16 research outputs found

    An efficient one-pot synthesis of carbazole fused benzoquinolines and pyridocarbazoles

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    Cobalt­(II), in the presence of acetate and nitrate, quantitatively adds to the manganese–cobalt oxido cubane Mn<sup>IV</sup>Co<sup>III</sup><sub>3</sub>O<sub>4</sub>(OAc)<sub>5</sub>(py)<sub>3</sub> (<b>1</b>) to furnish the pentametallic dangler complex Mn<sup>IV</sup>Co<sup>III</sup><sub>3</sub>Co<sup>II</sup>O<sub>4</sub>(OAc)<sub>6</sub>(NO<sub>3</sub>)­(py)<sub>3</sub> (<b>2</b>). Complex <b>2</b> is structurally reminiscent of photosystem II’s oxygen-evolving center, and is a rare example of a transition-metal “dangler” complex. Superconducting quantum interference device magnetometry and density functional theory calculations characterize <b>2</b> as having an <i>S</i> = 0 ground state arising from antiferromagnetic coupling between the Co<sup>II</sup> and Mn<sup>IV</sup> ions. At higher temperatures, an uncoupled state dominates. The voltammogram of <b>2</b> has four electrochemical events, two more than that of its parent cubane <b>1</b>, suggesting that addition of the dangler increases available redox states. Structural, electrochemical, and magnetic comparisons of complexes <b>1</b> and <b>2</b> allow a better understanding of the dangler’s influence on a cubane

    Control of Electronic Structure and Conductivity in Two-Dimensional Metal–Semiquinoid Frameworks of Titanium, Vanadium, and Chromium

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    The isostructural, two-dimensional metal–organic frameworks (H2NMe2)2M2­(Cl2dhbq)3 (M = Ti, V; Cl2dhbqn– = deprotonated 2,5-dichloro-3,6-dihydroxybenzoquinone) and (H2NMe2)1.5Cr2­(dhbq)3 (dhbqn– = deprotonated 2,5-dihydroxybenzoquinone) are synthesized and investigated by spectroscopic, magnetic, and electrochemical methods. The three frameworks exhibit substantial differences in their electronic structures, and the bulk electronic conductivities of these phases correlate with the extent of delocalization observed via UV–vis–NIR and IR spectroscopies. Notably, substantial metal–ligand covalency in the vanadium phase results in the quenching of ligand-based spins, the observation of simultaneous metal- and ligand-based redox processes, and a high electronic conductivity of 0.45 S/cm. A molecular orbital analysis of these materials and a previously reported iron congener suggests that the differences in conductivity can be explained by correlating the metal–ligand energy alignment with the energy of intervalence charge-transfer transitions, which should determine the barrier to charge hopping in the mixed-valence frameworks

    Synthesis and O<sub>2</sub> Reactivity of a Titanium(III) Metal–Organic Framework

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    Metal–organic frameworks featuring pores lined with exposed metal cations have received attention for a wide range of adsorption-related applications. While many frameworks with coordinatively unsaturated M<sup>II</sup> centers have been reported, there are relatively few examples of porous materials with coordinatively unsaturated M<sup>III</sup> centers. Here, we report the synthesis and characterization of Ti<sub>3</sub>O­(OEt)­(bdc)<sub>3</sub>(solv)<sub>2</sub> (Ti-MIL-101; bdc<sup>2–</sup> = 1,4-benzenedicarboxylate; solv = <i>N</i>,<i>N</i>-dimethylformamide, tetrahydrofuran), the first metal–organic framework containing exclusively Ti<sup>III</sup> centers. Through a combination of gas adsorption, X-ray diffraction, magnetic susceptibility, and electronic and vibrational spectroscopy measurements, this high-surface-area framework is shown to contain five-coordinate Ti<sup>III</sup> centers upon desolvation, which irreversibly bind O<sub>2</sub> to form titanium­(IV) superoxo and peroxo species. Electronic absorption spectra suggest that the five-coordinate Ti<sup>III</sup> sites adopt a distorted trigonal-bipyramidal geometry that effectively shields nuclear charge and inhibits strong adsorption of nonredox-active gases

