280 research outputs found
Spatial effects of Fano resonance in local tunneling conductivity in vicinity of impurity on semiconductor surface
We present the results of local tunneling conductivity spatial distribution
detailed theoretical investigations in vicinity of impurity atom for a wide
range of applied bias voltage. We observed Fano resonance in tunneling
conductivity resulting from interference between resonant tunneling channel
through impurity energy level and direct tunneling channel between the
tunneling contact leads. We have found that interference between tunneling
channels strongly modifies form of tunneling conductivity measured by the
scanning tunneling microscopy/spectroscopy (STM/STS) depending on the distance
value from the impurity.Comment: 4 pages, 3 figure
Spatial distribution of local density of states in vicinity of impurity on semiconductor surface
We present the results of detailed theoretical investigations of changes in
local density of total electronic surface states in 2D anisotropic atomic
semiconductor lattice in vicinity of impurity atom for a wide range of applied
bias voltage. We have found that taking into account changes in density of
continuous spectrum states leads to the formation of a downfall at the
particular value of applied voltage when we are interested in the density of
states above the impurity atom or even to a series of downfalls for the fixed
value of the distance from the impurity. The behaviour of local density of
states with increasing of the distance from impurity along the chain differs
from behaviour in the direction perpendicular to the chain.Comment: 6 pages, 5 figure
Correlation induced switching of local spatial charge distribution in two-level system
We present theoretical investigation of spatial charge distribution in the
two-level system with strong Coulomb correlations by means of Heisenberg
equations analysis for localized states total electron filling numbers taking
into account pair correlations of local electron density. It was found that
tunneling current through nanometer scale structure with strongly coupled
localized states causes Coulomb correlations induced spatial redistribution of
localized charges. Conditions for inverse occupation of two-level system in
particular range of applied bias caused by Coulomb correlations have been
revealed. We also discuss possibility of charge manipulation in the proposed
system.Comment: 6 pages, 4 figures Submitted to JETP Letter
Scanning tunneling microscopy and spectroscopy at low temperatures of the (110) surface of Te doped GaAs single crystals
We have performed voltage dependent imaging and spatially resolved
spectroscopy on the (110) surface of Te doped GaAs single crystals with a low
temperature scanning tunneling microscope (STM). A large fraction of the
observed defects are identified as Te dopant atoms which can be observed down
to the fifth subsurface layer. For negative sample voltages, the dopant atoms
are surrounded by Friedel charge density oscillations. Spatially resolved
spectroscopy above the dopant atoms and above defect free areas of the GaAs
(110) surface reveals the presence of conductance peaks inside the
semiconductor band gap. The appearance of the peaks can be linked to charges
residing on states which are localized within the tunnel junction area. We show
that these localized states can be present on the doped GaAs surface as well as
at the STM tip apex.Comment: 8 pages, 8 figures, accepted for publication in PR
Basic principles of postgrowth annealing of CdTe:Cl ingot to obtain semi-insulating crystals
The process of annealing of a CdTe:Cl ingot during its cooling after growth
was studied. The annealing was performed in two stages: a high-temperature
stage, with an approximate equality of chlorine and cadmium vacancy
concentrations established at the thermodynamic equilibrium between the crystal
and vapors of volatile components, and a low-temperature stage, with charged
defects interacting to form neutral associations. The chlorine concentrations
necessary to obtain semi-insulating crystals were determined for various ingot
cooling rates in the high temperature stage. The dependence of the chlorine
