13 research outputs found

    Ru/O<sub>2</sub>‑Catalyzed Oxidative C–H Activation/Alkyne Annulation Using Quinoline-Functionalized NHC as a Directing and Functionalizable Group

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    The ruthenium/O2-catalyzed oxidative annulation reaction of imidazo[1,5-a]quinolin-2-ium salts with alkynes via N-heterocyclic carbene-directed C–H activation to obtain π-conjugated fused imidazo[1,5-a]quinolin-2-ium derivatives is reported. Molecular oxygen has been explored as an economic and clean oxidant and an alternative to metal oxidants. The current protocol exhibits a wide range of substrate scope including bioactive (±)-α-tocopherol derivatives. Moreover, most of the annulated products show strong fluorescence properties, indicating their potential for making new light-emitting materials

    Coordination and Ligand Substitution Chemistry of Bis(cyclooctyne)copper(I)

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    Cationic bis­(alkyne)­copper­(I) carbonyl and bis­(alkyne)­copper­(I) isocyanide complexes have been synthesized from the precursor (cyclooctyne)<sub>2</sub>CuBr. [Cu­(cyclo­octyne)<sub>2</sub>(CO)]­[SbF<sub>6</sub>] and [Cu­(cyclooctyne)<sub>2</sub>(CN<sup>t</sup>Bu)]­[SbF<sub>6</sub>] have trigonal-planar and three-coordinate copper centers. The copper carbonyl complex [Cu­(cyclooctyne)<sub>2</sub>(CO)]­[SbF<sub>6</sub>] displays its C–O stretching frequency in the “nonclassical” metal carbonyl region (2171 cm<sup>–1</sup>), and the analogous copper­(I) isocyanide complex [Cu­(cyclooctyne)<sub>2</sub>(CN<sup>t</sup>Bu)]­[SbF<sub>6</sub>] also has an unusually high CN stretching band at 2230 cm<sup>–1</sup>. The reaction of 3,5-Me<sub>2</sub>C<sub>6</sub>H<sub>3</sub>NH<sub>2</sub> and 4-<sup>t</sup>BuC<sub>6</sub>H<sub>4</sub>NH<sub>2</sub> with [Cu­(cyclooctyne)<sub>2</sub>(CO)]­[SbF<sub>6</sub>] led to CO displacement rather than addition to CO. CN<sup>t</sup>Bu reacts with [Cu­(cyclooctyne)<sub>2</sub>(CO)]­[SbF<sub>6</sub>] to afford [Cu­(cyclooctyne)<sub>2</sub>(CN<sup>t</sup>Bu)]­[SbF<sub>6</sub>]. The syntheses of [Cu­(cyclooctyne)­(CN<sup>t</sup>Bu)<sub>2</sub>]­[SbF<sub>6</sub>] and [Cu­(CN<sup>t</sup>Bu)<sub>4</sub>]­[SbF<sub>6</sub>] from the (cyclooctyne)<sub>2</sub>CuBr precursor are also reported

    Isolable, Copper(I) Dicarbonyl Complexes Supported by <i>N</i>‑Heterocyclic Carbenes

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    Cationic copper­(I) dicarbonyl complexes supported by <i>N</i>-heterocyclic carbene ligands, SIPr and IPr*, have been synthesized. [(SIPr)­Cu­(CO)<sub>2</sub>]­[SbF<sub>6</sub>] and [(IPr*)­Cu­(CO)<sub>2</sub>]­[SbF<sub>6</sub>] have a trigonal planar, three-coordinate copper atom with an average Cu–CO distance of 1.915 Å and display C–O stretching frequencies higher than that of the free CO (2143 cm<sup>–1</sup>). The high CO stretching frequencies suggest that the Cu­(I)–CO interaction in these cationic adducts is dominated by electrostatic and OC → Cu σ-donor components. [(SIPr)­Cu­(CO)<sub>2</sub>]­[SbF<sub>6</sub>] and [(IPr*)­Cu­(CO)<sub>2</sub>]­[SbF<sub>6</sub>] readily form the corresponding [(SIPr)­Cu­(CO)­(H<sub>2</sub>O)]­[SbF<sub>6</sub>] and [(IPr*)­Cu­(CO)­(H<sub>2</sub>O)]­[SbF<sub>6</sub>] with loss of a CO even with traces of water, but they can be converted back to the dicarbonyl adducts using excess CO. The synthesis and structure of [(IPr*)­Cu­(H<sub>2</sub>O)]­[SbF<sub>6</sub>] are also reported. It is a two-coordinate copper adduct with a Cu–O distance of 1.874(2) Å. It reacts with excess CO to form [(IPr*)­Cu­(CO)<sub>2</sub>]­[SbF<sub>6</sub>]

