Liquid Crystal Unit Research Articles

Optical Information Encryption Based on Secret Sharing Liquid Crystal Elements with Spatial Dislocation

AbstractOptical encryption is an increasingly significant technique in the realm of information security. In the recent decade, there has been considerable interest in using planar optics elements for information encryption. However, information leakage possibly occurs due to limited encrytion channels available for single‐layer devices. To circumvent this problem, a novel encryption method is put forward using secret sharing cascaded liquid crystal (LC) elements with spatial dislocation, which can produce near‐field patterns and far‐field holographic images under different illumination conditions. Specifically, Malus's Law and its inherent one‐to‐four mapping of rotational degeneracy, along with the Pancharatnam‐Berry (PB) phase introduced by LC molecules, to achieve multi‐channel encryption are utilized. Therefore, each cascaded LC unit can manipulate the amplitude and phase imparted to output light independently, thus only by obtaining both LC devices can decryption be realized. To further enhance the encryption security, the author purposely divide each LC device into multiple regions and find that the encrypted patterns can only be recovered when the two LC elements align precisely with a specific dislocation. These experimental measurements agree well with the design, thus demonstrating the strong encryption capability and broad application prospects of the design approach in the field of optical encryption with high cost‐effectiveness.

Two‐Step Photoalignment with High Resolution for the Alignment of Blue Phase Liquid Crystal

AbstractThe self‐assembling properties of liquid crystal (LC) are ideal for realizing switchable optical components. The director organization is strongly determined by the alignment at the substrate interfaces and photoalignment is a versatile method based on linearly polarized UV light. In this work, a two‐step photoalignment procedure is proposed to pattern the alignment at the surface. Illumination with uniform polarization or with an interference pattern is combined to obtain stripe patterns or square patterns of photoalignment. It can indeed be confirmed that the nematic director follows the varying azimuthal orientation. By increasing the angle between the two interfering beams, photoalignment with sub‐micrometer resolution is obtained, compatible with the dimensions of blue phase (BP) LC unit cell. Homogeneous domains of BP II with (100) or (110) crystal orientation are obtained and their Kossel patterns are recorded. The two‐step photoalignment technique allows to create patterns with high resolution and to control the orientation of BP LC, which is promising for photonic applications that require single domains.

The influence of flexible spacer and the chirality of the core on the formation of chiral nematic phase of symmetric dimers containing trifluoromethyl terminal

ABSTRACTSeven symmetric liquid crystal (LC) dimers containing different chiral cores and LC arms have been synthesised, termed EPDA-(R,S)PD, TFBDA-(R,S)PD, TFBA-(R,S)PD, TFBDA-(R)PD, TFBA-(R)PD, TFBDA-IB and TFBA-IB, respectively. TFBDA-(R,S)PD, TFBA-(R,S)PD, TFBDA-(R)PD and TFBDA-IB displayed chiral smectic A (SmA*) phase, while EPDA-(R,S)PD, TFBA-(R)PD and TFBA-IB exhibited chiral nematic (N*) phase. The effects of flexible spacer, structural type of LC arms and the chirality of the cores on the thermal properties of the dimers and the formation of N* phase have been studied. The results indicated that the chiral core was prone to induce the N* phase in LC dimer that contained nematic arms although the chirality of the core is very weak, while for the smectic LC arms containing CF3 terminal, the removal of the flexible spacer between chiral core and rigid LC units was conducive to the formation of N* phase. For example, TFBDA-(R)PD and TFBDA-IB displayed SmA* phase, while TFBA-(R)PD and TFBA-IB exhibited N* phase. However TFBA-(R,S)PD did not display N* phase, which reminded us that the chirality of the core and the conformation of the dimer also played an influence in the formation of the LC phase.

Synthesis, Self-Assembly, and Drug-Release Properties of New Amphipathic Liquid Crystal Polycarbonates.

