9 research outputs found

    Structural Studies on the Basic Ionic Liquid 1-Ethyl-1,4-diazabicyclo[2.2.2]octanium Bis(trifluoromethylsulfonyl)imide and Its Bromide Precursor

    No full text
    The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bis­(trifluoromethylsulfonyl)­imide ([C<sub>2</sub>DABCO]­[NTf<sub>2</sub>]) was determined by single crystal X-ray diffraction, and its behavior with temperature was examined by synchrotron powder diffraction, differential scanning calorimetry (DSC), and Raman spectroscopy. [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] undergoes a solid–solid phase transition at 309 K and a solid–liquid (melting) transition at 350 K, as reported previously in the literature. The crystal structure of [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] was determined at temperatures below the solid–solid transition (solid-I phase), whereas in situ synchrotron powder diffraction enabled the unit cell of the solid phase observed above the solid–solid transition temperature (solid-II phase) to be indexed. High-resolution synchrotron powder diffraction data indicated the coexistence of a metastable phase with the solid-I and solid-II phases around the temperature of the solid–solid phase transition. A variable temperature Raman study suggested rotational movement of both [C<sub>2</sub>DABCO]<sup>+</sup> and [NTf<sub>2</sub>]<sup>−</sup> in the solid-II phase indicating the formation of a rotator phase. The structure of the [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bromide ([C<sub>2</sub>DABCO]­[Br]) was also determined by single crystal X-ray diffraction and its phase transitions were examined by differential scanning calorimetry. A comparison of the structures and phase transitions of the two analogous salts provides insights into the relative electrostatic attraction between the ions and the relative packing density and efficiency in the crystal lattices

    Structural Studies on the Basic Ionic Liquid 1-Ethyl-1,4-diazabicyclo[2.2.2]octanium Bis(trifluoromethylsulfonyl)imide and Its Bromide Precursor

    No full text
    The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bis­(trifluoromethylsulfonyl)­imide ([C<sub>2</sub>DABCO]­[NTf<sub>2</sub>]) was determined by single crystal X-ray diffraction, and its behavior with temperature was examined by synchrotron powder diffraction, differential scanning calorimetry (DSC), and Raman spectroscopy. [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] undergoes a solid–solid phase transition at 309 K and a solid–liquid (melting) transition at 350 K, as reported previously in the literature. The crystal structure of [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] was determined at temperatures below the solid–solid transition (solid-I phase), whereas in situ synchrotron powder diffraction enabled the unit cell of the solid phase observed above the solid–solid transition temperature (solid-II phase) to be indexed. High-resolution synchrotron powder diffraction data indicated the coexistence of a metastable phase with the solid-I and solid-II phases around the temperature of the solid–solid phase transition. A variable temperature Raman study suggested rotational movement of both [C<sub>2</sub>DABCO]<sup>+</sup> and [NTf<sub>2</sub>]<sup>−</sup> in the solid-II phase indicating the formation of a rotator phase. The structure of the [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bromide ([C<sub>2</sub>DABCO]­[Br]) was also determined by single crystal X-ray diffraction and its phase transitions were examined by differential scanning calorimetry. A comparison of the structures and phase transitions of the two analogous salts provides insights into the relative electrostatic attraction between the ions and the relative packing density and efficiency in the crystal lattices

    Structure of [C<sub>4</sub>mpyr][NTf<sub>2</sub>] Room-Temperature Ionic Liquid at Charged Gold Interfaces

    No full text
    The structure of 1-butyl-1-methylpyrrolidinium bis­(trifluoromethylsulfonyl)­imide ([C<sub>4</sub>mpyr]­[NTf<sub>2</sub>]) room-temperature ionic liquid at an electrified gold interface was studied using neutron reflectometry, cyclic voltammetry, and differential capacitance measurements. Subtle differences were observed between the reflectivity data collected on a gold electrode at three different applied potentials. Detailed analysis of the fitted reflectivity data reveals an excess of [C<sub>4</sub>mpyr]<sup>+</sup> at the interface, with the amount decreasing at increasingly positive potentials. A cation rich interface was found even at a positively charged electrode, which indicates a nonelectrostatic (specific) adsorption of [C<sub>4</sub>mpyr]<sup>+</sup> onto the gold electrode