    Coordination and Ligand Substitution Chemistry of Bis(cyclooctyne)copper(I)

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    Cationic bis­(alkyne)­copper­(I) carbonyl and bis­(alkyne)­copper­(I) isocyanide complexes have been synthesized from the precursor (cyclooctyne)<sub>2</sub>CuBr. [Cu­(cyclo­octyne)<sub>2</sub>(CO)]­[SbF<sub>6</sub>] and [Cu­(cyclooctyne)<sub>2</sub>(CN<sup>t</sup>Bu)]­[SbF<sub>6</sub>] have trigonal-planar and three-coordinate copper centers. The copper carbonyl complex [Cu­(cyclooctyne)<sub>2</sub>(CO)]­[SbF<sub>6</sub>] displays its C–O stretching frequency in the “nonclassical” metal carbonyl region (2171 cm<sup>–1</sup>), and the analogous copper­(I) isocyanide complex [Cu­(cyclooctyne)<sub>2</sub>(CN<sup>t</sup>Bu)]­[SbF<sub>6</sub>] also has an unusually high CN stretching band at 2230 cm<sup>–1</sup>. The reaction of 3,5-Me<sub>2</sub>C<sub>6</sub>H<sub>3</sub>NH<sub>2</sub> and 4-<sup>t</sup>BuC<sub>6</sub>H<sub>4</sub>NH<sub>2</sub> with [Cu­(cyclooctyne)<sub>2</sub>(CO)]­[SbF<sub>6</sub>] led to CO displacement rather than addition to CO. CN<sup>t</sup>Bu reacts with [Cu­(cyclooctyne)<sub>2</sub>(CO)]­[SbF<sub>6</sub>] to afford [Cu­(cyclooctyne)<sub>2</sub>(CN<sup>t</sup>Bu)]­[SbF<sub>6</sub>]. The syntheses of [Cu­(cyclooctyne)­(CN<sup>t</sup>Bu)<sub>2</sub>]­[SbF<sub>6</sub>] and [Cu­(CN<sup>t</sup>Bu)<sub>4</sub>]­[SbF<sub>6</sub>] from the (cyclooctyne)<sub>2</sub>CuBr precursor are also reported

    Inducing Single Molecule Magnetic Behavior in a [Co<sub>4</sub>O<sub>4</sub>] Cubane via a Pronounced Solvatomagnetic Effect

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    The pyrazole-based tridentate diol ligand 2-(1-(2-hydroxyethyl)-1<i>H</i>-pyrazol-3-yl)­phenol (H<sub>2</sub>L) forms a cubane-type complex [Co<sub>4</sub>L<sub>4</sub>(MeOH)<sub>4</sub>] (<b>1</b>) that features a {Co<sub>4</sub>O<sub>4</sub>} core and four exogenous MeOH ligands. Electrospray ionization mass spectrometry suggests that the MeOH ligands are easily lost, and thermogravimetric analysis evinces a thermally induced release of those methanol molecules from solid material in the temperature range from 380 to 440 K. Desolvation was found to give rise to a pronounced solvatomagnetic effect that causes a switching of the spin ground state of the {Co<sub>4</sub>O<sub>4</sub>} core from diamagnetic to magnetic. Furthermore, the desolvated “naked” [Co<sub>4</sub>L<sub>4</sub>] cube (<b>1</b>*) shows slow relaxation of the magnetization and butterfly-like magnetic hysteresis at 2 K. A comparatively high relaxation barrier <i>U</i><sub>eff</sub>/<i>k</i><sub>B</sub> = 64.4 K and a characteristic relaxation time τ<sub>0</sub> = 3.8 × 10<sup>–9</sup> s for <b>1</b>* have been derived from an Arrhenius plot. These findings thus demonstrate that the emergence of interesting magnetic properties in molecule-based materials can be triggered via a solvatomagnetic process, even for materials that in their solvated form have a diamagnetic (<i>S</i><sub>T</sub> = 0) ground state