concentration [Cl+Te] in the ingot on the temperature of annealing in the
high-temperature stage was found. The carrier lifetimes and drift mobilities
were obtained in relation to the temperature and cadmium vapor pressure in the
postgrowth annealing of the ingot.Comment: 6 pages, 6 figure
Decay and Continuity of Boltzmann Equation in Bounded Domains
Boundaries occur naturally in kinetic equations and boundary effects are
crucial for dynamics of dilute gases governed by the Boltzmann equation. We
develop a mathematical theory to study the time decay and continuity of
Boltzmann solutions for four basic types of boundary conditions: inflow,
bounce-back reflection, specular reflection, and diffuse reflection. We
establish exponential decay in norm for hard potentials for
general classes of smooth domains near an absolute Maxwellian. Moreover, in
convex domains, we also establish continuity for these Boltzmann solutions away
from the grazing set of the velocity at the boundary. Our contribution is based
on a new decay theory and its interplay with delicate
decay analysis for the linearized Boltzmann equation, in the presence of many
repeated interactions with the boundary.Comment: 89 pages
Coulomb correlations effects on localized charge relaxation in the coupled quantum dots
We analyzed localized charge time evolution in the system of two interacting
quantum dots (QD) (artificial molecule) coupled with the continuous spectrum
states. We demonstrated that Coulomb interaction modifies relaxation rates and
is responsible for non-monotonic time evolution of the localized charge. We
suggested new mechanism of this non-monotonic charge time evolution connected
with charge redistribution between different relaxation channels in each QD.Comment: 10 pages, 10 figure
Charge and spin configurations in the coupled quantum dots with Coulomb correlations induced by tunneling current
We investigated the peculiarities of non-equilibrium charge states and spin
configurations in the system of two strongly coupled quantum dots (QDs) weakly
connected to the electrodes in the presence of Coulomb correlations. We
analyzed the modification of non-equilibrium charge states and different spin
configurations of the system in a wide range of applied bias voltage and
revealed well pronounced ranges of system parameters where negative tunneling
conductivity appears due to the Coulomb correlations.Comment: 10 pages, 6 figure
Sun and shade leaf variability in Liquidambar chinensis and Liquidambar formosana (Altingiaceae): Implications for palaeobotany
Β© 2018 The Linnean Society of London. Many factors influence leaf anatomy and morphology in the crown of a tree, particularly those resulting from microclimatic differences between the periphery and the interior of the crown. These influences can be so strong that single species can produce different leaf forms in which shade and sun leaves exhibit consistently distinctive morphological and epidermal character sets. Here we show, using Liquidambar as a model system, that the principal morphological characters for distinguishing shade and sun leaves in two modern Liquidambar spp. with different lamina types (entire in L. chinensis and lobate in L. formosana) are the leaf lamina length to width ratio, the degree of development of venation networks, tooth size and tooth shape. The main epidermal characters are ordinary cell size and anticlinal wall outlines. Many fossils, however, are only preserved as impressions and morphological characters alone have been used to distinguish shade and sun leaf morphotypes. To evaluate the utility of our approach, populations of fossil Liquidambar leaves from the Eocene of southern China, preserved only as impressions, were categorized into sun and shade morphotypes. Recognition that sun and shade leaf morphological diversity exists in fossil populations will enable palaeobotanists to identify more reliably foliar polymorphisms that would otherwise be used to describe, incorrectly, different species
Π‘ΠΎΠ·Π΄Π°Π½ΠΈΠ΅ Π½ΠΎΠ²ΡΡ ΡΠΎΡΠΌ ΡΠΎΠΌΠ°ΡΠ° Ρ Π³Π΅Π½Π°ΠΌΠΈ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ ΠΊ Π³ΡΠΈΠ±Π½ΡΠΌ Π±ΠΎΠ»Π΅Π·Π½ΡΠΌ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΌΠ°ΡΠΊΠ΅ΡΠ½ΠΎΠΉ ΡΠ΅Π»Π΅ΠΊΡΠΈΠΈ