    Structural Studies on the Basic Ionic Liquid 1-Ethyl-1,4-diazabicyclo[2.2.2]octanium Bis(trifluoromethylsulfonyl)imide and Its Bromide Precursor

    No full text
    The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bis­(trifluoromethylsulfonyl)­imide ([C<sub>2</sub>DABCO]­[NTf<sub>2</sub>]) was determined by single crystal X-ray diffraction, and its behavior with temperature was examined by synchrotron powder diffraction, differential scanning calorimetry (DSC), and Raman spectroscopy. [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] undergoes a solid–solid phase transition at 309 K and a solid–liquid (melting) transition at 350 K, as reported previously in the literature. The crystal structure of [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] was determined at temperatures below the solid–solid transition (solid-I phase), whereas in situ synchrotron powder diffraction enabled the unit cell of the solid phase observed above the solid–solid transition temperature (solid-II phase) to be indexed. High-resolution synchrotron powder diffraction data indicated the coexistence of a metastable phase with the solid-I and solid-II phases around the temperature of the solid–solid phase transition. A variable temperature Raman study suggested rotational movement of both [C<sub>2</sub>DABCO]<sup>+</sup> and [NTf<sub>2</sub>]<sup>−</sup> in the solid-II phase indicating the formation of a rotator phase. The structure of the [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bromide ([C<sub>2</sub>DABCO]­[Br]) was also determined by single crystal X-ray diffraction and its phase transitions were examined by differential scanning calorimetry. A comparison of the structures and phase transitions of the two analogous salts provides insights into the relative electrostatic attraction between the ions and the relative packing density and efficiency in the crystal lattices

    Structure of [C<sub>4</sub>mpyr][NTf<sub>2</sub>] Room-Temperature Ionic Liquid at Charged Gold Interfaces

    No full text
    The structure of 1-butyl-1-methylpyrrolidinium bis­(trifluoromethylsulfonyl)­imide ([C<sub>4</sub>mpyr]­[NTf<sub>2</sub>]) room-temperature ionic liquid at an electrified gold interface was studied using neutron reflectometry, cyclic voltammetry, and differential capacitance measurements. Subtle differences were observed between the reflectivity data collected on a gold electrode at three different applied potentials. Detailed analysis of the fitted reflectivity data reveals an excess of [C<sub>4</sub>mpyr]<sup>+</sup> at the interface, with the amount decreasing at increasingly positive potentials. A cation rich interface was found even at a positively charged electrode, which indicates a nonelectrostatic (specific) adsorption of [C<sub>4</sub>mpyr]<sup>+</sup> onto the gold electrode

    Structural Studies on the Basic Ionic Liquid 1-Ethyl-1,4-diazabicyclo[2.2.2]octanium Bis(trifluoromethylsulfonyl)imide and Its Bromide Precursor

    No full text
    The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bis­(trifluoromethylsulfonyl)­imide ([C<sub>2</sub>DABCO]­[NTf<sub>2</sub>]) was determined by single crystal X-ray diffraction, and its behavior with temperature was examined by synchrotron powder diffraction, differential scanning calorimetry (DSC), and Raman spectroscopy. [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] undergoes a solid–solid phase transition at 309 K and a solid–liquid (melting) transition at 350 K, as reported previously in the literature. The crystal structure of [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] was determined at temperatures below the solid–solid transition (solid-I phase), whereas in situ synchrotron powder diffraction enabled the unit cell of the solid phase observed above the solid–solid transition temperature (solid-II phase) to be indexed. High-resolution synchrotron powder diffraction data indicated the coexistence of a metastable phase with the solid-I and solid-II phases around the temperature of the solid–solid phase transition. A variable temperature Raman study suggested rotational movement of both [C<sub>2</sub>DABCO]<sup>+</sup> and [NTf<sub>2</sub>]<sup>−</sup> in the solid-II phase indicating the formation of a rotator phase. The structure of the [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bromide ([C<sub>2</sub>DABCO]­[Br]) was also determined by single crystal X-ray diffraction and its phase transitions were examined by differential scanning calorimetry. A comparison of the structures and phase transitions of the two analogous salts provides insights into the relative electrostatic attraction between the ions and the relative packing density and efficiency in the crystal lattices