    Triple Role of Proton Sponge (DMAN) in the Palladium-Catalyzed Direct Stereoselective Synthesis of <i>C</i>‑Aryl Glycosides from Glycals

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    The triple role of 1,8-bis(dimethylamino)naphthalene (proton sponge) as a reductant, ligand precursor, and organic base in the palladium-catalyzed Heck-type coupling reaction of glycals with aryl iodides affords the rapid and stereoselective synthesis of 2â€Č,3â€Č-unsaturated α-C-aryl glycosides in excellent yields. The role of the proton sponge in reducing palladium(II) to (0) has been studied using cyclic voltammetry, UV–vis, HRMS, and other spectroscopic techniques. This is the first example of a palladium proton sponge complex utilized in coupling reactions. The method is observed to be tolerant of various functional groups, as demonstrated by the huge substrate scope. Moreover, the 2â€Č,3â€Č-unsaturated α-C-aryl glycosides were also converted to 3-keto-ÎČ-C-glycosides under sterically hindered pyridinium salt catalysis via a ring-opening and -closing mechanism

    Reversible Solvatomagnetic Effect in Novel Tetranuclear Cubane-Type Ni<sub>4</sub> Complexes and Magnetostructural Correlations for the [Ni<sub>4</sub>(ÎŒ<sub>3</sub>‑O)<sub>4</sub>] Core

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    A new family of tetranuclear nickel cube complexes [Ni<sub>4</sub>L<sub>4</sub>(solv)<sub>4</sub>] (<b>1</b>, solv = MeOH; <b>2</b>, solv = H<sub>2</sub>O; H<sub>2</sub>L = pyrazole-based tridentate {ONO} ligand) has been studied in detail, in particular by X-ray diffraction and superconducting quantum interference device (SQUID) magnetometry. Different solvates <b>1·H</b><sub><b>2</b></sub><b>O</b>, <b>2·4C</b><sub><b>3</b></sub><b>H</b><sub><b>6</b></sub><b>O</b>, <b>2·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>, and <b>2·H</b><sub><b>2</b></sub><b>O</b> were obtained in crystalline form. Only small structural variations were found for the Ni–O–Ni angles of the [Ni<sub>4</sub>O<sub>4</sub>] cores of those compounds, but these slight variations have dramatic consequences for the magnetic properties. [Ni<sub>4</sub>L<sub>4</sub>(MeOH)<sub>4</sub>]·H<sub>2</sub>O (<b>1·H</b><sub><b>2</b></sub><b>O</b>) and [Ni<sub>4</sub>L<sub>4</sub>(H<sub>2</sub>O)<sub>4</sub>]·H<sub>2</sub>O (<b>2·H</b><sub><b>2</b></sub><b>O</b>) can be reversibly interconverted in the solid state by exposure to the respective solvent, MeOH or H<sub>2</sub>O, and this goes along with a switching of the spin ground state from magnetic (<i>S</i><sub>T</sub> = 4) to diamagnetic (<i>S</i><sub>T</sub> = 0). Likewise the (irreversible) loss of lattice solvent in [Ni<sub>4</sub>L<sub>4</sub>(H<sub>2</sub>O)<sub>4</sub>]·4C<sub>3</sub>H<sub>6</sub>O (<b>2·4C</b><sub><b>3</b></sub><b>H</b><sub><b>6</b></sub><b>O</b>) to give <b>2·2C</b><sub><b>3</b></sub><b>H</b><sub><b>6</b></sub><b>O</b> changes the ground state from <i>S</i><sub>T</sub> = 4 to <i>S</i><sub>T</sub> = 0. In view of these dramatic solvatomagnetic effects for the present [Ni<sub>4</sub>L<sub>4</sub>(solv)<sub>4</sub>] complexes, which occur upon extrusion of lattice solvent or facile exchange of coordinated solvent molecules while keeping the robust [Ni<sub>4</sub>O<sub>4</sub>] core intact, a note of care is issued: whenever magnetic data are obtained for powdered material or for crystals that easily loose lattice solvent molecules, the magnetic properties may not necessarily reflect the situation observed in the corresponding single crystal diffraction study. Finally, a thorough analysis of the present series of complexes as well as other {Ni<sub>4</sub>(ÎŒ<sub>3</sub>-OR)<sub>4</sub>} cubes reported in the literature confirms that a correlation between the (Ni–O–Ni)<sub>av</sub> bond angle and <i>J</i> in [Ni<sub>4</sub>O<sub>4</sub>] cubane complexes does indeed exist

