1,978 research outputs found
Active tuning of photonic device characteristics during operation by ferroelectric domain switching
Ferroelectrics have many unusual properties. Two properties that are often exploited are first, their complex, nonlinear optical response and second, their strong nonlinear coupling between electromagnetic and mechanical fields through the domain patterns or microstructure. The former has led to the use of ferroelectrics in optical devices and the latter is used in ferroelectric sensors and actuators. We show the feasibility of using these properties together in nanoscale photonic devices. The electromechanical coupling allows us to change the domain patterns or microstructure. This in turn changes the optical characteristics. Together, these could provide photonic devices with tunable properties. We present calculations for two model devices. First, in a photonic crystal consisting of a triangular lattice of air holes in barium titanate, we find the change in the band structure when the domains are switched. The change is significant compared to the frequency spread of currently available high-quality light sources and may provide a strategy for optical switching. Second, we show that periodically poled 90Β° domain patterns, despite their complex geometry, do not cause dispersion or have band gaps. Hence, they may provide an alternative to the antiparallel domains that are usually used in quasiphase matching and allow for tunable higher-harmonic generation
Frequency tunability of solid-core photonic crystal fibers filled with nanoparticle-doped liquid crystals
We infiltrate liquid crystals doped with BaTiO3 nanoparticles in a photonic crystal fiber and compare the measured transmission spectrum with the one achieved without dopant. New interesting features, such as frequency modulation response of the device and a transmission spectrum with tunable attenuation on the short wavelength side of the widest bandgap, suggest a potential application of this device as a tunable all-in-fiber gain equalization filter with an adjustable slope. The tunability of the device is achieved by varying the amplitude and the frequency of the applied external electric field. The threshold voltage for doped and undoped liquid crystals in a silica capillary and in a glass cell are also measured as a function of the frequency of the external electric field and the achieved results are compared
Ferroelectric Based Photonic Crystal Cavity by Liquid Crystal Infiltration
Cataloged from PDF version of article.A novel type of two-dimensional photonic crystal is investigated for it optical properties as a core-shell-type ferroelectric nanorod infiltrated with nematic liquid crystals. Using the plane wave expansion method and finite-difference time-domain method, the photonic crystal structure, which is composed of a photonic crystal in a core-shell-type ferroelectric nanorod, is designed for the square lattice and the hexagonal lattice. It has been used 5CB as a photonic crystal core, and LiNbO3 as a ferroelectric material. The photonic crystal with a core-shell-type LiNbO3 nanorod infiltrated with nematic liquid crystals is compared with the photonic crystal with solid LiNbO3 rods and the photonic crystal with hollow LiNbO3 rods
Liquid Crystals on Ferroelectric Thin Films
Barium titanate (BTO) and lead zirconate titanate (PZT) are two of the most common ferroelectric materials used in applications. These two materials offer excellent dielectric, piezo-electric, electro-optic and pyro-electric properties. The excellent electro-optic properties of our PZT and BTO deposited thin films may lead to cheap and versatile ultra-fast electro-optic modulators on existing photonic platforms [1], such as the Si or the SiN nanophotonic platform. In this work however, we exploit the extremely high dielectric permittivity of PZT (in the order of 500 to 1000). The permittivity is quasi independent of the underlying substrate material (glass, glass + ITO, glass + Pt, Si, etc.).
Liquid crystals exhibit electro-optic effects that are an order of magnitude larger compared to PZT, which makes them ideal materials for use in beam steering applications of focus tunable lenses. In these applications the liquid crystal imposes a spatially varying optical path length to light passing through the liquid crystal layer. By working with a number of separately addressable electrodes the optical path length variation can be accurately controlled. Using multi-electrode designs for example, tunable lenses with high optical quality have been demonstrated. One major problem of multi-electrode designs is the appearance of fringe fields which leads to unwanted behavior of the liquid crystal and may eventually lead to the formation of disclination lines which reduces the optical performance drastically. Using a PZT thin film, we demonstrate that the fringe fields are eliminated and that designs with fewer separately addressable electrodes are necessary. Tunable lenses with a liquid crystal layer integrated on top of a PZT layer are demonstrated [2].
Next to the experimental demonstration we provide numerical simulations of the effect of the high permittivity layer on the liquid crystal.
