205 research outputs found

    ЀотоориСнтация ΠΈ Ρ„ΠΎΡ‚ΠΎΠΏΠ°Ρ‚Ρ‚Π΅Ρ€Π½ΠΈΠ½Π³: Новая ТидкокристалличСская тСхнология для дисплССв ΠΈ Ρ„ΠΎΡ‚ΠΎΠ½ΠΈΠΊΠΈ

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    Objectives. Since the end of the 20th century, liquid crystals have taken a leading position as a working material for the display industry. In particular, this is due to the advances in the control of surface orientation in thin layers of liquid crystals, which is necessary for setting the initial orientation of the layer structure in the absence of an electric field. The operation of most liquid crystal displays is based on electro-optical effects, arising from the changes in the initial orientation of the layers when the electric field is turned on, and the relaxation of the orientation structure under the action of surfaces after the electric field is turned off. In this regard, the high quality of surface orientation directly affects the technical characteristics of liquid crystal displays. The traditional technology of rubbing substrates, currently used in the display industry, has several disadvantages associated with the formation of a static charge on the substrates and surface contamination with microparticles. This review discusses an alternative photoalignment technology for liquid crystals on the surface, using materials sensitive to polarization of electromagnetic irradiation. Also, this review describes various applications of photosensitive azo dyes as photo-oriented materials. Results. The alternative photoalignment technology, which employs materials sensitive to electromagnetic polarization, allows to create the orientation of liquid crystals on the surface without mechanical impact and to control the surface anchoring force of a liquid crystal. This provides the benefits of using the photoalignment technology in the display industry and photonicsβ€”where the use of the rubbing technology is extremely difficult. The optical image rewriting mechanism is discussed, using electronic paper with photo-inert and photoaligned surfaces as an example. Further, different ways of using the photoalignment technology in liquid crystal photonics devices that control light beams are described. In particular, we consider switches, controllers and polarization rotators, optical attenuators, switchable diffraction gratings, polarization image analyzers, liquid crystal lenses, and ferroelectric liquid crystal displays with increased operation speed. Conclusions. The liquid crystal photoalignment and photopatterning technology is a promising tool for new display and photonics applications. It can be used for light polarization rotation; voltage controllable diffraction; fast switching of the liquid crystal refractive index; alignment of liquid crystals in super-thin photonic holes, curved and 3D surfaces; and many more applications.Π¦Π΅Π»ΠΈ. Π‘ ΠΊΠΎΠ½Ρ†Π° XX Π²Π΅ΠΊΠ° ΠΆΠΈΠ΄ΠΊΠΈΠ΅ кристаллы Π·Π°Π½ΠΈΠΌΠ°ΡŽΡ‚ Π»ΠΈΠ΄ΠΈΡ€ΡƒΡŽΡ‰Π΅Π΅ ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠ΅ срСди Ρ€Π°Π±ΠΎΡ‡ΠΈΡ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² для дисплСйной индустрии. Π’ частности, это стало Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹ΠΌ благодаря достиТСниям Π² области управлСния повСрхностной ΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠ΅ΠΉ Π² Ρ‚ΠΎΠ½ΠΊΠΈΡ… слоях ΠΆΠΈΠ΄ΠΊΠΈΡ… кристаллов, Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΠΉ для задания исходной ΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ структуры слоя Π² отсутствиС элСктричСского поля. Π Π°Π±ΠΎΡ‚Π° Π±ΠΎΠ»ΡŒΡˆΠΈΠ½ΡΡ‚Π²Π° ТидкокристалличСских дисплССв основана Π½Π° элСктрооптичСских эффСктах, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡŽΡ‰ΠΈΡ… Π·Π° счСт измСнСния исходной ΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ слоСв ΠΏΡ€ΠΈ Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠΈ элСктричСского поля ΠΈ ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ рСлаксации ΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ структуры ΠΏΠΎΠ΄ дСйствиСм повСрхностСй послС Π²Ρ‹ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΡ элСктричСского поля. По этой ΠΏΡ€ΠΈΡ‡ΠΈΠ½Π΅ высокоС качСство повСрхностной ΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ Π½Π°ΠΏΡ€ΡΠΌΡƒΡŽ влияСт Π½Π° тСхничСскиС характСристики ТидкокристалличСских дисплССв. Π˜ΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΠ°Ρ Π² настоящСС врСмя Π² дисплСйной индустрии традиционная Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ натирания ΠΏΠΎΠ΄Π»ΠΎΠΆΠ΅ΠΊ ΠΈΠΌΠ΅Π΅Ρ‚ ряд нСдостатков, связанных с ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π½Π° ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ°Ρ… статичСского заряда ΠΈ загрязнСниСм повСрхности микрочастицами. Π’ Π΄Π°Π½Π½ΠΎΠΌ ΠΎΠ±Π·ΠΎΡ€Π΅ рассмотрСна Π°Π»ΡŒΡ‚Π΅Ρ€Π½Π°Ρ‚ΠΈΠ²Π½Π°Ρ тСхнология Ρ„ΠΎΡ‚ΠΎΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ ΠΆΠΈΠ΄ΠΊΠΈΡ… кристаллов Π½Π° повСрхности с использованиСм ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ², Ρ‡ΡƒΠ²ΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΊ поляризации элСктромагнитного излучСния. Π’Π°ΠΊΠΆΠ΅ описаны Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Π΅ прилоТСния с использованиСм Ρ„ΠΎΡ‚ΠΎΡ‡ΡƒΠ²ΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… азокраситСлСй Π² качСствС Ρ„ΠΎΡ‚ΠΎΠΎΡ€ΠΈΠ΅Π½Ρ‚ΠΈΡ€ΡƒΠ΅ΠΌΡ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ². Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. ΠΠ»ΡŒΡ‚Π΅Ρ€Π½Π°Ρ‚ΠΈΠ²Π½Π°Ρ тСхнология Ρ„ΠΎΡ‚ΠΎΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ позволяСт ΡΠΎΠ·Π΄Π°Π²Π°Ρ‚ΡŒ ΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΡŽ ΠΆΠΈΠ΄ΠΊΠΈΡ… кристаллов Π½Π° повСрхности Π±Π΅Π· мСханичСского воздСйствия, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ силу сцСплСния ΠΆΠΈΠ΄ΠΊΠΎΠ³ΠΎ кристалла с ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚ΡŒΡŽ ΠΏΠΎΠ΄Π»ΠΎΠΆΠ΅ΠΊ. Π­Ρ‚ΠΎ обСспСчиваСт прСимущСство использования Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Ρ„ΠΎΡ‚ΠΎΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ Π² дисплСйной индустрии ΠΈ Π² Ρ„ΠΎΡ‚ΠΎΠ½ΠΈΠΊΠ΅, Π³Π΄Π΅ ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ натирания ΠΊΡ€Π°ΠΉΠ½Π΅ Π·Π°Ρ‚Ρ€ΡƒΠ΄Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ. На ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ элСктронной Π±ΡƒΠΌΠ°Π³ΠΈ с Ρ„ΠΎΡ‚ΠΎΠΈΠ½Π΅Ρ€Ρ‚Π½ΠΎΠΉ ΠΈ Ρ„ΠΎΡ‚ΠΎΡ‡ΡƒΠ²ΡΡ‚Π²ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ повСрхностями рассмотрСн ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌ оптичСской пСрСзаписи изобраТСния. ΠžΠΏΠΈΡΠ°Π½Ρ‹ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Π΅ Π²Π°Ρ€ΠΈΠ°Π½Ρ‚Ρ‹ использования Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Ρ„ΠΎΡ‚ΠΎΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ Π² ТидкокристалличСских устройствах Ρ„ΠΎΡ‚ΠΎΠ½ΠΈΠΊΠΈ, ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΡ… ΡƒΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠ΅ свСтовыми ΠΏΡƒΡ‡ΠΊΠ°ΠΌΠΈ. Π’ частности, рассмотрСны ΠΏΠ΅Ρ€Π΅ΠΊΠ»ΡŽΡ‡Π°Ρ‚Π΅Π»ΠΈ, ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»Π»Π΅Ρ€Ρ‹ ΠΈ Π²Ρ€Π°Ρ‰Π°Ρ‚Π΅Π»ΠΈ поляризации, оптичСскиС Π°Ρ‚Ρ‚Π΅Π½ΡŽΠ°Ρ‚ΠΎΡ€Ρ‹, ΠΏΠ΅Ρ€Π΅ΠΊΠ»ΡŽΡ‡Π°Π΅ΠΌΡ‹Π΅ Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΎΠ½Π½Ρ‹Π΅ Ρ€Π΅ΡˆΠ΅Ρ‚ΠΊΠΈ, поляризационныС Π°Π½Π°Π»ΠΈΠ·Π°Ρ‚ΠΎΡ€Ρ‹ изобраТСния, ТидкокристалличСскиС Π»ΠΈΠ½Π·Ρ‹, Π° Ρ‚Π°ΠΊΠΆΠ΅ фСрроэлСктричСскиС ТидкокристалличСскиС дисплСи с ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½Π½Ρ‹ΠΌ быстродСйствиСм. Π’Ρ‹Π²ΠΎΠ΄Ρ‹. ВСхнология Ρ„ΠΎΡ‚ΠΎΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ ΠΈ Ρ„ΠΎΡ‚ΠΎΠΏΠ°Ρ‚Ρ‚Π΅Ρ€Π½ΠΈΠ½Π³Π° ΠΆΠΈΠ΄ΠΊΠΈΡ… кристаллов являСтся ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±Π΅Ρ‰Π°ΡŽΡ‰Π΅ΠΉ для Π½ΠΎΠ²Ρ‹Ρ… ΠΏΡ€ΠΈΠ»ΠΎΠΆΠ΅Π½ΠΈΠΉ Π² области дисплССв ΠΈ Ρ„ΠΎΡ‚ΠΎΠ½ΠΈΠΊΠΈ. ВСхнология ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ использована для вращСния поляризации свСта; Π΄ΠΈΡ„Ρ€Π°ΠΊΡ†ΠΈΠΈ, управляСмой напряТСниСм; быстрого ΠΏΠ΅Ρ€Π΅ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΡ показатСля прСломлСния ΠΆΠΈΠ΄ΠΊΠΎΠ³ΠΎ кристалла; ΠΎΡ€ΠΈΠ΅Π½Ρ‚Π°Ρ†ΠΈΠΈ ΠΆΠΈΠ΄ΠΊΠΈΡ… кристаллов Π² супСртонких Ρ„ΠΎΡ‚ΠΎΠ½Π½Ρ‹Ρ… Π΄Ρ‹Ρ€Π°Ρ…, Π½Π° искривлСнных ΠΈ 3D повСрхностях; ΠΈ ΠΌΠ½ΠΎΠ³ΠΎΠ³ΠΎ Π΄Ρ€ΡƒΠ³ΠΎΠ³ΠΎ.