    Reversible Solvatomagnetic Effect in Novel Tetranuclear Cubane-Type Ni<sub>4</sub> Complexes and Magnetostructural Correlations for the [Ni<sub>4</sub>(ÎŒ<sub>3</sub>‑O)<sub>4</sub>] Core

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    A new family of tetranuclear nickel cube complexes [Ni<sub>4</sub>L<sub>4</sub>(solv)<sub>4</sub>] (<b>1</b>, solv = MeOH; <b>2</b>, solv = H<sub>2</sub>O; H<sub>2</sub>L = pyrazole-based tridentate {ONO} ligand) has been studied in detail, in particular by X-ray diffraction and superconducting quantum interference device (SQUID) magnetometry. Different solvates <b>1·H</b><sub><b>2</b></sub><b>O</b>, <b>2·4C</b><sub><b>3</b></sub><b>H</b><sub><b>6</b></sub><b>O</b>, <b>2·CH</b><sub><b>2</b></sub><b>Cl</b><sub><b>2</b></sub>, and <b>2·H</b><sub><b>2</b></sub><b>O</b> were obtained in crystalline form. Only small structural variations were found for the Ni–O–Ni angles of the [Ni<sub>4</sub>O<sub>4</sub>] cores of those compounds, but these slight variations have dramatic consequences for the magnetic properties. [Ni<sub>4</sub>L<sub>4</sub>(MeOH)<sub>4</sub>]·H<sub>2</sub>O (<b>1·H</b><sub><b>2</b></sub><b>O</b>) and [Ni<sub>4</sub>L<sub>4</sub>(H<sub>2</sub>O)<sub>4</sub>]·H<sub>2</sub>O (<b>2·H</b><sub><b>2</b></sub><b>O</b>) can be reversibly interconverted in the solid state by exposure to the respective solvent, MeOH or H<sub>2</sub>O, and this goes along with a switching of the spin ground state from magnetic (<i>S</i><sub>T</sub> = 4) to diamagnetic (<i>S</i><sub>T</sub> = 0). Likewise the (irreversible) loss of lattice solvent in [Ni<sub>4</sub>L<sub>4</sub>(H<sub>2</sub>O)<sub>4</sub>]·4C<sub>3</sub>H<sub>6</sub>O (<b>2·4C</b><sub><b>3</b></sub><b>H</b><sub><b>6</b></sub><b>O</b>) to give <b>2·2C</b><sub><b>3</b></sub><b>H</b><sub><b>6</b></sub><b>O</b> changes the ground state from <i>S</i><sub>T</sub> = 4 to <i>S</i><sub>T</sub> = 0. In view of these dramatic solvatomagnetic effects for the present [Ni<sub>4</sub>L<sub>4</sub>(solv)<sub>4</sub>] complexes, which occur upon extrusion of lattice solvent or facile exchange of coordinated solvent molecules while keeping the robust [Ni<sub>4</sub>O<sub>4</sub>] core intact, a note of care is issued: whenever magnetic data are obtained for powdered material or for crystals that easily loose lattice solvent molecules, the magnetic properties may not necessarily reflect the situation observed in the corresponding single crystal diffraction study. Finally, a thorough analysis of the present series of complexes as well as other {Ni<sub>4</sub>(ÎŒ<sub>3</sub>-OR)<sub>4</sub>} cubes reported in the literature confirms that a correlation between the (Ni–O–Ni)<sub>av</sub> bond angle and <i>J</i> in [Ni<sub>4</sub>O<sub>4</sub>] cubane complexes does indeed exist

