4 research outputs found

    Carr–Purcell Pulsed Electron Double Resonance with Shaped Inversion Pulses

    No full text
    Pulsed electron paramagnetic resonance (EPR) spectroscopy allows the determination of distances, in the range of 1.5–8 nm, between two spin-labels attached to macromolecules containing protons. Unfortunately, for hydrophobic lipid-bound or detergent-solubilized membrane proteins, the maximum distance accessible is much lower, because of a strongly reduced coherence time of the electron spins. Here we introduce a pulse sequence, based on a Carr–Purcell decoupling scheme on the observer spin, where each π-pulse is accompanied by a shaped sech/tanh inversion pulse applied to the second spin, to overcome this limitation. This pump/probe excitation scheme efficiently recouples the dipolar interaction, allowing a substantially longer observation time window to be achieved. This increases the upper limit and accuracy of distances that can be determined in membrane protein complexes. We validated the method on a bis-nitroxide model compound and applied this technique to the trimeric betaine transporter <i>BetP</i>. Interprotomer distances as long as 6 nm could be reliably determined, which is impossible with the existing methods

    A Preorganized Ditopic Borane as Highly Efficient One- or Two-Electron Trap

    No full text
    Reduction of the bis­(9-borafluorenyl)­methane <b>1</b> with excess lithium furnishes the red dianion salt Li<sub>2</sub>[<b>1</b>]. The corresponding dark green monoanion radical Li­[<b>1</b>] is accessible through the comproportionation reaction between <b>1</b> and Li<sub>2</sub>[<b>1</b>]. EPR spectroscopy on Li­[<b>1</b>] reveals hyperfine coupling of the unpaired electron to two magnetically equivalent boron nuclei (<i>a</i>(<sup>11</sup>B) = 5.1 ± 0.1 G, <i>a</i>(<sup>10</sup>B) = 1.7 ± 0.2 G). Further coupling is observed to the unique B–C<i>H</i>–B bridgehead proton (<i>a</i>(<sup>1</sup>H) = 7.2 ± 0.2 G) and to eight aromatic protons (<i>a</i>(<sup>1</sup>H) = 1.4 ± 0.1 G). According to X-ray crystallography, the B···B distances continuously decrease along the sequence <b>1</b> → [<b>1</b>]<sup>•–</sup> → [<b>1</b>]<sup>2–</sup> with values of 2.534(2), 2.166(4), and 1.906(3) Å, respectively. Protonation of Li<sub>2</sub>[<b>1</b>] leads to the cyclic borohydride species Li­[<b>1H</b>] featuring a B–H–B two-electron-three-center bond. This result strongly indicates a nucleophilic character of the boron atoms; the reaction can also be viewed as rare example of the protonation of an element–element σ bond. According to NMR spectroscopy, EPR spectroscopy, and quantum-chemical calculations, [<b>1</b>]<sup>2–</sup> represents a closed-shell singlet without any spin contamination. Detailed wave function analyses of [<b>1</b>]<sup>•–</sup> and [<b>1</b>]<sup>2–</sup> reveal strongly localized interactions of the two boron p<sub><i>z</i></sub>-type orbitals, with small delocalized contributions of the 9-borafluorenyl π systems. Overall, our results provide evidence for a direct B–B one-electron and two-electron bonding interaction in [<b>1</b>]<sup>•–</sup> and [<b>1</b>]<sup>2–</sup>, respectively

    Exhaustively Trichlorosilylated C<sub>1</sub> and C<sub>2</sub> Building Blocks: Beyond the Müller–Rochow Direct Process

