383 research outputs found
ΠΡΠΈΡΠΈΠ½Ρ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ ΠΊΠΎΠΌΠΌΡΠ½ΠΈΠΊΠ°ΡΠΈΠ²Π½ΡΡ Π½Π΅ΡΠ΄Π°Ρ Π² ΠΏΠΎΠ»ΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΡΠ΅ΠΊΡΡΠ΅: Π»ΠΈΠ½Π³Π²ΠΎΠΏΡΠ°Π³ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ Π°ΡΠΏΠ΅ΠΊΡ
ΠΠΎΠ½Π΄ΡΠ°ΡΠ΅Π½ΠΊΠΎ Π. Π. ΠΡΠΈΡΠΈΠ½Ρ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΡ ΠΊΠΎΠΌΠΌΡΠ½ΠΈΠΊΠ°ΡΠΈΠ²Π½ΡΡ
Π½Π΅ΡΠ΄Π°Ρ Π² ΠΏΠΎΠ»ΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΡΠ΅ΠΊΡΡΠ΅: Π»ΠΈΠ½Π³Π²ΠΎΠΏΡΠ°Π³ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ Π°ΡΠΏΠ΅ΠΊΡ / Π. Π. ΠΠΎΠ½Π΄ΡΠ°ΡΠ΅Π½ΠΊΠΎ // ΠΠ΄Π΅ΡΡΠΊΠΈΠΉ Π»ΡΠ½Π³Π²ΡΡΡΠΈΡΠ½ΠΈΠΉ Π²ΡΡΠ½ΠΈΠΊ : Π·Π±. Π½Π°ΡΠΊ. ΠΏΡΠ°ΡΡ / [Π³ΠΎΠ»ΠΎΠ². ΡΠ΅Π΄. Π. Π. ΠΠ΅ΡΠ»ΡΡΠ΅Π½ΠΊΠΎ] ; ΠΠ°Ρ. ΡΠ½-Ρ Β«ΠΠ΄Π΅Ρ. ΡΡΠΈΠ΄. Π°ΠΊΠ°Π΄.Β». β ΠΠΈΠΏ. 3.- Π‘ΠΏΠ΅Ρ. Π²ΠΈΠΏ., ΠΏΡΠΈΡΠ²ΡΡΠ΅Π½ΠΈΠΉ 200-ΡΡΡΡΡ Π²ΡΠ΄ Π΄Π½Ρ Π½Π°ΡΠΎΠ΄ΠΆΠ΅Π½Π½Ρ Π’. Π. Π¨Π΅Π²ΡΠ΅Π½ΠΊΠ°. β ΠΠ΄Π΅ΡΠ° : ΠΠ΅Π»ΡΠ²Π΅ΡΠΈΠΊΠ°, 2014. β Π‘. 118-123.Π‘ΡΠ°ΡΡΡ ΠΏΠΎΡΠ²ΡΡΠ΅Π½Π° ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ ΠΊΠΎΠΌΠΌΡΠ½ΠΈΠΊΠ°ΡΠΈΠ²Π½ΡΡ
Π½Π΅ΡΠ΄Π°Ρ ΠΊΠ°ΠΊ Π½Π΅ΠΏΠΎΠ½ΠΈ- ΠΌΠ°Π½ΠΈΡ ΡΠ΅ΡΠΈΠΏΠΈΠ΅Π½ΡΠΎΠΌ Π½Π°ΠΌΠ΅ΡΠ΅Π½ΠΈΡ Π³ΠΎΠ²ΠΎΡΡΡΠ΅Π³ΠΎ. Π ΠΏΠΎΠ»ΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΌ Π΄ΠΈΡΠΊΡΡΡΠ΅ ΠΊΠΎΠΌΠΌΡΠ½ΠΈΠΊΠ°ΡΠΈΠ²Π½ΡΠ΅ Π½Π΅ΡΠ΄Π°ΡΠΈ ΠΌΠΎΠ³ΡΡ Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡ Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ Π½Π΅ΠΏΡΠ°Π²ΠΈΠ»ΡΠ½ΠΎ ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠ΅ΠΊΡΡΠ°, Π² ΡΠ°ΡΡΠ½ΠΎΡΡΠΈ Π΅Π³ΠΎ Π΄Π΅ΡΠ΅ΠΌΠ°Π½ΡΠΈΠ·Π°ΡΠΈΠΈ. ΠΡΠΈΡΠΈΠ½ΠΎΠΉ ΡΡΡΠ°ΡΡ ΡΠΌΡΡΠ»Π° Π² ΠΏΠΎΠ»ΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΡΠ΅ΠΊΡΡΠ΅ ΡΡΠ°Π½ΠΎΠ²ΡΡΡΡ Π»Π΅ΠΊΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈ Π³ΡΠ°ΠΌΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ°Π±Π»ΠΎΠ½Ρ, ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΊΠΎΡΠΎΡΡΡ
ΠΈ ΡΠ½ΠΈΠΆΠ°Π΅Ρ ΡΠΌΡΡΠ»ΠΎΠ²ΡΡ Π½Π°Π³ΡΡΠ·ΠΊΡ Π½Π° ΡΠ΅ΡΠΈΠΏΠΈΠ΅Π½ΡΠ°
Growth and crystallization of molybdenum layers on amorphous silicon
The structure of molybdenum layers deposited by direct current magnetron sputtering onto the amorphous silicon (a-Si) layers as function of nominal layer thickness was studied by methods of transmission electron microscopy. Molybdenum layers with nominal thickness 1.5btMo nomb1.9 nm consist of clusters which should be considered as a transient state between strongly disordered (amorphous) state and crystal one. A transition from clusters to polycrystals takes place within the thickness range of 1.9btMo nomb2.5 nm. Resulting Mo crystallites have an inequiaxial form with dimensions of (3β4)Γ(15β30)nm2 and consist of blocks. The lateral axis of inequiaxial crystallites is parallel to 110 direction. As the metal layer thickness increases Mocrystallites take the more regular form at the expense of recrystallization