    Zinc-Mediated Carbene Insertion to C–Cl Bonds of Chloromethanes and Isolable Zinc(II) Isocyanide Adducts

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    The zinc adduct {[HB­(3,5-(CF<sub>3</sub>)<sub>2</sub>Pz)<sub>3</sub>]­Zn}<sup>+</sup>, which was generated from [HB­(3,5-(CF<sub>3</sub>)<sub>2</sub>Pz)<sub>3</sub>]­ZnEt and [Ph<sub>3</sub>C]­{B­[3,5-(CF<sub>3</sub>)<sub>2</sub>C<sub>6</sub>H<sub>3</sub>]<sub>4</sub>}, catalyzes the activation of C–halogen bonds of chloromethanes via carbene insertion. Ethyl diazoacetate serves as the carbene precursor. The presence of {[HB­(3,5-(CF<sub>3</sub>)<sub>2</sub>Pz)<sub>3</sub>]­Zn}<sup>+</sup> in the reaction mixture was confirmed by obtaining {[HB­(3,5-(CF<sub>3</sub>)<sub>2</sub>Pz)<sub>3</sub>]­Zn­(CN<sup>t</sup>Bu)<sub>3</sub>}<sup>+</sup> using CN<sup>t</sup>Bu as a trapping agent. {[HB­(3,5-(CF<sub>3</sub>)<sub>2</sub>Pz)<sub>3</sub>]­Zn­(CN<sup>t</sup>Bu)<sub>3</sub>}<sup>+</sup> loses one zinc-bound CN<sup>t</sup>Bu easily to produce five-coordinate {[HB­(3,5-(CF<sub>3</sub>)<sub>2</sub>Pz)<sub>3</sub>]­Zn­(CN<sup>t</sup>Bu)<sub>2</sub>}<sup>+</sup>

    Tris(alkyne) and Bis(alkyne) Complexes of Coinage Metals: Synthesis and Characterization of (cyclooctyne)<sub>3</sub>M<sup>+</sup> (M = Cu, Ag) and (cyclooctyne)<sub>2</sub>Au<sup>+</sup> and Coinage Metal (M = Cu, Ag, Au) Family Group Trends

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    The tris­(alkyne) copper complex [(cyclooctyne)<sub>3</sub>Cu]­[SbF<sub>6</sub>] has been synthesized using cyclooctyne and in situ generated CuSbF<sub>6</sub>. Tris­(alkyne) silver complexes [(cyclooctyne)<sub>3</sub>Ag]<sup>+</sup> involving weakly coordinating counterions such as [SbF<sub>6</sub>]<sup>−</sup> and [PF<sub>6</sub>]<sup>−</sup> have also been isolated in good yield using cyclooctyne and commercially available AgSbF<sub>6</sub> and AgPF<sub>6</sub>. These coinage metal tris­(alkyne) adducts have trigonal-planar metal sites. The alkyne carbon atoms and the metal site form distorted spoke-wheel (rather than upright trigonal-prismatic) structures in the solid state. In [(cyclooctyne)<sub>3</sub>Cu]­[SbF<sub>6</sub>], these distortions result in a propeller-like arrangement of alkynes. A cationic gold­(I) complex having two alkynes has been prepared by a reaction of equimolar amounts of Au­(cyclooctyne)<sub>2</sub>Cl and AgSbF<sub>6</sub> in dichloromethane. The gold atom of [(cyclooctyne)<sub>2</sub>Au]<sup>+</sup> coordinates to the cyclooctynes in a linear fashion, while the carbon atoms of the alkyne groups form a tetrahedron around gold­(I). Optimized geometries of cationic [(cyclooctyne)<sub>3</sub>M]<sup>+</sup>, [(cyclooctyne)<sub>2</sub>M]<sup>+</sup>, and [(cyclooctyne)­M]<sup>+</sup> and neutral [(cyclooctyne)<sub>2</sub>MCl] and [(cyclooctyne)­MCl] adducts (M = Cu, Ag, Au) using density functional theory (DFT) at the BP86/def2-TZVPP level of theory and a detailed analysis of metal–alkyne bonding interactions are also presented
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