    Photoinduced ordering and anchoring properties of azo-dye films

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    We study both theoretically and experimentally anchoring properties of photoaligning azo-dye films in contact with a nematic liquid crystal depending on photoinduced ordering of azo-dye molecules. In the mean field approximation, we found that the bare surface anchoring energy linearly depends on the azo-dye order parameter and the azimuthal anchoring strength decays to zero in the limit of vanishing photoinduced ordering. From the absorption dichroism spectra measured in the azo-dye films that are prepared from the azo-dye derivative with polymerizable terminal groups (SDA-2) we obtain dependence of the dichroic ratio on the irradiation dose. We also measure the polar and azimuthal anchoring strengths in nematic liquid crystal (NLC) cells aligned by the azo-dye films and derive the anchoring strengths as functions of the dichroic ratio. Though linear fitting of the experimental data for both anchoring strengths gives reasonably well results, it, in contradiction with the theory, predicts vanishing of the azimuthal anchoring strength at certain nonzero value of the azo-dye order parameter. By using a simple phenomenological model we show that this discrepancy can be attributed to the difference between the surface and bulk order parameters in the films.Comment: revtex4, 25 pages, 9 figure

    Kinetics of photoinduced ordering in azo-dye films: two-state and diffusion models

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    We study the kinetics of photoinduced ordering in the azo-dye SD1 photoaligning layers and present the results of modeling performed using two different phenomenological approaches. A phenomenological two state model is deduced from the master equation for an ensemble of two-level molecular systems. Using an alternative approach, we formulate the two-dimensional (2D) diffusion model as the free energy Fokker-Planck equation simplified for the limiting regime of purely in-plane reorientation. The models are employed to interpret the irradiation time dependence of the absorption order parameters extracted from the available experimental data by using the exact solution to the light transmission problem for a biaxially anisotropic absorbing layer. The transient photoinduced structures are found to be biaxially anisotropic whereas the photosteady and the initial states are uniaxial.Comment: revtex4, 34 pages, 9 figure