    No full text
    The Cl<sup>–</sup>-induced heterolysis of the Si–Si bond in Si<sub>2</sub>Cl<sub>6</sub> generates an [SiCl<sub>3</sub>]<sup>−</sup> ion as reactive intermediate. When carried out in the presence of CCl<sub>4</sub> or Cl<sub>2</sub>CCCl<sub>2</sub> (CH<sub>2</sub>Cl<sub>2</sub> solutions, room temperature or below), the reaction furnishes the monocarbanion [C­(SiCl<sub>3</sub>)<sub>3</sub>]<sup>−</sup> ([<b>A</b>]<sup>−</sup>; 92%) or the vicinal dianion [(Cl<sub>3</sub>Si)<sub>2</sub>C–C­(SiCl<sub>3</sub>)<sub>2</sub>]<sup>2–</sup> ([<b>B</b>]<sup>2–</sup>; 85%) in excellent yields. Starting from [<b>B</b>]<sup>2–</sup>, the tetrasilylethane (Cl<sub>3</sub>Si)<sub>2</sub>(H)­C–C­(H)­(SiCl<sub>3</sub>)<sub>2</sub> (H<sub>2</sub><b>B</b>) and the tetrasilylethene (Cl<sub>3</sub>Si)<sub>2</sub>CC­(SiCl<sub>3</sub>)<sub>2</sub> (<b>B</b>; 96%) are readily available through protonation (CF<sub>3</sub>SO<sub>3</sub>H) or oxidation (CuCl<sub>2</sub>), respectively. Equimolar mixtures of H<sub>2</sub><b>B</b>/[<b>B</b>]<sup>2–</sup> or <b>B</b>/[<b>B</b>]<sup>2–</sup> quantitatively produce 2 equiv of the monoanion [H<b>B</b>]<sup>−</sup> or the blue radical anion [<b>B</b><sup><b>•</b></sup>]<sup>−</sup>, respectively. Treatment of <b>B</b> with Cl<sup>–</sup> ions in the presence of CuCl<sub>2</sub> furnishes the disilylethyne Cl<sub>3</sub>SiCCSiCl<sub>3</sub> (<b>C</b>; 80%); in the presence of [HMe<sub>3</sub>N]­Cl, the trisilylethene (Cl<sub>3</sub>Si)<sub>2</sub>CC­(H)­SiCl<sub>3</sub> (<b>D</b>; 72%) is obtained. Alkyne <b>C</b> undergoes a [4+2]-cycloaddition reaction with 2,3-dimethyl-1,3-butadiene (CH<sub>2</sub>Cl<sub>2</sub>, 50 °C, 3d) and thus provides access to 1,2-bis­(trichlorosilyl)-4,5-dimethylbenzene (<b>E1</b>; 80%) after oxidation with DDQ. The corresponding 1,2-bis­(trichlorosilyl)-3,4,5,6-tetraphenylbenzene (<b>E2</b>; 83%) was prepared from <b>C</b> and 2,3,4,5-tetraphenyl-2,4-cyclopentadien-1-one under CO extrusion at elevated temperatures (CH<sub>2</sub>Cl<sub>2</sub>, 180 °C, 4 d). All closed-shell products were characterized by <sup>1</sup>H, <sup>13</sup>C­{<sup>1</sup>H}, and <sup>29</sup>Si NMR spectroscopy; an EPR spectrum of [<i>n</i>Bu<sub>4</sub>N]­[<b>B</b><sup><b>•</b></sup>] was recorded. The molecular structures of [<i>n</i>Bu<sub>4</sub>N]­[<b>A</b>], [<i>n</i>Bu<sub>4</sub>N]<sub>2</sub>[<b>B</b>], <b>B</b>, <b>E1</b>, and <b>E2</b> were further confirmed by single-crystal X-ray diffraction. On the basis of detailed experimental investigations, augmented by quantum-chemical calculations, plausible reaction mechanisms for the formation of [<b>A</b>]<sup>−</sup>, [<b>B</b>]<sup>2–</sup>, <b>C</b>, and <b>D</b> are postulated

    Exhaustively Trichlorosilylated C<sub>1</sub> and C<sub>2</sub> Building Blocks: Beyond the Müller–Rochow Direct Process

