15 research outputs found

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

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    CobaltĀ­(II), in the presence of acetate and nitrate, quantitatively adds to the manganeseā€“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>)Ā­(py)<sub>3</sub> (<b>2</b>). Complex <b>2</b> is structurally reminiscent of photosystem IIā€™s oxygen-evolving center, and is a rare example of a transition-metal ā€œdanglerā€ 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 danglerā€™s influence on a cubane

    Utility of Lithium in Rare-Earth Metal Reduction Reactions to Form Nontraditional Ln<sup>2+</sup> Complexes and Unusual [Li(2.2.2-cryptand)]<sup>1+</sup> Cations

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    The utility of lithium compared to other alkali metals in generating Ln<sup>2+</sup> rare-earth metal complexes via reduction of Ln<sup>3+</sup> precursors in reactions abbreviated as LnA<sub>3</sub>/M (Ln = rare-earth metal; A = anionic ligand; M = alkali metal) is described. Lithium reduction of Cpā€²<sub>3</sub>Ln (Cpā€² = C<sub>5</sub>H<sub>4</sub>SiMe<sub>3</sub>; Ln = Y, Tb, Dy, Ho) under Ar in the presence of 2.2.2-cryptand (crypt) forms new examples of crystallographically characterizable Ln<sup>2+</sup> complexes of these metals, [LiĀ­(crypt)]Ā­[Cpā€²<sub>3</sub>Ln]. In each complex, lithium is found in an N<sub>2</sub>O<sub>4</sub> donor atom coordination geometry that is unusual for the cryptand ligand. Magnetic susceptibility data on these new examples of nontraditional divalent lanthanide complexes are consistent with 4f<sup><i>n</i></sup>5d<sup>1</sup> electronic configurations. The Dy and Ho complexes have exceptionally high single-ion magnetic moments, 11.35 and 11.67 Ī¼<sub>B</sub>, respectively. Lithium reduction of Cpā€²<sub>3</sub>Y under N<sub>2</sub> at āˆ’35 Ā°C forms the Y<sup>2+</sup> complex (Cpā€²<sub>3</sub>Y)<sup>1ā€“</sup>, which reduces dinitrogen upon warming to room temperature to generate the (N<sub>2</sub>)<sup>2ā€“</sup> complex [Cpā€²<sub>2</sub>YĀ­(THF)]<sub>2</sub>(Ī¼-Ī·<sup>2</sup>:Ī·<sup>2</sup>-N<sub>2</sub>). These results provide insight on the factors that lead to reduced dinitrogen complexes and/or stable divalent lanthanide complexes as a function of the specific reducing agent and conditions

    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 [KĀ­(crypt)]Ā­[Cpā€²<sub>3</sub>Ln], <b>1-Ln</b> (Cpā€² = C<sub>5</sub>H<sub>4</sub>SiMe<sub>3</sub>; crypt = 2.2.2-cryptand; Ln = La, Ce, Pr, and Nd), and [KĀ­(crypt)]Ā­[Cpā€²ā€²<sub>3</sub>Ln], <b>2-Ln</b> [Cpā€²ā€² = 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 Cpā€²ā€²<sub>3</sub>Ln with potassium graphite in the presence of crypt and crystallographically characterized. The structures and UVā€“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 Metalā€“Organic Framework

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    A three-dimensional network solid composed of Fe<sup>III</sup> centers and paraĀ­magnetic semiĀ­quinoid linkers, (NBu<sub>4</sub>)<sub>2</sub>Ā­Fe<sup>III</sup><sub>2</sub>Ā­(dhbq)<sub>3</sub> (dhbq<sup>2ā€“/3ā€“</sup> = 2,5-dioxidoĀ­benzoĀ­quinone/ā€‹1,2-dioxido-4,5-semiĀ­quinone), is shown to exhibit a conductivity of 0.16 Ā± 0.01 S/cm at 298 K, one of the highest values yet observed for a metalā€“organic framework (MOF). The origin of this electronic conductivity is determined to be ligand mixed-valency, which is characterized using a suite of spectroĀ­scopic techniques, slow-scan cyclic voltammetry, and variable-temperature conductivity and magnetic susceptibility measurements. Importantly, UVā€“visā€“NIR diffuse reflectance measurements reveal the first observation of Robinā€“Day Class II/III mixed valency in a MOF. Pursuit of stoichioĀ­metric control over the ligand redox states resulted in synthesis of the reduced frameĀ­work material Na<sub>0.9</sub>Ā­(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 metalā€“semiĀ­quinoid system is established as a particularly promising scaffold for achieving tunable long-range electronic communication in MOFs

    Electronic Conductivity, Ferrimagnetic Ordering, and Reductive Insertion Mediated by Organic Mixed-Valence in a Ferric Semiquinoid Metalā€“Organic Framework

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    A three-dimensional network solid composed of Fe<sup>III</sup> centers and paraĀ­magnetic semiĀ­quinoid linkers, (NBu<sub>4</sub>)<sub>2</sub>Ā­Fe<sup>III</sup><sub>2</sub>Ā­(dhbq)<sub>3</sub> (dhbq<sup>2ā€“/3ā€“</sup> = 2,5-dioxidoĀ­benzoĀ­quinone/ā€‹1,2-dioxido-4,5-semiĀ­quinone), is shown to exhibit a conductivity of 0.16 Ā± 0.01 S/cm at 298 K, one of the highest values yet observed for a metalā€“organic framework (MOF). The origin of this electronic conductivity is determined to be ligand mixed-valency, which is characterized using a suite of spectroĀ­scopic techniques, slow-scan cyclic voltammetry, and variable-temperature conductivity and magnetic susceptibility measurements. Importantly, UVā€“visā€“NIR diffuse reflectance measurements reveal the first observation of Robinā€“Day Class II/III mixed valency in a MOF. Pursuit of stoichioĀ­metric control over the ligand redox states resulted in synthesis of the reduced frameĀ­work material Na<sub>0.9</sub>Ā­(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 metalā€“semiĀ­quinoid 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)ā€“Triazolate Metalā€“Organic Framework