Reactive diffusion in Sc/Si multilayer X-ray mirrors with CrB2 barrier layers
Processes undergoing in Sc/Si multilayer X-ray mirrors (MXMs) with periods of βΌ27 nm and barrier layers of CrB20.3- and 0.7-nm thick within the temperature range
of 420β780 K were studied by methods of small-angle Xray reflectivity (Ξ» = 0.154 nm) and cross-sectional transmission electron microscopy. All layers with the exception of
Sc ones are amorphous. Barrier layers are stable at least up to a temperature of 625 K and double the activation energy of diffusional intermixing at moderate temperatures. Introduction of barriers improves the thermal stability of Sc/Si MXMs at least by 80 degrees. Diffusion of Si atoms through barrier layers into Sc layers with formation of silicides was shown to be the main degradation mechanism of MXMs. A comparison of the stability for Sc/Si MXMs with different barriers published in the literature is conducted. The ways of further improvement of barrier properties are discusse
Theory of transverse spin dynamics in a polarized Fermi liquid and an itinerant ferromagnet
The linear equations for transverse spin dynamics in a weakly polarized
degenerate Fermi liquid with arbitrary relationship between temperature and
polarization are derived from Landau-Silin phenomenological kinetic equation
with general form of two-particle collision integral. Unlike the previous
treatment where Fermi velocity and density of states have been taken as
constants independent of polarization here we made derivation free from this
assumption. The obtained equations are applicable for description of spin
dynamics in paramagnetic Fermi liquid with finite polarization as well in an
itinerant ferromagnet. In both cases transverse spin wave frequency is found to
be proportional to the square of the wave vector with complex constant of
proportionality (diffusion coefficient) such that the damping has a finite
value at T=0. The polarization dependence of the diffusion coefficient is found
to be different for a polarized Fermi liquid and for an itinerant ferromagnet.
