4 research outputs found
Carr–Purcell Pulsed Electron Double Resonance with Shaped Inversion Pulses
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
Reduction of the bisÂ(9-borafluorenyl)Âmethane <b>1</b> with
excess lithium furnishes the red dianion salt Li<sub>2</sub>[<b>1</b>]. The corresponding dark green monoanion radical LiÂ[<b>1</b>] is accessible through the comproportionation reaction between <b>1</b> and Li<sub>2</sub>[<b>1</b>]. EPR spectroscopy on
LiÂ[<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) Ã…, respectively. Protonation of Li<sub>2</sub>[<b>1</b>] leads to the cyclic borohydride species LiÂ[<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
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>Cî—»CCl<sub>2</sub> (CH<sub>2</sub>Cl<sub>2</sub> solutions, room temperature
or below), the reaction furnishes the monocarbanion [CÂ(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–CÂ(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)ÂC–CÂ(H)Â(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>Cî—»CÂ(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>SiCî—¼CSiCl<sub>3</sub> (<b>C</b>; 80%); in the presence of [HMe<sub>3</sub>N]ÂCl, the trisilylethene (Cl<sub>3</sub>Si)<sub>2</sub>Cî—»CÂ(H)ÂSiCl<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-bisÂ(trichlorosilyl)-4,5-dimethylbenzene (<b>E1</b>; 80%)
after oxidation with DDQ. The corresponding 1,2-bisÂ(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>CÂ{<sup>1</sup>H}, and <sup>29</sup>Si NMR spectroscopy; an EPR spectrum of [<i>n</i>Bu<sub>4</sub>N]Â[<b>B</b><sup><b>•</b></sup>] was recorded.
The molecular structures of [<i>n</i>Bu<sub>4</sub>N]Â[<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
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>Cî—»CCl<sub>2</sub> (CH<sub>2</sub>Cl<sub>2</sub> solutions, room temperature
or below), the reaction furnishes the monocarbanion [CÂ(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–CÂ(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)ÂC–CÂ(H)Â(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>Cî—»CÂ(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>SiCî—¼CSiCl<sub>3</sub> (<b>C</b>; 80%); in the presence of [HMe<sub>3</sub>N]ÂCl, the trisilylethene (Cl<sub>3</sub>Si)<sub>2</sub>Cî—»CÂ(H)ÂSiCl<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-bisÂ(trichlorosilyl)-4,5-dimethylbenzene (<b>E1</b>; 80%)
after oxidation with DDQ. The corresponding 1,2-bisÂ(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>CÂ{<sup>1</sup>H}, and <sup>29</sup>Si NMR spectroscopy; an EPR spectrum of [<i>n</i>Bu<sub>4</sub>N]Â[<b>B</b><sup><b>•</b></sup>] was recorded.
The molecular structures of [<i>n</i>Bu<sub>4</sub>N]Â[<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