Optical activity and light scattering in the isotropic and smectic A* phases of a highly chiral smectic liquid crystal

The results of optical activity measurements on the smectic A* phase of 1-methylheptyl 4'-[(4-n-tetradecyloxyphenyl)proprioloyloxy]biphenyl-4-carboxylate (14P1M7) and the chiral nematic phase of a chiral-racemic mixture of S-4-(2-methylbutyl)phenyl 4-decyloxybenzoate (CE6) are shown to be extremely similar. This is in full agreement with the proposed model of the A* phase as a twistgrain-boundary (TGB) phase. In addition, new light scattering measurements using circularly polarized light in a back-scattering geometry yield information on the fluctuations in the isotropic phase. Unlike in chiral nematics where only one structural mode is affected, the data show a strong deviation from the normal temperature dependence near the isotropic-smectic A* transition for two structural modes. Possible reasons for this behaviour in highly chiral smectic liquid crystals are discussed.     

The Previously Unclassified Smectic Phases of Bis-(4′-n-Heptyloxybenzylidene)-1, 4–Phenylenediamine (HEPTOBPD)

Re-examination of the bis-(4′-n-alkoxy-benzylidene)-1,4–phenylenediamines, particularly the heptyloxy homologue, by optical microscopy and differential scanning calorimetry has confirmed the existence of two hitherto unclassified smectic phases, which are now assigned the code letters J and K (S_J andS_k     

A Natural Progression from Smectic C to Tilted Smectic B Properties in the n-Alkyl 4′-n-Alkoxybiphenyl-4-carboxylates

Recently^1,2 the n-alkyl esters of the 4′-n-heptyloxy- to 4′-n-decyloxy-biphenyl-4-carboxylic acids (inclusive) were prepared. These homologous series all showed a sudden injection of smectic C properties at the n-butyl ester. In the current work, a number of esters of the 4′-n-dodecyloxy-4′-n-tetradecyloxy-, 4′-n-hexadecyloxy-, and 4′-n-octadecyloxy-biphenyl-4-carboxylic acids have been prepared in order to establish the smectic phase sequences at longer, terminal alkoxy chain lengths. It was found that, as the terminal alkoxy chain length was increased there was a natural, smooth progression to esters which exhibit tilted smectic B phases rather than tilted smectic C phases.     

Self-organizing properties of monosubstituted sucrose fatty acid esters: the effects of chain length and unsaturation

Three families of mono-substituted sucrose fatty acid esters were prepared by enzymatic and classical synthetic procedures, and their self-assembly and self-organizational properties were investigated by thermal polarised light microscopy, differential scanning calorimetry and X-ray diffraction. The properties were evaluated as a function of the fatty acid chain length. For the lower homologues of the series columnar liquid-crystalline stacking structures were found, whereas for the higher homologues, lamellar phases predominated. A model for the columnar stacking arrangement, consisting of a unique arrangement of the molecules which could lead to the creation of multiple internal ion channels between the hydrophobic interior and the hydrophilic exterior of the columns, is suggested.     

New synthetic strategies and disconnections in the synthesis of liquid crystals enabled by photoredox cross-coupling reactions

In this letter we describe the application of metallaphotoredox cross-electrophile couplings to the synthesis of liquid crystals using dual nickel and iridium catalysis. Given the proliferation of aryl and alkyl bromides in liquid crystal research we consider that the silyl-radical mediated cross-coupling of alkyl bromide with an aryl bromide (to afford a direct alkyl–aryl bond) will become an extremely powerful tool in the synthesis of liquid crystalline materials, and we use this to synthesise several well-known materials (PCH32, 5CB, CB7CB and CB15) in a single synthetic step from inexpensive and commercially available building blocks. The metallaphotoredox decarboxylative sp³–sp² cross-coupling of an aryl bromide with an alkyl carboxylic acid provides a complimentary method to form alkyl–aryl bonds, and we use this to successfully prepare trans PCH5 in a single synthetic step from commercially available building blocks. We also prepare novel methylene-linked materials in a single synthetic step, one of which exhibit the topical TB phase.     

