38 research outputs found

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    Solid State 13

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    Distribution of 1‑Butyl-3-methylimidazolium Bistrifluoromethylsulfonimide in Mesoporous Silica As a Function of Pore Filling

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    Rotational dynamics of the ionic liquid (IL) 1-butyl-3-methylimidazolium bistrifluoromethylsulfonimide, [C<sub>4</sub>mim]­[Tf<sub>2</sub>N], <b>1</b>, as a neat liquid, and confined in mesoporous silica were investigated by <sup>1</sup>H spin–spin (<i>T</i><sub>2</sub>) and spin–lattice (<i>T</i><sub>1</sub>) relaxation measurements and <sup>13</sup>C NMR spectroscopy. Translational dynamics (self-diffusion) were monitored via the diffusion coefficient, <i>D</i>, obtained with <sup>1</sup>H pulsed field gradient NMR measurements. These data were used to determine the distribution of <b>1</b> in the pores of KIT-6, a mesoporous silica with a bicontinuous gyroid pore structure, as a function of filling fraction. Relaxation studies performed as a function of filling factor and temperature reveal a dynamic heterogeneity in both translational and rotational motions for <b>1</b> at filling factors, <i>f</i> = 0.2–1.0 (<i>f</i> = 1 corresponds to fully filled pores). Spin–lattice and spin–spin relaxation times reveal that the motion of <b>1</b> in silica mesopores conforms to that expected for a two-dimensional relaxation model. The relaxation dynamics are interpreted using a two-state, fast exchange model for all motions; a slow rotation (and translation) of molecules in contact with the surface and a faster motion approximated by the values for bulk relaxation and diffusion. Compound <b>1</b> retains liquid-like behavior at all filling factors and temperatures that extend to ca. 50 degrees below the bulk melting point. Translational motion in these systems, interpreted with MD-simulated diffusivity limits, confirms the high propensity of <b>1</b> to form a monolayer film on the silica surface at low filling factors. The attractive interaction of <b>1</b> with the surface is greater than that for self-association of <b>1</b>. The trends in diffusion data at short and long diffusion time suggest that the population of surface-bound <b>1</b> is in intimate contact with <b>1</b> in the pores. This condition is most easily met at higher filling fractions with successive additions of <b>1</b> increasing the layer thickness built up on the surface layer
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