    Carbon - containing covering for anchoring breaking nematic microdevices

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    We demonstrate experimentally, that inresidual atmosphere of scanning electron microscope the nano-scale carbon-containing (hydrocarbon) films by snuff effect can be produced. The micropattern of carbon film including axial-symmetric ones is defined by the e-beam rasteryesBelgorod State Universit

    Effects of polarization azimuth in dynamics of electrically assisted light-induced gliding of nematic liquid-crystal easy axis

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    We experimentally study the reorientation dynamics of the nematic liquid crystal easy axis at photoaligned azo-dye films under the combined action of in-plane electric field and reorienting UV light linearly polarized at varying polarization azimuth, ϕp\phi_p. In contrast to the case where the light polarization vector is parallel to the initial easy axis and ϕp=0\phi_p=0, at ϕp≠0\phi_p\ne 0, the pronounced purely photoinduced reorientation is observed outside the interelectrode gaps. In the regions between electrodes with non-zero electric field, it is found that the dynamics of reorientation slows down with ϕp\phi_p and the sense of easy axis rotation is independent of the sign of ϕp\phi_p.Comment: revtex-4.1, 4 pages, 3 figure

    Photoinduced reordering in thin azo-dye films and light-induced reorientation dynamics of nematic liquid-crystal easy axis

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    We theoretically study the kinetics of photoinduced reordering triggered by linearly polarized (LP) reorienting light in thin azo-dye films that were initially illuminated with LP ultraviolet (UV) pumping beam. The process of reordering is treated as a rotational diffusion of molecules in the light intensity-dependent mean-field potential. The two dimensional diffusion model which is based on the free energy rotational Fokker-Planck equation and describes the regime of in-plane reorientation is generalized to analyze the dynamics of the azo-dye order parameter tensor at varying polarization azimuth of the reorienting light. It is found that, in the photosteady state, the intensity of LP reorienting light determines the scalar order parameter (the largest eigenvalue of the order parameter tensor), whereas the steady state orientation of the corresponding eigenvector (the in-plane principal axis) depends solely on the polarization azimuth. We show that, under certain conditions, reorientation takes place only if the reorienting light intensity exceeds its critical value. Such threshold behavior is predicted to occur in the bistability region provided that the initial principal axis lies in the polarization plane of reorienting light. The model is used to interpret the experimental data on the light-induced azimuthal gliding of liquid-crystal easy axis on photoaligned azo-dye substrates.Comment: 27 pages, 11 fugure

    Liquid crystal anchoring transitions on aligning substrates processed by plasma beam

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    We observe a sequence of the anchoring transitions in nematic liquid crystals (NLC) sandwiched between the hydrophobic polyimide substrates treated with the plasma beam. There is a pronounced continuous transition from homeotropic to low tilted (nearly planar) alignment with the easy axis parallel to the incidence plane of the plasma beam (the zenithal transition) that takes place as the exposure dose increases. In NLC with positive dielectric anisotropy, a further increase in the exposure dose results in in-plane reorientation of the easy axis by 90 degrees (the azimuthal transition). This transition occurs through the two-fold degenerated alignment characteristic for the second order anchoring transitions. In contrast to critical behavior of anchoring, the contact angle of NLC and water on the treated substrates monotonically declines with the exposure dose. It follows that the surface concentration of hydrophobic chains decreases continuously. The anchoring transitions under consideration are qualitatively interpreted by using a simple phenomenological model of competing easy axes which is studied by analyzing anchoring diagrams of the generalized polar and non-polar anchoring models.Comment: revtex4, 18 pages, 10 figure

    Orientational instabilities in nematics with weak anchoring under combined action of steady flow and external fields

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    We study the homogeneous and the spatially periodic instabilities in a nematic liquid crystal layer subjected to steady plane {\em Couette} or {\em Poiseuille} flow. The initial director orientation is perpendicular to the flow plane. Weak anchoring at the confining plates and the influence of the external {\em electric} and/or {\em magnetic} field are taken into account. Approximate expressions for the critical shear rate are presented and compared with semi-analytical solutions in case of Couette flow and numerical solutions of the full set of nematodynamic equations for Poiseuille flow. In particular the dependence of the type of instability and the threshold on the azimuthal and the polar anchoring strength and external fields is analysed.Comment: 12 pages, 6 figure
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