Dielectric studies of the hexatic B-smectic A and crystal B-smectic A transitions

Static dielectric constants, ε_∥ and ε_⊥ as well as the low frequency dielectric dispersion of ε_∥ have been studied in the vicinity of the hexatic B-smectic A transition in n-hexyl-4'-pentyloxybiphenyl-4-carboxylate (65OBC) and n-butyl-4'-hexyloxybiphenyl-4-carboxylate (46OBC) and also near the crystal B-smectic A transition in n-(4-n-butyloxybenzylidene)-4-n-octylaniline (4O. 8). While the behaviour of the dielectric anisotropy is essentially similar for both transitions, the dispersion results show significant differences.     

Conformational distribution of a ferroelectric liquid crystal revealed using fingerprint vibrational spectroscopy and the density functional theory

The authors have investigated the conformational structure of the ferroelectric liquid crystal compound 4-3-methyl-2-chloropentanoyloxy-4"-hexyloxy-biphenyl also known under the abbreviations 3M2CPHOB and C6 using vibrational (IR and Raman) spectroscopy. The measured spectra exhibit two bands corresponding to the C=O stretching vibration that are separated by 20 cm(-1). In contrast, the molecular structure comprises only one such group. They assigned the two bands to different conformers that coexist in a temperature range between 25 and 65 degrees C covering the entire mesophase of this material. This assignment is strongly confirmed by calculated vibrational spectra based on the density functional theory.     

Thermotropic liquid crystalline glycolipids

Are the liquid crystalline properties of the materials of living systems important in biological structures, functions, diseases and treatments? There is a growing consciousness that the observed lyotropic, and often thermotropic liquid crystallinity, of many biological materials that possess key biological functionality might be more than curious coincidence. Rather, as the survival of living systems depends on the flexibility and reformability of structures, it seems more likely that it is the combination of softness and structure of the liquid-crystalline state that determines the functionality of biological materials. The richest sources of liquid crystals derived from living systems are found in cell membranes, of these glycolipids are a particularly important class of components. In this critical review, we will examine the relationship between chemical structure and the self-assembling and self-organising properties of glycolipids that ultimately lead to mesophase formation.     

The Discotic Phase of Uro-Porphyrin I Octa-N-Dodecyl Estei

A number of materials which exhibit the relatively new discotic phase have recently been discovered. All of the materials known which show this type of phase have molecular structures that are flat and hexagonal in shape. In this current work, we have shown that a porphyrin compound, uro-porphyrin I octa-n-dodecyl ester, which has a flat, octagonally shaped molecular structure can also exhibit a discotic phase. This is the first report of the discotic liquid crystal phase being exhibited by porphyrin compounds.     

The magnitude and temperature dependence of the Kerr constant in liquid crystal blue phases and the dark conglomerate phase

A new method of evaluating the Kerr constant in liquid crystals (LCs) is used to determine the temperature dependence of the Kerr effect in blue phases I and II (BPI and BPII) and to investigate the Kerr constant of the isotropic dark conglomerate (DC) phase. This method employs relatively small driving voltages and a vertical field switching (VFS) device geometry. An unusually large Kerr constant, K, is determined in the BPs of a non-polymer-stabilised material, ～3×10^?9 mV^?2 (BPI). The large value of K is attributed to significant pre-transitional values of the dielectric anisotropy and birefringence. K follows an inverse dependence on temperature and we consequently suggest that BPI demonstrates properties best suited to electro-optic devices. The new methodology has the advantage of revealing the dispersion of K in a single measurement. It is also possible to deconvolute the influence of the Kerr effect from measurements of electrostriction of the BP lattice. Finally, the Kerr effect has been measured for the first time in the DC phase of an oxadiazole bent-core liquid crystalline material, and is found to take rather low values, ～1×10^?11 mV^?2, which can be understood in the context of the physical properties of the material.