These conclusions are confirmed by derivation of transverse spin wave
dispersion law in frame of field theoretical methods from the integral equation
for the vortex function. It is shown that similar derivation taking into
consideration the divergency of static transverse susceptibility also leads to
the same attenuating spin wave spectrum.Comment: 7 pages, no figure
Skin effect with arbitrary specularity in Maxwellian plasma
The problem of skin effect with arbitrary specularity in maxwellian plasma
with specular--diffuse boundary conditions is solved. A new analytical method
is developed that makes it possible to to obtain a solution up to an arbitrary
degree of accuracy. The method is based on the idea of symmetric continuation
not only the electric field, but also electron distribution function. The
solution is obtained in a form of von Neumann series.Comment: 7 pages, 2 figure
Π‘Π°Π½ΠΊΡΠΈΠΈ ΠΏΡΠΎΡΠΈΠ² Π ΠΎΡΡΠΈΠΈ: ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΈ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΡ Π ΠΎΡΡΠΈΠΈ
The current stage of development of the entire world community, including Russia, is associated with such a thing as βsanction warsβ. As an example, one can recall the introduction of US sanctions against China, Iran, Venezuela, and other countries, European sanctions, as well as various countersanctions of countries subjected to sanction pressure.As part of this paper, the sanctions imposed against Russia in connection with the Ukrainian crisis in 2014 and countersanctions imposed by Russia are considered. The purpose of this study is to identify the impact of sanctions and countersanctions on the national security of Russia. In this regard, the following tasks were set: to identify the list of sanctions of Western countries imposed against Russia and their impact on the national security of Russia, to identify the list of countersanctions of Russia against Western countries and their impact on the national security of Russia, to identify further actions of Russia to ensure the national security of Russia under the conditions of sanction pressure.The study is based on the dialectical, historical and systematic approach, analysis, synthesis and comparison, induction and deduction. The study analyzed Russian and international literature on the topic of sanctions and their impact on national security.Based on the results of the study, the directions of economic development based on the promotion of import substitution, innovation and public-private partnerships with the aim of ensuring the national security of Russia under the conditions of sanction pressure have been proposed. The findings of the study may be of interest to the academic community, studying the impact of sanctions on the national security of the country. The experience of Russia may be of interest to countries subjected to sanction