    No full text
    The Cl<sup>–</sup>-induced heterolysis of the Si–Si bond in Si<sub>2</sub>Cl<sub>6</sub> generates an [SiCl<sub>3</sub>]<sup>−</sup> ion as reactive intermediate. When carried out in the presence of CCl<sub>4</sub> or Cl<sub>2</sub>CCCl<sub>2</sub> (CH<sub>2</sub>Cl<sub>2</sub> solutions, room temperature or below), the reaction furnishes the monocarbanion [C­(SiCl<sub>3</sub>)<sub>3</sub>]<sup>−</sup> ([<b>A</b>]<sup>−</sup>; 92%) or the vicinal dianion [(Cl<sub>3</sub>Si)<sub>2</sub>C–C­(SiCl<sub>3</sub>)<sub>2</sub>]<sup>2–</sup> ([<b>B</b>]<sup>2–</sup>; 85%) in excellent yields. Starting from [<b>B</b>]<sup>2–</sup>, the tetrasilylethane (Cl<sub>3</sub>Si)<sub>2</sub>(H)­C–C­(H)­(SiCl<sub>3</sub>)<sub>2</sub> (H<sub>2</sub><b>B</b>) and the tetrasilylethene (Cl<sub>3</sub>Si)<sub>2</sub>CC­(SiCl<sub>3</sub>)<sub>2</sub> (<b>B</b>; 96%) are readily available through protonation (CF<sub>3</sub>SO<sub>3</sub>H) or oxidation (CuCl<sub>2</sub>), respectively. Equimolar mixtures of H<sub>2</sub><b>B</b>/[<b>B</b>]<sup>2–</sup> or <b>B</b>/[<b>B</b>]<sup>2–</sup> quantitatively produce 2 equiv of the monoanion [H<b>B</b>]<sup>−</sup> or the blue radical anion [<b>B</b><sup><b>•</b></sup>]<sup>−</sup>, respectively. Treatment of <b>B</b> with Cl<sup>–</sup> ions in the presence of CuCl<sub>2</sub> furnishes the disilylethyne Cl<sub>3</sub>SiCCSiCl<sub>3</sub> (<b>C</b>; 80%); in the presence of [HMe<sub>3</sub>N]­Cl, the trisilylethene (Cl<sub>3</sub>Si)<sub>2</sub>CC­(H)­SiCl<sub>3</sub> (<b>D</b>; 72%) is obtained. Alkyne <b>C</b> undergoes a [4+2]-cycloaddition reaction with 2,3-dimethyl-1,3-butadiene (CH<sub>2</sub>Cl<sub>2</sub>, 50 °C, 3d) and thus provides access to 1,2-bis­(trichlorosilyl)-4,5-dimethylbenzene (<b>E1</b>; 80%) after oxidation with DDQ. The corresponding 1,2-bis­(trichlorosilyl)-3,4,5,6-tetraphenylbenzene (<b>E2</b>; 83%) was prepared from <b>C</b> and 2,3,4,5-tetraphenyl-2,4-cyclopentadien-1-one under CO extrusion at elevated temperatures (CH<sub>2</sub>Cl<sub>2</sub>, 180 °C, 4 d). All closed-shell products were characterized by <sup>1</sup>H, <sup>13</sup>C­{<sup>1</sup>H}, and <sup>29</sup>Si NMR spectroscopy; an EPR spectrum of [<i>n</i>Bu<sub>4</sub>N]­[<b>B</b><sup><b>•</b></sup>] was recorded. The molecular structures of [<i>n</i>Bu<sub>4</sub>N]­[<b>A</b>], [<i>n</i>Bu<sub>4</sub>N]<sub>2</sub>[<b>B</b>], <b>B</b>, <b>E1</b>, and <b>E2</b> were further confirmed by single-crystal X-ray diffraction. On the basis of detailed experimental investigations, augmented by quantum-chemical calculations, plausible reaction mechanisms for the formation of [<b>A</b>]<sup>−</sup>, [<b>B</b>]<sup>2–</sup>, <b>C</b>, and <b>D</b> are postulated
    corecore