Abstract:We have measured the electric-field dependence of the reflectivity of the blue phase III (BP III) of cholesteric liquid crystals when the dielectric anisotropy e a < 0. We propose a model which assumes that the boundary aligns the sample to a depth L and in which L is increased by the applied field. The free energy is proportional to E" y where n depends on the structure of BP III. The data are fitted well by a Lorentzian line shape, and the peak intensity and linewidth agree well with the theory for n =2.1. T… Show more
“…The blue phases I and I1 show qualitatively different line shapes. This result contradicts conclusions based on measurements of the line shape-electric field dependence in the BPIII [35]. The relation of the lattice period of the blue phases to the wavelength of light is of the order of unity.…”
Spatial dispersion effects in chiral liquid crystals are reviewed. New spatial dispersion phenomena are observed in the vicinity of the Bragg reflection wavelength-an anomaly of the refractive index and an optical anisotropy of the cubic blue phases. These effects can be explained by taking into account the spatial dispersion correction of the dielectric tensor of the medium of higher orders in the ratio of the light wave vector to the structural wave vector of chiral phases.
“…The blue phases I and I1 show qualitatively different line shapes. This result contradicts conclusions based on measurements of the line shape-electric field dependence in the BPIII [35]. The relation of the lattice period of the blue phases to the wavelength of light is of the order of unity.…”
Spatial dispersion effects in chiral liquid crystals are reviewed. New spatial dispersion phenomena are observed in the vicinity of the Bragg reflection wavelength-an anomaly of the refractive index and an optical anisotropy of the cubic blue phases. These effects can be explained by taking into account the spatial dispersion correction of the dielectric tensor of the medium of higher orders in the ratio of the light wave vector to the structural wave vector of chiral phases.
“…We have observed here at least two of them. The first one corresponds to a loose random network of double twist cylinders, which is consistent with the spaghetti model of BP I11 [24,25]. This phase, that has hitherto been described as macroscopically amorphous, while locally highly ordered, still remains somewhat enigmatic.…”
Section: Long-range Ordering Of the Double Twist Cylindersmentioning
confidence: 65%
“…This phase, that has hitherto been described as macroscopically amorphous, while locally highly ordered, still remains somewhat enigmatic. Three main models have been proposed: (i) the spaghetti model as a spaghetti-like tangle of double twist cylinders [24,25], (ii) the cubic domain model in which double twist tubes form local small cubic domains that are randomly oriented relative to one another [20,26] and (iii) the quasi-crystal model that abides by an icosahedral symmetry [22, 271. DNA solution could provide an accurate tool to further investigations of this enigmatic BP I11 structure. Indeed, our observations not only support the spaghetti model, but also allow one to specify it.…”
Section: Long-range Ordering Of the Double Twist Cylindersmentioning
The isotropic-liquid crystalline transition of concentrated DNA solutions is investigated using freeze-fracture electron microscopy in order to understand the first steps of the DNA condensation process. Between the isotropic liquid and the cholesteric mesophase, we report the existence of double twist DNA bundles and describe their long range ordering into 3D networks. This organization corresponds to the formation of 'blue phases' already observed in thermotropic liquid crystals, but never reported in lyotropic systems. In addition, the size of the DNA molecule, about ten times that of most thermotropic materials, allows here the molecular resolution imaging of blue phase structures. Since such structures recall chromatin organization of some Procaryotes and lower Eucaryotes, we suspect that they may be widespread and of potential interest in the regulation of chromatin functions.
“…[6] It can be expected that BPIII consists of double twist cylinders with arbitrary orientation. [2,7,8] Usually, blue phases are found in a very narrow temperature range (ca. 1 K) between the isotropic liquid and the chiral nematic (N*) phase of sufficiently short pitch, except in a few cases where a SmA to BP transition has been observed.…”
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