    Electronic Conductivity, Ferrimagnetic Ordering, and Reductive Insertion Mediated by Organic Mixed-Valence in a Ferric Semiquinoid Metal–Organic Framework

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    A three-dimensional network solid composed of Fe<sup>III</sup> centers and para­magnetic semi­quinoid linkers, (NBu<sub>4</sub>)<sub>2</sub>­Fe<sup>III</sup><sub>2</sub>­(dhbq)<sub>3</sub> (dhbq<sup>2–/3–</sup> = 2,5-dioxido­benzo­quinone/​1,2-dioxido-4,5-semi­quinone), is shown to exhibit a conductivity of 0.16 ± 0.01 S/cm at 298 K, one of the highest values yet observed for a metal–organic framework (MOF). The origin of this electronic conductivity is determined to be ligand mixed-valency, which is characterized using a suite of spectro­scopic techniques, slow-scan cyclic voltammetry, and variable-temperature conductivity and magnetic susceptibility measurements. Importantly, UV–vis–NIR diffuse reflectance measurements reveal the first observation of Robin–Day Class II/III mixed valency in a MOF. Pursuit of stoichio­metric control over the ligand redox states resulted in synthesis of the reduced frame­work material Na<sub>0.9</sub>­(NBu<sub>4</sub>)<sub>1.8</sub>Fe<sup>III</sup><sub>2</sub>(dhbq)<sub>3</sub>. Differences in electronic conductivity and magnetic ordering temperature between the two compounds are investigated and correlated to the relative ratio of the two different ligand redox states. Overall, the transition metal–semi­quinoid system is established as a particularly promising scaffold for achieving tunable long-range electronic communication in MOFs

    Trimethylsilyl versus Bis(trimethylsilyl) Substitution in Tris(cyclopentadienyl) Complexes of La, Ce, and Pr: Comparison of Structure, Magnetic Properties, and Reactivity

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    To evaluate the effect of cyclopentadienyl ligand substitution in complexes of new +2 ions of the lanthanides, comparisons in reactivity and spectroscopic and magnetic properties have been made between [K­(crypt)]­[Cp′<sub>3</sub>Ln], <b>1-Ln</b> (Cp′ = C<sub>5</sub>H<sub>4</sub>SiMe<sub>3</sub>; crypt = 2.2.2-cryptand; Ln = La, Ce, Pr, and Nd), and [K­(crypt)]­[Cp′′<sub>3</sub>Ln], <b>2-Ln</b> [Cp′′ = C<sub>5</sub>H<sub>3</sub>(SiMe<sub>3</sub>)<sub>2</sub>]. The <b>2-Ln</b> complexes (Ce, Pr, and Nd) were synthesized by reduction of Cp′′<sub>3</sub>Ln with potassium graphite in the presence of crypt and crystallographically characterized. The structures and UV–visible spectra of <b>2-Ln</b> are similar to those of <b>1-Ln</b>, as expected, but greater thermal stability for <b>2-Ln</b>, expected from comparisons of <b>2-U</b> and <b>1-U</b>, was not observed. The magnetic susceptibilities of <b>2-Ce</b> and <b>2-Pr</b> were investigated because those of <b>1-Ce</b> and <b>1-Pr</b> did not match simple coupling models for 4f<sup><i>n</i></sup>5d<sup>1</sup> electron configurations. The magnetic data of the <b>2-Ln</b> complexes are similar to those of <b>1-Ln</b>, which suggests that Ce<sup>2+</sup> and Pr<sup>2+</sup> complexes with 4f<sup><i>n</i></sup>5d<sup>1</sup> electron configurations may have more complex electronic structures compared to nontraditional divalent complexes of the later lanthanides. Reactivity studies of isolated samples of <b>1-Ln</b> and <b>2-Ln</b> with 1,2-dimethoxyethane (DME) were conducted to determine if methoxide products, found in previous <i>in situ</i> studies of the synthesis of <b>2-Ln</b> by Lappert and co-workers, would form. Methoxide products were not observed, which shows that the chemistry of the isolated complexes differs from that of the <i>in situ</i> reduction reactions

