)Ā­MnMe<sub>3</sub>, are described, along with its facile disproportionation to the corresponding MnĀ­(II) and MnĀ­(IV) complexes. Characterization by single-crystal XRD, UVā€“vis spectroscopy, high-frequency and -field EPR (HFEPR), magnetic susceptibility, and density functional theory (DFT) computations indicate that the (TMEDA)Ā­MnMe<sub>3</sub> electronic structure can be described as largely square pyramidal MnĀ­(III) centered. The paucity of manganeseĀ­(III) polyalkyls and the simplicity and reactivity of this compound implicate it as a potentially useful synthetic building block

    Ligand Substituent Effects in Manganese Pyridinophane Complexes: Implications for Oxygen-Evolving Catalysis

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    A series of MnĀ­(II) complexes of differently substituted pyridinophane ligands, (Py<sub>2</sub>NR<sub>2</sub>)Ā­MnCl<sub>2</sub> (R = <i><sup>i</sup></i>Pr, Cy) and [(Py<sub>2</sub>NR<sub>2</sub>)Ā­MnF<sub>2</sub>]Ā­(PF<sub>6</sub>) (R = <i><sup>i</sup></i>Pr, Cy, <i><sup>t</sup></i>Bu) are synthesized and characterized. The electrochemical properties of these complexes are investigated by cyclic voltammetry, along with those of previously reported (Py<sub>2</sub>NMe<sub>2</sub>)Ā­MnCl<sub>2</sub> and the MnĀ­(III) complex [(Py<sub>2</sub>NMe<sub>2</sub>)Ā­MnF<sub>2</sub>]Ā­(PF<sub>6</sub>). The electronic structure of this and other MnĀ­(III) complexes is probed experimentally and theoretically, via high-frequency and -field electron paramagnetic resonance (HFEPR) spectroscopy ab initio quantum chemical theory (QCT), respectively. These studies show that the complexes contain relatively typical six-coordinate MnĀ­(III). The catalytic activity of these complexes toward both H<sub>2</sub>O<sub>2</sub> disproportionation and H<sub>2</sub>O oxidation has also been investigated. The rate of H<sub>2</sub>O<sub>2</sub> disproportionation decreases with increasing substituent size. Some of these complexes are active for electrocatalytic H<sub>2</sub>O oxidation; however this activity cannot be rationalized in terms of simple electronic or steric effects
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