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
The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>2</sub>DABCO]Â[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]Â[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]Â[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]Â[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bromide ([C<sub>2</sub>DABCO]Â[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
The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>2</sub>DABCO]Â[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]Â[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]Â[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]Â[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bromide ([C<sub>2</sub>DABCO]Â[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
The structure of 1-butyl-1-methylpyrrolidinium bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>4</sub>mpyr]Â[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
The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>2</sub>DABCO]Â[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]Â[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]Â[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]Â[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bromide ([C<sub>2</sub>DABCO]Â[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
The structure of 1-butyl-1-methylpyrrolidinium bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>4</sub>mpyr]Â[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
The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>2</sub>DABCO]Â[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]Â[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]Â[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]Â[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bromide ([C<sub>2</sub>DABCO]Â[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
The structure of 1-butyl-1-methylpyrrolidinium bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>4</sub>mpyr]Â[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
The structure of 1-butyl-1-methylpyrrolidinium bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>4</sub>mpyr]Â[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
The structure of 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bisÂ(trifluoromethylsulfonyl)Âimide
([C<sub>2</sub>DABCO]Â[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]Â[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]Â[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]Â[NTf<sub>2</sub>] precursor 1-ethyl-1,4-diazabicyclo[2.2.2]Âoctanium
bromide ([C<sub>2</sub>DABCO]Â[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