    Electronic Conductivity, Ferrimagnetic Ordering, and Reductive Insertion Mediated by Organic Mixed-Valence in a Ferric Semiquinoid Metal–Organic Framework

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    A three-dimensional network solid composed of Fe<sup>III</sup> centers and para­magnetic semi­quinoid linkers, (NBu<sub>4</sub>)<sub>2</sub>­Fe<sup>III</sup><sub>2</sub>­(dhbq)<sub>3</sub> (dhbq<sup>2–/3–</sup> = 2,5-dioxido­benzo­quinone/​1,2-dioxido-4,5-semi­quinone), is shown to exhibit a conductivity of 0.16 ± 0.01 S/cm at 298 K, one of the highest values yet observed for a metal–organic framework (MOF). The origin of this electronic conductivity is determined to be ligand mixed-valency, which is characterized using a suite of spectro­scopic techniques, slow-scan cyclic voltammetry, and variable-temperature conductivity and magnetic susceptibility measurements. Importantly, UV–vis–NIR diffuse reflectance measurements reveal the first observation of Robin–Day Class II/III mixed valency in a MOF. Pursuit of stoichio­metric control over the ligand redox states resulted in synthesis of the reduced frame­work material Na<sub>0.9</sub>­(NBu<sub>4</sub>)<sub>1.8</sub>Fe<sup>III</sup><sub>2</sub>(dhbq)<sub>3</sub>. Differences in electronic conductivity and magnetic ordering temperature between the two compounds are investigated and correlated to the relative ratio of the two different ligand redox states. Overall, the transition metal–semi­quinoid system is established as a particularly promising scaffold for achieving tunable long-range electronic communication in MOFs

    Reversible CO Scavenging via Adsorbate-Dependent Spin State Transitions in an Iron(II)–Triazolate Metal–Organic Framework

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    A new metal–organic framework, Fe-BTTri (Fe3[(Fe4Cl)3(BTTri)8]2·18CH3OH, H3BTTri =1,3,5-tris­(1H-1,2,3-triazol-5-yl)­benzene)), is found to be highly selective in the adsorption of CO over a variety of other gas molecules, making it extremely effective, for example, in the removal of trace CO from mixtures with H2, N2, and CH4. This framework not only displays significant CO adsorption capacity at very low pressures (1.45 mmol/g at just 100 μbar), but, importantly, also exhibits readily reversible CO binding. Fe-BTTri utilizes a unique spin state change mechanism to bind CO in which the coordinatively unsaturated, high-spin FeII centers of the framework convert to octahedral, low-spin FeII centers upon CO coordination. Desorption of CO converts the FeII sites back to a high-spin ground state, enabling the facile regeneration and recyclability of the material. This spin state change is supported by characterization via infrared spectroscopy, single crystal X-ray analysis, Mössbauer spectroscopy, and magnetic susceptibility measurements. Importantly, the spin state change is selective for CO and is not observed in the presence of other gases, such as H2, N2, CO2, CH4, or other hydrocarbons, resulting in unprecedentedly high selectivities for CO adsorption for use in CO/H2, CO/N2, and CO/CH4 separations and in preferential CO adsorption over typical strongly adsorbing gases like CO2 and ethylene. While adsorbate-induced spin state transitions are well-known in molecular chemistry, particularly for CO, to our knowledge this is the first time such behavior has been observed in a porous material suitable for use in a gas separation process. Potentially, this effect can be extended to selective separations involving other π-acids

    Reversible CO Scavenging via Adsorbate-Dependent Spin State Transitions in an Iron(II)–Triazolate Metal–Organic Framework