[1] J.P. George, et al. Lanthanide-Assisted Deposition of Strongly Electro-optic PZT Thin Films on Silicon: Toward Integrated Active Nanophotonic Devices. ACS Appl. Mater. Inter. 7 13350-9 (2015)
[2] O. Willekens, et al., Ferroelectric thin films with liquid crystal for gradient index applications, Optics Express (submitted
Π€ΠΎΡΠΎΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΡ ΠΈ ΡΠΎΡΠΎΠΏΠ°ΡΡΠ΅ΡΠ½ΠΈΠ½Π³: ΠΠΎΠ²Π°Ρ ΠΆΠΈΠ΄ΠΊΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠ΅Ρ Π½ΠΎΠ»ΠΎΠ³ΠΈΡ Π΄Π»Ρ Π΄ΠΈΡΠΏΠ»Π΅Π΅Π² ΠΈ ΡΠΎΡΠΎΠ½ΠΈΠΊΠΈ
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 photonicsβwhere 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‘ ΠΊΠΎΠ½ΡΠ° XX Π²Π΅ΠΊΠ° ΠΆΠΈΠ΄ΠΊΠΈΠ΅ ΠΊΡΠΈΡΡΠ°Π»Π»Ρ Π·Π°Π½ΠΈΠΌΠ°ΡΡ Π»ΠΈΠ΄ΠΈΡΡΡΡΠ΅Π΅ ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠ΅ ΡΡΠ΅Π΄ΠΈ ΡΠ°Π±ΠΎΡΠΈΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Π΄Π»Ρ Π΄ΠΈΡΠΏΠ»Π΅ΠΉΠ½ΠΎΠΉ ΠΈΠ½Π΄ΡΡΡΡΠΈΠΈ. Π ΡΠ°ΡΡΠ½ΠΎΡΡΠΈ, ΡΡΠΎ ΡΡΠ°Π»ΠΎ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠΌ Π±Π»Π°Π³ΠΎΠ΄Π°ΡΡ Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΡΠΌ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΠΎΠΉ ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠ΅ΠΉ Π² ΡΠΎΠ½ΠΊΠΈΡ
ΡΠ»ΠΎΡΡ
ΠΆΠΈΠ΄ΠΊΠΈΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ², Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΠΉ Π΄Π»Ρ Π·Π°Π΄Π°Π½ΠΈΡ ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠΉ ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ ΡΠ»ΠΎΡ Π² ΠΎΡΡΡΡΡΡΠ²ΠΈΠ΅ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ. Π Π°Π±ΠΎΡΠ° Π±ΠΎΠ»ΡΡΠΈΠ½ΡΡΠ²Π° ΠΆΠΈΠ΄ΠΊΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄ΠΈΡΠΏΠ»Π΅Π΅Π² ΠΎΡΠ½ΠΎΠ²Π°Π½Π° Π½Π° ΡΠ»Π΅ΠΊΡΡΠΎΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΡΠ΅ΠΊΡΠ°Ρ
, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡΠΈΡ
Π·Π° ΡΡΠ΅Ρ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΈΡΡ
ΠΎΠ΄Π½ΠΎΠΉ ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ ΡΠ»ΠΎΠ΅Π² ΠΏΡΠΈ Π²ΠΊΠ»ΡΡΠ΅Π½ΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ ΠΈ ΠΎΠ±ΡΠ°ΡΠ½ΠΎΠΉ ΡΠ΅Π»Π°ΠΊΡΠ°ΡΠΈΠΈ ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΡΡΡΠΊΡΡΡΡ ΠΏΠΎΠ΄ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ΅ΠΉ ΠΏΠΎΡΠ»Π΅ Π²ΡΠΊΠ»ΡΡΠ΅Π½ΠΈΡ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΠΎΠ»Ρ. ΠΠΎ ΡΡΠΎΠΉ ΠΏΡΠΈΡΠΈΠ½Π΅ Π²ΡΡΠΎΠΊΠΎΠ΅ ΠΊΠ°ΡΠ΅ΡΡΠ²ΠΎ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΠΎΠΉ ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ Π½Π°ΠΏΡΡΠΌΡΡ Π²Π»ΠΈΡΠ΅Ρ Π½Π° ΡΠ΅Ρ
Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ ΠΆΠΈΠ΄ΠΊΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄ΠΈΡΠΏΠ»Π΅Π΅Π². ΠΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΠΌΠ°Ρ Π² Π½Π°ΡΡΠΎΡΡΠ΅Π΅ Π²ΡΠ΅ΠΌΡ Π² Π΄ΠΈΡΠΏΠ»Π΅ΠΉΠ½ΠΎΠΉ ΠΈΠ½Π΄ΡΡΡΡΠΈΠΈ ΡΡΠ°Π΄ΠΈΡΠΈΠΎΠ½Π½Π°Ρ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π½Π°ΡΠΈΡΠ°Π½ΠΈΡ ΠΏΠΎΠ΄Π»ΠΎΠΆΠ΅ΠΊ ΠΈΠΌΠ΅Π΅Ρ ΡΡΠ΄ Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΊΠΎΠ², ΡΠ²ΡΠ·Π°Π½Π½ΡΡ
Ρ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π½Π° ΠΏΠΎΠ΄Π»ΠΎΠΆΠΊΠ°Ρ
ΡΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π·Π°ΡΡΠ΄Π° ΠΈ Π·Π°Π³ΡΡΠ·Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΌΠΈΠΊΡΠΎΡΠ°ΡΡΠΈΡΠ°ΠΌΠΈ. Π Π΄Π°Π½Π½ΠΎΠΌ ΠΎΠ±Π·ΠΎΡΠ΅ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½Π° Π°Π»ΡΡΠ΅ΡΠ½Π°ΡΠΈΠ²Π½Π°Ρ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡ ΡΠΎΡΠΎΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ ΠΆΠΈΠ΄ΠΊΠΈΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², ΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΊ ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ. Π’Π°ΠΊΠΆΠ΅ ΠΎΠΏΠΈΡΠ°Π½Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ ΠΏΡΠΈΠ»ΠΎΠΆΠ΅Π½ΠΈΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΎΡΠΎΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΡΡ
Π°Π·ΠΎΠΊΡΠ°ΡΠΈΡΠ΅Π»Π΅ΠΉ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΡΠΎΡΠΎΠΎΡΠΈΠ΅Π½ΡΠΈΡΡΠ΅ΠΌΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ². Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΠ»ΡΡΠ΅ΡΠ½Π°ΡΠΈΠ²Π½Π°Ρ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡ ΡΠΎΡΠΎΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΡΠΎΠ·Π΄Π°Π²Π°ΡΡ ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΡ ΠΆΠΈΠ΄ΠΊΠΈΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ Π±Π΅Π· ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΊΠΎΠ½ΡΡΠΎΠ»ΠΈΡΠΎΠ²Π°ΡΡ ΡΠΈΠ»Ρ ΡΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡ ΠΆΠΈΠ΄ΠΊΠΎΠ³ΠΎ ΠΊΡΠΈΡΡΠ°Π»Π»Π° Ρ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΡ ΠΏΠΎΠ΄Π»ΠΎΠΆΠ΅ΠΊ. ΠΡΠΎ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Π΅Ρ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΡΠΎΡΠΎΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ Π² Π΄ΠΈΡΠΏΠ»Π΅ΠΉΠ½ΠΎΠΉ ΠΈΠ½Π΄ΡΡΡΡΠΈΠΈ ΠΈ Π² ΡΠΎΡΠΎΠ½ΠΈΠΊΠ΅, Π³Π΄Π΅ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π½Π°ΡΠΈΡΠ°Π½ΠΈΡ ΠΊΡΠ°ΠΉΠ½Π΅ Π·Π°ΡΡΡΠ΄Π½ΠΈΡΠ΅Π»ΡΠ½ΠΎ. ΠΠ° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ Π±ΡΠΌΠ°Π³ΠΈ Ρ ΡΠΎΡΠΎΠΈΠ½Π΅ΡΡΠ½ΠΎΠΉ ΠΈ ΡΠΎΡΠΎΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΠΌΠΈ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΠ΅ΡΠ΅Π·Π°ΠΏΠΈΡΠΈ ΠΈΠ·ΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΡ. ΠΠΏΠΈΡΠ°Π½Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ Π²Π°ΡΠΈΠ°Π½ΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΡΠΎΡΠΎΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ Π² ΠΆΠΈΠ΄ΠΊΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΡΡΠΎΠΉΡΡΠ²Π°Ρ
ΡΠΎΡΠΎΠ½ΠΈΠΊΠΈ, ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°ΡΡΠΈΡ
ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ ΡΠ²Π΅ΡΠΎΠ²ΡΠΌΠΈ ΠΏΡΡΠΊΠ°ΠΌΠΈ. Π ΡΠ°ΡΡΠ½ΠΎΡΡΠΈ, ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΠΏΠ΅ΡΠ΅ΠΊΠ»ΡΡΠ°ΡΠ΅Π»ΠΈ, ΠΊΠΎΠ½ΡΡΠΎΠ»Π»Π΅ΡΡ ΠΈ Π²ΡΠ°ΡΠ°ΡΠ΅Π»ΠΈ ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ, ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π°ΡΡΠ΅Π½ΡΠ°ΡΠΎΡΡ, ΠΏΠ΅ΡΠ΅ΠΊΠ»ΡΡΠ°Π΅ΠΌΡΠ΅ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΠ΅ ΡΠ΅ΡΠ΅ΡΠΊΠΈ, ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΎΠ½Π½ΡΠ΅ Π°Π½Π°Π»ΠΈΠ·Π°ΡΠΎΡΡ ΠΈΠ·ΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΡ, ΠΆΠΈΠ΄ΠΊΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π»ΠΈΠ½Π·Ρ, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠ΅ΡΡΠΎΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΆΠΈΠ΄ΠΊΠΎΠΊΡΠΈΡΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π΄ΠΈΡΠΏΠ»Π΅ΠΈ Ρ ΠΏΠΎΠ²ΡΡΠ΅Π½Π½ΡΠΌ Π±ΡΡΡΡΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ. ΠΡΠ²ΠΎΠ΄Ρ. Π’Π΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡ ΡΠΎΡΠΎΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ ΠΈ ΡΠΎΡΠΎΠΏΠ°ΡΡΠ΅ΡΠ½ΠΈΠ½Π³Π° ΠΆΠΈΠ΄ΠΊΠΈΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±Π΅ΡΠ°ΡΡΠ΅ΠΉ Π΄Π»Ρ Π½ΠΎΠ²ΡΡ
ΠΏΡΠΈΠ»ΠΎΠΆΠ΅Π½ΠΈΠΉ Π² ΠΎΠ±Π»Π°ΡΡΠΈ Π΄ΠΈΡΠΏΠ»Π΅Π΅Π² ΠΈ ΡΠΎΡΠΎΠ½ΠΈΠΊΠΈ. Π’Π΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Π° Π΄Π»Ρ Π²ΡΠ°ΡΠ΅Π½ΠΈΡ ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ ΡΠ²Π΅ΡΠ°; Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ, ΡΠΏΡΠ°Π²Π»ΡΠ΅ΠΌΠΎΠΉ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠ΅ΠΌ; Π±ΡΡΡΡΠΎΠ³ΠΎ ΠΏΠ΅ΡΠ΅ΠΊΠ»ΡΡΠ΅Π½ΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ ΠΏΡΠ΅Π»ΠΎΠΌΠ»Π΅Π½ΠΈΡ ΠΆΠΈΠ΄ΠΊΠΎΠ³ΠΎ ΠΊΡΠΈΡΡΠ°Π»Π»Π°; ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ ΠΆΠΈΠ΄ΠΊΠΈΡ
ΠΊΡΠΈΡΡΠ°Π»Π»ΠΎΠ² Π² ΡΡΠΏΠ΅ΡΡΠΎΠ½ΠΊΠΈΡ
ΡΠΎΡΠΎΠ½Π½ΡΡ
Π΄ΡΡΠ°Ρ
, Π½Π° ΠΈΡΠΊΡΠΈΠ²Π»Π΅Π½Π½ΡΡ
ΠΈ 3D ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΡ
; ΠΈ ΠΌΠ½ΠΎΠ³ΠΎΠ³ΠΎ Π΄ΡΡΠ³ΠΎΠ³ΠΎ.
- β¦