pressure from the United States and its allies.La etapa actual de desarrollo de toda la comunidad mundial, incluida Rusia, estΓ‘ asociada con cosas como "guerras de sanciones", por ejemplo, podemos recordar la introducciΓ³n de sanciones de Estados Unidos contra China, IrΓ‘n, Venezuela y otros paΓses, sanciones europeas, asΓ como varios paΓses. sometido a presiΓ³n de sanciΓ³n. Como parte de este artΓculo, se consideran las sanciones impuestas contra Rusia en relaciΓ³n con la crisis ucraniana en 2014 y las sanciones contrarias impuestas por Rusia. El propΓ³sito de este estudio es determinar el impacto de las sanciones y contra-sanciones en la seguridad nacional de Rusia. En este sentido, se establecieron las siguientes tareas: determinar la lista de sanciones de los paΓses occidentales impuestas contra Rusia, y su impacto en la seguridad nacional de Rusia, determinar la lista de contra-sanciones de Rusia contra los paΓses occidentales y su impacto en la seguridad nacional de Rusia, para determinar acciones adicionales de Rusia para garantizar la seguridad nacional de Rusia bajo condiciones de presiΓ³n de sanciΓ³n. El estudio se basa en un enfoque dialΓ©ctico, histΓ³rico y sistemΓ‘tico, anΓ‘lisis, sΓntesis y comparaciΓ³n, inducciΓ³n y deducciΓ³n. El estudio analizΓ³ la literatura rusa e internacional sobre el tema de las sanciones y su impacto en la seguridad nacional. Sobre la base de los resultados del estudio, se proponen las direcciones del desarrollo econΓ³mico basadas en la promociΓ³n de la sustituciΓ³n de importaciones, la innovaciΓ³n y las asociaciones pΓΊblico-privadas con el objetivo de garantizar la seguridad nacional de Rusia en condiciones de presiΓ³n de sanciΓ³n. Los hallazgos del estudio pueden ser de interΓ©s para la comunidad cientΓfica, al estudiar el impacto de las sanciones en la seguridad nacional del paΓs, la experiencia de Rusia puede ser de interΓ©s para los paΓses sujetos a la presiΓ³n de las sanciones de los Estados Unidos y sus aliados.ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠΉ ΡΡΠ°ΠΏ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π²ΡΠ΅Π³ΠΎ ΠΌΠΈΡΠΎΠ²ΠΎΠ³ΠΎ ΡΠΎΠΎΠ±ΡΠ΅ΡΡΠ²Π°, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ Π ΠΎΡΡΠΈΠΈ, ΡΠ²ΡΠ·Π°Π½ Ρ ΡΠ°ΠΊΠΈΠΌ ΡΠ²Π»Π΅Π½ΠΈΠ΅ΠΌ ΠΊΠ°ΠΊ Β«ΡΠ°Π½ΠΊΡΠΈΠΎΠ½Π½ΡΠ΅ Π²ΠΎΠΉΠ½ΡΒ», Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΏΡΠΈΠΌΠ΅ΡΠ° ΠΌΠΎΠΆΠ½ΠΎ Π²ΡΠΏΠΎΠΌΠ½ΠΈΡΡ Π²Π²Π΅Π΄Π΅Π½ΠΈΠ΅ ΡΠ°Π½ΠΊΡΠΈΠΈ Π‘Π¨Π ΠΏΡΠΎΡΠΈΠ² ΠΠΈΡΠ°Ρ, ΠΡΠ°Π½Π°, ΠΠ΅Π½Π΅ΡΡΡΠ»Ρ ΠΈ Π΄ΡΡΠ³ΠΈΡ
ΡΡΡΠ°Π½, Π΅Π²ΡΠΎΠΏΠ΅ΠΉΡΠΊΠΈΠ΅ ΡΠ°Π½ΠΊΡΠΈΠΈ, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ ΠΊΠΎΠ½ΡΡΡΠ°Π½ΠΊΡΠΈΠΈ ΡΡΡΠ°Π½, ΠΏΠΎΠ΄Π²Π΅ΡΠ³ΡΠΈΡ
ΡΡ ΡΠ°Π½ΠΊΡΠΈΠΎΠ½Π½ΠΎΠΌΡ Π΄Π°Π²Π»Π΅Π½ΠΈΡ.Π ΡΠ°ΠΌΠΊΠ°Ρ
