To cite this article: Igor Gvozdovskyy (2015): 'Blue phases' of highly chiral thermotropic liquid crystals with a wide range of near-room temperature, Liquid Crystals,The phase transitions of pure cholesteric liquid crystals, based on right-or left-handed chiral dopants (ChDs) (enantiomers R-811 and S-811, Merck, Darmstadt, Germany) with various concentrations dissolving in the nematic liquid crystal mixture CHCA (ZhK-805, Russia, NIOPIK) were experimentally studied. For the first time, blue phases of cholesterics were found at the concentration range of ChDs 32-36 wt.%. Experimentally it was observed that during the cooling process the blue phase of cholesterics is stable over a wide temperature range about~15°C including human body and near-room temperatures. Thermal phase transitions, spectral characteristics and electro-optical features of blue phases were examined. Planar and homeotropic alignment layers were used to study the influence of various boundary conditions on platelet textures of blue phases.
IntroductionIt is known that for certain chiral liquid crystals (CLCs) and their mixtures the transition between the regular (helical) cholesteric phase (Ch) and the isotropic phase (Iso) occurs through a series of additional transitions well known as 'blue' phases (BPs), [1-9] which in most cases can exist only for cholesterics with pitch P < 5000 Å.[5,10] Within a narrow temperature range three thermodynamically stable blue phases (BP-III, BP-II and BP-I) exist, which can be usually observed on cooling from Iso to Ch, but sometimes on heating from Ch to Iso [3,9,11] and vice versa with thermal hysteresis. [11][12][13] The so-called 'fog' blue phase (BP-III) is amorphous with a local cubic lattice structure in the director field, which appears over a very narrow temperature range between BP-II and the Iso,[3,14-17] while BP-II and BP-I have a fluid three-dimensional periodic structure in the director field with simple cubic and body-centred cubic symmetry, respectively. [6][7][8]15,16,18] For BP-I the elementary cell (lattice) size changes with temperature; while for BP-II there is not temperature change in the lattice size. [19] According to the theory,[19] structures of BPs can be described as 'double twist' cylinders (in which the director twists simultaneously in two independent directions), filling up large volumes and disclinations. The fact that the periods of lattices of BP-II and BP-I are of the order of the visible wavelength region, leads to the observation of the selective Bragg diffraction. In addition, BPs are optically active but, unlike Ch,