Publications by authors named "Vitaly P Panov"

The self-assembly of nematic molecules in microcompartments with unambiguously defined surface anchoring is well predictable and is likely to have a single stable topological structure. Here, in contrast, a confined nematic system comprising an array of microcompartments interconnected by channels is demonstrated, exhibiting diverse molecular assembly pathways leading to the formation of four types of topological structures and twelve different patterns randomly distributed. Intercompartment communication via channels plays a crucial role in the diversity of patterns and distributions.

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Article Synopsis
  • The study examines the response of a specific subphase in a binary liquid crystal mixture when subjected to an electric field, utilizing specially aligned cells.
  • In the antiferroelectric phases, distortions in the structure induce polarization that aligns with the electric field, but in the 1/2 subphase, the structure initially resists deformation, leading to a significant change in optical properties at low electric field strengths.
  • The findings suggest that thermal fluctuations are crucial in facilitating a reorientation of the liquid crystal structure, contributing to a unique switching behavior seen in certain liquid crystal displays.
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We report waveform-induced rotation-time symmetry breaking in liquid crystal director motion. Homeotropic cells filled with a negative dielectric anisotropy chiral nematic exhibit persistent and visually observable waves of director orientation with a time period of at least 30 driving field cycles. Their existence in the space of driving waveform parameters is explored.

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Article Synopsis
  • The chiral smectic phases SmC^{*} and SmC_{A}^{*} exhibit unique ordering types, with synclinic ferroelectric F and anticlinic antiferroelectric A configurations in different layers, and show mixed states at a phase-transition point.
  • Sandhya et al. highlighted the crucial role of thermal fluctuations alongside long-range interlayer interactions in stabilizing these mixed states in certain liquid crystal mixtures.
  • This study investigates the dielectric properties of a specific subphase, revealing its stability at high temperatures, antiferroelectric characteristics, increasing dielectric amplitude related to phase changes, and notable irregularities in relaxation modes at lower temperatures due to layer dynamics.
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Photopolymerization of a reactive mesogen mixed with a mesogenic dimer, shown to exhibit the twist-bend nematic phase (N), reveals the complex structure of the self-deformation patterns observed in planar cells. The polymerized reactive mesogen retains the structure formed by liquid crystalline molecules in the twist bend phase, thus enabling its observation by scanning electron microscopy (SEM). Hierarchical ordering scales ranging from tens of nanometers to micrometers are imaged in detail.

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Liquid crystals (LCs) represent one of the foundations of modern communication and photonic technologies. Present display technologies are based mainly on nematic LCs, which suffer from limited response time for use in active colour sequential displays and limited image grey scale. Herein we report the first observation of a spontaneously formed helix in a polar tilted smectic LC phase (SmC phase) of achiral bent-core (BC) molecules with the axis of helix lying parallel to the layer normal and a pitch much shorter than the optical wavelength.

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Three bent-core nematic liquid crystals having the same core but with different terminal groups, short (C4) and long (C7,C9) tails, are investigated by dielectric and electro-optic contrast spectroscopic techniques. C4 shows sign reversal in the dielectric anisotropy Δε' as a function of both temperature and frequency, whereas C9 shows only negative Δε' in the entire mesophasic region. The behavior of C7 is intermediate of the two.

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We present spectroscopic and optical studies of a non-layer-shrinkage ferroelectric liquid crystal DSiKN65. The orientational order parameters S, measured with respect to the smectic layer normal using IR spectroscopy on a sample aligned homeotropically, does not exhibit any significant variation between the smectic-A∗ and smectic-C∗ phases. In contrast the birefringence of a planar homogenous sample abruptly increases at the smectic-A∗ to smectic-C∗ transition.

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