New amphiphilic liquid crystal (LC) polycarbonate block copolymers containing side-chain cholesteryl units were synthesized. Their structure, thermal stability, and LC phase behavior were characterized with Fourier transform infrared (FT-IR) spectrum, 1H NMR, gel permeation chromatographic (GPC), thermogravimetric analysis (TGA), differential scanning calorimetry (DSC), polarizing optical microscope (POM), and XRD methods. The results demonstrated that the LC copolymers showed a double molecular arrangement of a smectic A phase at room temperature. With the elevating of LC unit content in such LC copolymers, the corresponding properties including decomposition temperature (Td), glass temperature (Tg), and isotropic temperature (Ti) increased. The LC copolymers showed pH-responsive self-assembly behavior under the weakly acidic condition, and with more side-chain LC units, the self-assembly process was faster, and the formed particle size was smaller. It indicated that the self-assembly driving force was derived from the orientational ability of LC. The particle size and morphologies of self-assembled microspheres loaded with doxorubicin (DOX), together with drug release tracking, were evaluated by dynamic light scattering (DLS), SEM, and UV–vis spectroscopy. The results showed that DOX could be quickly released in a weakly acidic environment due to the pH response of the self-assembled microspheres. This would offer a new strategy for drug delivery in clinic applications.

Two-step crosslinked liquid-crystalline elastomer with reversible two-way shape memory characteristics

ABSTRACTLiquid-crystalline elastomers (LCEs) possess large and equilibrium reversible anisotropic dimensional change in response to applied stimuli. The deformation behavior demonstrated by current LCE materials under the stimuli are generally determined by their own geometries and the alignment distributions of liquid crystal (LC) units in the LCE matrices. Here we report a LCE whose synthesis was through a two-stage crosslinking coupled with a mechanical reshaping process, where the shape was mechanically reset before the final crosslinking. It demonstrated reversible memory and change between the initial geometries formed during the first crosslinking stage and any reshaped geometries under the stimuli. Its deformation is not influenced by the geometries and the alignment distributions of LC units in the LCE matrix. This characteristic in LCEs holds promise in a wide range of application researches requiring sophisticated functions and smart structures.

On the application of positron annihilation spectroscopy for studying the photodestruction of biological membranes

Possible therapeutic applications of methods of positron annihilation spectroscopy (PAS) with low-energy positron beams are discussed in this review. These methods are used to study the defect structure of material layers of micro- and submicrometer size (surface layers in electronic devices, cell walls and liquid-crystal units in biomedical applications, etc.). We consider a model of analysis with the positron annihilation-lifetime spectroscopy (PALS) method for the states of irradiated membranes of bacterial cells in a cycle of photodynamic therapy, which lies in the destruction or irreversible oxidative damage of pathogenic cells by the photo-inactivated oxygen of a photosensitizer incorporated into the target cell immediately before light exposure.

Morphology and thermal properties of liquid crystalp-PAEB/styrene copolymer

The homopolymer of unsaturated liquid crystal (LC) monomer for p-phenylene di {4-[2-(allyloxy) ethoxy] benzoate} (p-PAEB), and copolymer poly (p-PAEB/St) of p-PAEB with styrene (St) have been synthesized. The LC behavior and thermal properties of p-PAEB and poly(p-PAEB/St) have been studied by Polarizing Optical Microscopic (POM), Differential Scanning Calorimetry, X-Ray Diffractometer (XRD), and Torsional Braid Analysis (TBA). The results demonstrate that LC phase texture and phase transition temperature of copolymers are affected by the composition of LC units in copolymers. The POM and XRD reveal that p-PAEB has a smectic phase structure; the copolymer of p-PAEB with styrene reveal deformed focal conics texture of smectic phase. The phase transition temperature range of p-PAEB is 120.5–191.5°C, but the homopolymer of p-PAEB has a broad LC temperature range from 77 to 170°C. The LC temperature range of poly(p-PAEB/St) is broadened with increased content of p-PAEB. The dynamic mechanical properties of LC polymer networks were investigated with TBA. The results indicate that the peak temperature of maximal mechanical loss is 114°C and is decreased with the addition of styrene © 2006 Wiley Periodicals, Inc. J Appl Polym Sci 102: 5731–5736, 2006