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    A new metal–organic framework, Fe-BTTri (Fe<sub>3</sub>[(Fe<sub>4</sub>Cl)<sub>3</sub>(BTTri)<sub>8</sub>]<sub>2</sub>·18CH<sub>3</sub>OH, H<sub>3</sub>BTTri =1,3,5-tris­(1<i>H</i>-1,2,3-triazol-5-yl)­benzene)), is found to be highly selective in the adsorption of CO over a variety of other gas molecules, making it extremely effective, for example, in the removal of trace CO from mixtures with H<sub>2</sub>, N<sub>2</sub>, and CH<sub>4</sub>. This framework not only displays significant CO adsorption capacity at very low pressures (1.45 mmol/g at just 100 μbar), but, importantly, also exhibits readily reversible CO binding. Fe-BTTri utilizes a unique spin state change mechanism to bind CO in which the coordinatively unsaturated, high-spin Fe<sup>II</sup> centers of the framework convert to octahedral, low-spin Fe<sup>II</sup> centers upon CO coordination. Desorption of CO converts the Fe<sup>II</sup> sites back to a high-spin ground state, enabling the facile regeneration and recyclability of the material. This spin state change is supported by characterization via infrared spectroscopy, single crystal X-ray analysis, Mössbauer spectroscopy, and magnetic susceptibility measurements. Importantly, the spin state change is selective for CO and is not observed in the presence of other gases, such as H<sub>2</sub>, N<sub>2</sub>, CO<sub>2</sub>, CH<sub>4</sub>, or other hydrocarbons, resulting in unprecedentedly high selectivities for CO adsorption for use in CO/H<sub>2</sub>, CO/N<sub>2</sub>, and CO/CH<sub>4</sub> separations and in preferential CO adsorption over typical strongly adsorbing gases like CO<sub>2</sub> and ethylene. While adsorbate-induced spin state transitions are well-known in molecular chemistry, particularly for CO, to our knowledge this is the first time such behavior has been observed in a porous material suitable for use in a gas separation process. Potentially, this effect can be extended to selective separations involving other π-acids

    Structural and Electronic Effects on the Properties of Fe<sub>2</sub>(dobdc) upon Oxidation with N<sub>2</sub>O

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    We report electronic, vibrational, and magnetic properties, together with their structural dependences, for the metal–organic framework Fe<sub>2</sub>(dobdc) (dobdc<sup>4–</sup> = 2,5-dioxido-1,4-benzenedicarboxylate) and its derivatives, Fe<sub>2</sub>(O)<sub>2</sub>(dobdc) and Fe<sub>2</sub>(OH)<sub>2</sub>(dobdc)species arising in the previously proposed mechanism for the oxidation of ethane to ethanol using N<sub>2</sub>O as an oxidant. Magnetic susceptibility measurements reported for Fe<sub>2</sub>(dobdc) in an earlier study and reported in the current study for Fe<sup>II</sup><sub>0.26</sub>[Fe<sup>III</sup>(OH)]<sub>1.74</sub>(dobdc)­(DMF)<sub>0.15</sub>(THF)<sub>0.22</sub>, which is more simply referred to as Fe<sub>2</sub>(OH)<sub>2</sub>(dobdc), were used to confirm the computational results. Theory was also compared to experiment for infrared spectra and powder X-ray diffraction structures. Structural and magnetic properties were computed by using Kohn–Sham density functional theory both with periodic boundary conditions and with cluster models. In addition, we studied the effects of different treatments of the exchange interactions on the magnetic coupling parameters by comparing several approaches to the exchange-correlation functional: generalized gradient approximation (GGA), GGA with empirical Coulomb and exchange integrals for 3<i>d</i> electrons (GGA+U), nonseparable gradient approximation (NGA) with empirical Coulomb and exchange integrals for 3<i>d</i> electrons (NGA+U), hybrid GGA, meta-GGA, and hybrid meta-GGA. We found the coupling between the metal centers along a chain to be ferromagnetic in the case of Fe<sub>2</sub>(dobdc) and antiferromagnetic in the cases of Fe<sub>2</sub>(O)<sub>2</sub>(dobdc) and Fe<sub>2</sub>(OH)<sub>2</sub>(dobdc). The shift in magnetic coupling behavior correlates with the changing electronic structure of the framework, which derives from both structural and electronic changes that occur upon metal oxidation and addition of the charge-balancing oxo and hydroxo ligands
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