Π΄Π°Π½Π½ΠΎΠΉ ΡΡΠ°ΡΡΠΈ ΡΠ°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΡΠ°Π½ΠΊΡΠΈΠΈ, Π²Π²Π΅Π΄Π΅Π½Π½ΡΠ΅ ΠΏΡΠΎΡΠΈΠ² Π ΠΎΡΡΠΈΠΈ Π² ΡΠ²ΡΠ·ΠΈ Ρ ΡΠΊΡΠ°ΠΈΠ½ΡΠΊΠΈΠΌ ΠΊΡΠΈΠ·ΠΈΡΠΎΠΌ Π² 2014 Π³ΠΎΠ΄Ρ, ΠΈ ΠΊΠΎΠ½ΡΡΡΠ°Π½ΠΊΡΠΈΠΈ Π²Π²Π΅Π΄Π΅Π½Π½ΡΠ΅ Π ΠΎΡΡΠΈΠ΅ΠΉ. Π¦Π΅Π»ΡΡ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π²Π»ΠΈΡΠ½ΠΈΡ ΡΠ°Π½ΠΊΡΠΈΠΉ ΠΈ ΠΊΠΎΠ½ΡΡΡΠ°Π½ΠΊΡΠΈΠΉ Π½Π° Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΡ Π ΠΎΡΡΠΈΠΈ. Π ΡΡΠΎΠΉ ΡΠ²ΡΠ·ΠΈ Π±ΡΠ»ΠΈ ΠΏΠΎΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ»Π΅Π΄ΡΡΡΠΈΠ΅ Π·Π°Π΄Π°ΡΠΈ: ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΡΡ ΠΏΠ΅ΡΠ΅ΡΠ΅Π½Ρ ΡΠ°Π½ΠΊΡΠΈΠΈ Π·Π°ΠΏΠ°Π΄Π½ΡΡ
ΡΡΡΠ°Π½, Π²Π²Π΅Π΄Π΅Π½Π½ΡΡ
ΠΏΡΠΎΡΠΈΠ² Π ΠΎΡΡΠΈΠΈ, ΠΈ ΠΈΡ
Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΡ Π ΠΎΡΡΠΈΠΈ, ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΡΡ ΠΏΠ΅ΡΠ΅ΡΠ΅Π½Ρ ΠΊΠΎΠ½ΡΡΡΠ°Π½ΠΊΡΠΈΠΉ Π ΠΎΡΡΠΈΠΈ ΠΏΡΠΎΡΠΈΠ² Π·Π°ΠΏΠ°Π΄Π½ΡΡ
ΡΡΡΠ°Π½ ΠΈ ΠΈΡ
Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΡ Π ΠΎΡΡΠΈΠΈ, ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΡΡ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅Π΅ Π΄Π΅ΠΉΡΡΠ²ΠΈΡ Π ΠΎΡΡΠΈΠΈ ΠΏΠΎ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΠΈ Π ΠΎΡΡΠΈΠΈ Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΡΠ°Π½ΠΊΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π΄Π°Π²Π»Π΅Π½ΠΈΡ.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΎ Π½Π° Π΄ΠΈΠ°Π»Π΅ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠΌ, ΠΈΡΡΠΎΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈ ΡΠΈΡΡΠ΅ΠΌΠ½ΠΎΠΌ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Π΅, Π°Π½Π°Π»ΠΈΠ·Π΅, ΡΠΈΠ½ΡΠ΅Π·Π΅ ΠΈ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ, ΠΈΠ½Π΄ΡΠΊΡΠΈΠΈ ΠΈ Π΄Π΅Π΄ΡΠΊΡΠΈΠΈ. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π° ΡΠΎΡΡΠΈΠΉΡΠΊΠ°Ρ ΠΈ ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½Π°Ρ Π»ΠΈΡΠ΅ΡΠ°ΡΡΡΠ° Π½Π° ΡΠ΅ΠΌΡ ΡΠ°Π½ΠΊΡΠΈΠΉ ΠΈ ΠΈΡ
Π²Π»ΠΈΡΠ½ΠΈΡ Π½Π° Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΡ.ΠΠΎ ΠΈΡΠΎΠ³Π°ΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ, ΠΎΡΠ½ΠΎΠ²Π°Π½Π½ΡΠ΅ Π½Π° ΡΡΠΈΠΌΡΠ»ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΈΠΌΠΏΠΎΡΡΠΎΠ·Π°ΠΌΠ΅ΡΠ΅Π½ΠΈΡ, ΠΈΠ½Π½ΠΎΠ²Π°ΡΠΈΠΉ ΠΈ Π³ΠΎΡΡΠ΄Π°ΡΡΡΠ²Π΅Π½Π½ΠΎ-ΡΠ°ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠ°ΡΡΠ½Π΅ΡΡΡΠ²Π° Ρ ΡΠ΅Π»ΡΡ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΠΈ Π ΠΎΡΡΠΈΠΈ Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΡΠ°Π½ΠΊΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π΄Π°Π²Π»Π΅Π½ΠΈΡ. ΠΡΠ²ΠΎΠ΄Ρ, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ Π² Ρ
ΠΎΠ΄Π΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ, ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠ½Ρ Π½Π°ΡΡΠ½ΠΎΠΌΡ ΡΠΎΠΎΠ±ΡΠ΅ΡΡΠ²Ρ, ΠΈΠ·ΡΡΠ°ΡΡΠΈΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΡΠ°Π½ΠΊΡΠΈΠΉ Π½Π° Π½Π°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ Π±Π΅Π·ΠΎΠΏΠ°ΡΠ½ΠΎΡΡΡ ΡΡΡΠ°Π½Ρ, ΠΎΠΏΡΡ Π ΠΎΡΡΠΈΠΈ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΠΈΠ½ΡΠ΅ΡΠ΅ΡΠ΅Π½ ΡΡΡΠ°Π½Π°ΠΌ, ΠΏΠΎΠ΄Π²Π΅ΡΠ³ΡΠΈΠΌΡΡ ΡΠ°Π½ΠΊΡΠΈΠΎΠ½Π½ΠΎΠΌΡ Π΄Π°Π²Π»Π΅Π½ΠΈΡ Π‘Π¨Π ΠΈ ΠΈΡ
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