    Structure of [C<sub>4</sub>mpyr][NTf<sub>2</sub>] Room-Temperature Ionic Liquid at Charged Gold Interfaces

    No full text
    The structure of 1-butyl-1-methylpyrrolidinium bis­(trifluoromethylsulfonyl)­imide ([C<sub>4</sub>mpyr]­[NTf<sub>2</sub>]) room-temperature ionic liquid at an electrified gold interface was studied using neutron reflectometry, cyclic voltammetry, and differential capacitance measurements. Subtle differences were observed between the reflectivity data collected on a gold electrode at three different applied potentials. Detailed analysis of the fitted reflectivity data reveals an excess of [C<sub>4</sub>mpyr]<sup>+</sup> at the interface, with the amount decreasing at increasingly positive potentials. A cation rich interface was found even at a positively charged electrode, which indicates a nonelectrostatic (specific) adsorption of [C<sub>4</sub>mpyr]<sup>+</sup> onto the gold electrode

    Structure of [C<sub>4</sub>mpyr][NTf<sub>2</sub>] Room-Temperature Ionic Liquid at Charged Gold Interfaces

    No full text
    The structure of 1-butyl-1-methylpyrrolidinium bis­(trifluoromethylsulfonyl)­imide ([C<sub>4</sub>mpyr]­[NTf<sub>2</sub>]) room-temperature ionic liquid at an electrified gold interface was studied using neutron reflectometry, cyclic voltammetry, and differential capacitance measurements. Subtle differences were observed between the reflectivity data collected on a gold electrode at three different applied potentials. Detailed analysis of the fitted reflectivity data reveals an excess of [C<sub>4</sub>mpyr]<sup>+</sup> at the interface, with the amount decreasing at increasingly positive potentials. A cation rich interface was found even at a positively charged electrode, which indicates a nonelectrostatic (specific) adsorption of [C<sub>4</sub>mpyr]<sup>+</sup> onto the gold electrode

    Structural Studies on the Basic Ionic Liquid 1-Ethyl-1,4-diazabicyclo[2.2.2]octanium Bis(trifluoromethylsulfonyl)imide and Its Bromide Precursor

    No full text
    The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bis­(trifluoromethylsulfonyl)­imide ([C<sub>2</sub>DABCO]­[NTf<sub>2</sub>]) was determined by single crystal X-ray diffraction, and its behavior with temperature was examined by synchrotron powder diffraction, differential scanning calorimetry (DSC), and Raman spectroscopy. [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] undergoes a solid–solid phase transition at 309 K and a solid–liquid (melting) transition at 350 K, as reported previously in the literature. The crystal structure of [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] was determined at temperatures below the solid–solid transition (solid-I phase), whereas in situ synchrotron powder diffraction enabled the unit cell of the solid phase observed above the solid–solid transition temperature (solid-II phase) to be indexed. High-resolution synchrotron powder diffraction data indicated the coexistence of a metastable phase with the solid-I and solid-II phases around the temperature of the solid–solid phase transition. A variable temperature Raman study suggested rotational movement of both [C<sub>2</sub>DABCO]<sup>+</sup> and [NTf<sub>2</sub>]<sup>−</sup> in the solid-II phase indicating the formation of a rotator phase. The structure of the [C<sub>2</sub>DABCO]­[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]­octanium bromide ([C<sub>2</sub>DABCO]­[Br]) was also determined by single crystal X-ray diffraction and its phase transitions were examined by differential scanning calorimetry. A comparison of the structures and phase transitions of the two analogous salts provides insights into the relative electrostatic attraction between the ions and the relative packing density and efficiency in the crystal lattices
    corecore