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    A new metalā€“organic framework, Fe-BTTri (Fe<sub>3</sub>[(Fe<sub>4</sub>Cl)<sub>3</sub>(BTTri)<sub>8</sub>]<sub>2</sub>Ā·18CH<sub>3</sub>OH, H<sub>3</sub>BTTri =1,3,5-trisĀ­(1<i>H</i>-1,2,3-triazol-5-yl)Ā­benzene)), 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 Ī¼bar), 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, MoĢˆssbauer 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 Ļ€-acids

    Selective, Tunable O<sub>2</sub> Binding in Cobalt(II)ā€“Triazolate/Pyrazolate Metalā€“Organic Frameworks

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    The air-free reaction of CoCl<sub>2</sub> with 1,3,5-triĀ­(1<i>H</i>-1,2,3-triazol-5-yl)Ā­benzene (H<sub>3</sub>BTTri) in <i>N</i>,<i>N</i>-dimethylformamide (DMF) and methanol leads to the formation of Co-BTTri (Co<sub>3</sub>[(Co<sub>4</sub>Cl)<sub>3</sub>(BTTri)<sub>8</sub>]<sub>2</sub>Ā·DMF), a sodalite-type metalā€“organic framework. Desolvation of this material generates coordinatively unsaturated low-spin cobaltĀ­(II) centers that exhibit a strong preference for binding O<sub>2</sub> over N<sub>2</sub>, with isosteric heats of adsorption (<i>Q</i><sub>st</sub>) of āˆ’34(1) and āˆ’12(1) kJ/mol, respectively. The low-spin (<i>S</i> = 1/2) electronic configuration of the metal centers in the desolvated framework is supported by structural, magnetic susceptibility, and computational studies. A single-crystal X-ray structure determination reveals that O<sub>2</sub> binds end-on to each framework cobalt center in a 1:1 ratio with a Coā€“O<sub>2</sub> bond distance of 1.973(6) ƅ. Replacement of one of the triazolate linkers with a more electron-donating pyrazolate group leads to the isostructural framework Co-BDTriP (Co<sub>3</sub>[(Co<sub>4</sub>Cl)<sub>3</sub>(BDTriP)<sub>8</sub>]<sub>2</sub>Ā·DMF; H<sub>3</sub>BDTriP = 5,5ā€²-(5-(1<i>H</i>-pyrazol-4-yl)-1,3-phenylene)Ā­bisĀ­(1<i>H</i>-1,2,3-triazole)), which demonstrates markedly higher yet still fully reversible O<sub>2</sub> affinities (<i>Q</i><sub>st</sub> = āˆ’47(1) kJ/mol at low loadings). Electronic structure calculations suggest that the O<sub>2</sub> adducts in Co-BTTri are best described as cobaltĀ­(II)ā€“dioxygen species with partial electron transfer, while the stronger binding sites in Co-BDTriP form cobaltĀ­(III)ā€“superoxo moieties. The stability, selectivity, and high O<sub>2</sub> adsorption capacity of these materials render them promising new adsorbents for air separation processes

    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 metalā€“organic framework Fe<sub>2</sub>(dobdc) (dobdc<sup>4ā€“</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)ī—øspecies 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)Ā­(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 Kohnā€“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

    Charge Delocalization and Bulk Electronic Conductivity in the Mixed-Valence Metalā€“Organic Framework Fe(1,2,3-triazolate)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub>

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    Metalā€“organic frameworks are of interest for use in a variety of electrochemical and electronic applications, although a detailed understanding of their charge transport behavior, which is of critical importance for enhancing electronic conductivities, remains limited. Herein, we report isolation of the mixed-valence framework materials, FeĀ­(tri)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub> (tri<sup>ā€“</sup> = 1,2,3-triazolate; <i>x</i> = 0.09, 0.22, and 0.33), obtained from the stoichiometric chemical oxidation of the poorly conductive ironĀ­(II) framework FeĀ­(tri)<sub>2</sub>, and find that the conductivity increases dramatically with iron oxidation level. Notably, the most oxidized variant, FeĀ­(tri)<sub>2</sub>(BF<sub>4</sub>)<sub>0.33</sub>, displays a room-temperature conductivity of 0.3(1) S/cm, which represents an increase of 8 orders of magnitude from that of the parent material and is one of the highest conductivity values reported among three-dimensional metalā€“organic frameworks. Detailed characterization of FeĀ­(tri)<sub>2</sub> and the FeĀ­(tri)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub> materials via powder X-ray diffraction, MoĢˆssbauer spectroscopy, and IR and UVā€“vis-NIR diffuse reflectance spectroscopies reveals that the high conductivity arises from intervalence charge transfer between mixed-valence low-spin Fe<sup>II/III</sup> centers. Further, MoĢˆssbauer spectroscopy indicates the presence of a valence-delocalized Fe<sup>II/III</sup> species in FeĀ­(tri)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub> at 290 K, one of the first such observations for a metalā€“organic framework. The electronic structure of valence-pure FeĀ­(tri)<sub>2</sub> and the charge transport mechanism and electronic structure of mixed-valence FeĀ­(tri)<sub>2</sub>(BF<sub>4</sub>)<sub><i>x</i></sub> frameworks are discussed in detail
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