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Ionic liquid crystals (ILCs) combine the ion mobility of ionic liquids with the order and self-assembly of thermotropic mesophases. To understand the role of the anion in ILCs, wedge-shaped arylguanidinium salts with tetradecyloxy side chains were chosen as benchmark systems and their liquid crystalline self-assembly in the bulk phase as well as their electrochemical behavior in solution were studied depending on the anion. Differential scanning calorimetry (DSC), polarizing optical microscopy (POM) and X-ray diffraction (WAXS, SAXS) experiments revealed that for spherical anions, the phase width of the hexagonal columnar mesophase increased with the anion size, while for non-spherical anions, the trends were less clear cut. Depending on the anion, the ILCs showed different stability towards electrochemical oxidation and reduction with the most stable being the PF6 based compound. Cyclic voltammetry (CV) and density functional theory (DFT) calculations suggest a possible contribution of the guanidinium cation to the oxidation processes. [ABSTRACT FROM AUTHOR]

Ionic liquid crystals are ionic liquids that exhibit liquid crystalline mesomorphism together with ionic conductivity. As is known, confined liquid crystal mesophases can show anomalous dynamics and phase behavior. Investigations considering the factors controlling the macroscopic properties of ILCs in confinement are rare in the literature. This study reports the molecular mobility and the phase transition behavior of a guanidinium-based columnar ILC confined in the nanopores of self-ordered anodic aluminum oxide membranes of various pore diameters (25–180 nm) using broadband dielectric spectroscopy (BDS), calorimetry, and X-ray scattering. It is aimed at revealing in which way the pore size as well as the pore surface wettability (hydrophobic or hydrophilic) alter the molecular dynamics and phase transition behavior of this system. These properties are crucial for applications. The DSC investigations reveal the following: (i) the phase transition temperature for the transition from the plastic crystalline to the crystalline-liquid state has nonmonotonic dependence versus the inverse pore diameter; and (ii) the transition from the liquid crystalline to the isotropic phase is suppressed for all nanoconfined samples. This transition suppressed in the thermal signal was made evident by BDS and X-ray scattering. It is discussed as a continuous phase transition taking place in the pores instead of a discontinuous first-order transition, as observed for the bulk. BDS investigations show different relaxation processes for bulk and nanoconfined ILC. The molecular origins of various relaxation processes are discussed and suggested. It is further shown that the self-assembly of this ILC is dynamic in nature, which might apply for other ILCs too. The obtained results will have implications for nanoscale applications of ionic liquid crystals. [ABSTRACT FROM AUTHOR]

Abstract: The tilted smectic C phase is a rather uncommon phase in ionic liquid crystals (ILCs), whereas the orthogonal smectic A phase is the most common phase in ILCs. We now present 2 new groups of mesogens with an azobenzene core that exhibit smectic C as well as smectic A phases. Their phase sequences and tilt angles were studied by polarizing microscopy, and their temperature‐dependent layer spacings and orientational order parameters were investigated by X‐ray diffraction. We present 1 new amidinium azobenzene mesogen that forms enantiotropic smectic C and A phases and another amidinium as well as 2 new guanidinium azobenzene mesogens that exhibit monotropic smectic C and enantiotropic smectic A phases. With this study, we show that azobenzene is indeed an SmC‐promoting group in ILCs. Comparing these results with our earlier results on azobenzenes with an N‐methylimidazolium head group (N Kapernaum et al, ChemPhysChem 2016, 17, 4116‐4123), we show that the aromaticity of the imidazolium head group plays an important role in the formation of smectic C phases. [ABSTRACT FROM AUTHOR]