Relevance. The presented studies are aimed at obtaining new forms of tomato with a complex of genes for resistance to fungal diseases in combination with a standard type of bush and dark coloring of fruits based on marker-mediated selection.Methodology. The biological objects of the study are varieties and hybrid forms of tomato from the collection of the Michurinsky SAU. Molecular genetic analysis was performed using the following methods. DNA extraction was carried out from young leaves using a kit for isolation of NC Sample NC manufactured by Agrodiagnostika LLC according to the manufacturer's protocol. Fermentas production kits were used for PCR. Identification of the cladosporosis resistance gene was Cf-19 performed using the DNA marker R7. The presence of a fusarious wilting resistance gene was determined by a I-2/5 marker. The amplification results were visualized by agarose gel electrophoresis.Results. During the research, a collection of varieties and hybrid forms of tomato of the Michurinsky GAU was analyzed in order to identify genes for resistance to cladosporiosis Cf-19 and fusarium wilt I-2. A total of 52 genotypes were analyzed. It was found that most samples (41 samples) are characterized by a heterozygous state of the Cf-19 gene. All indeterminant and semi-determinant forms had both alleles. Of the 23 determinant forms presented in the collection, 10 had only one allele corresponding to recessive homozygote. Among all analyzed tomato genotypes, no dominant homozygous forms were noted. The study of the collection revealed several alleles of the I-2 gene. In total, four fragments corresponding to various alleles were amplified. A total of 50 resistant genotypes have been identified in the collection. Two alleys of the I-2 gene (633/693 bp) were identified in 42 tomato samples. Four varieties are homozygous in one allele (633 bp), which determines resistance. Three varieties have a second resistance allele (566 bp). One genotype has only an allele defining susceptibility (693 bp). On the basis of molecular analysis, as well as an assessment of the type of bush and fetal color, initial forms were selected with subsequent hybridization. 67 hybrid tomato plants were obtained. Evaluation of the presence of resistance genes showed that most of the resulting hybrids are resistant to cladosporiosis and fuzariosis. This is due to the presence of dominant alleles of Cf-19 and I-2 genes in a heterozygous state. Among the resulting hybrids, plants with a bark type of bush were identified. A total of 13 such plants were obtained.Conclusion. Thus, the work carried out allowed to obtain hybrid forms of tomato combine the signs of resistance to two pathogens of fungal diseases and the stem type of the bush. These forms are planned to be used in further selection work.Π¦Π΅Π»Ρ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½Ρ Π½Π° ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ Π½ΠΎΠ²ΡΡ
ΡΠΎΡΠΌ ΡΠΎΠΌΠ°ΡΠ° Ρ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠΎΠΌ Π³Π΅Π½ΠΎΠ² ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ ΠΊ Π³ΡΠΈΠ±Π½ΡΠΌ Π±ΠΎΠ»Π΅Π·Π½ΡΠΌ Π² ΡΠΎΡΠ΅ΡΠ°Π½ΠΈΠΈ ΡΠΎ ΡΡΠ°ΠΌΠ±ΠΎΠ²ΡΠΌ ΡΠΈΠΏΠΎΠΌ ΠΊΡΡΡΠ° ΠΈ ΡΠ΅ΠΌΠ½ΠΎΠΉ ΠΎΠΊΡΠ°ΡΠΊΠΎΠΉ ΠΏΠ»ΠΎΠ΄ΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΌΠ°ΡΠΊΠ΅Ρ-ΠΎΠΏΠΎΡΡΠ΅Π΄ΠΎΠ²Π°Π½Π½ΠΎΠΉ ΡΠ΅Π»Π΅ΠΊΡΠΈΠΈ.ΠΠ΅ΡΠΎΠ΄Ρ. ΠΠ±ΡΠ΅ΠΊΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ β ΡΠΎΡΡΠ° ΠΈ Π³ΠΈΠ±ΡΠΈΠ΄Π½ΡΠ΅ ΡΠΎΡΠΌΡ ΡΠΎΠΌΠ°ΡΠ° ΠΈΠ· ΠΊΠΎΠ»Π»Π΅ΠΊΡΠΈΠΈ ΠΠΈΡΡΡΠΈΠ½ΡΠΊΠΎΠ³ΠΎ ΠΠΠ£. ΠΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΠΎ-Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠ»Π΅Π΄ΡΡΡΠΈΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ². ΠΠΊΡΡΡΠ°Π³ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΠΠ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ ΠΈΠ· ΠΌΠΎΠ»ΠΎΠ΄ΡΡ
Π»ΠΈΡΡΡΠ΅Π² Ρ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π½Π°Π±ΠΎΡΠ° Π΄Π»Ρ Π²ΡΠ΄Π΅Π»Π΅Π½ΠΈΡ ΠΠ Β«ΠΡΠΎΠ±Π° ΠΠΒ» ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π° ΠΠΠ Β«ΠΠ³ΡΠΎΠ΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ°Β» ΡΠΎΠ³Π»Π°ΡΠ½ΠΎ ΠΏΡΠΎΡΠΎΠΊΠΎΠ»Ρ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΡΠ΅Π»Ρ. ΠΠ»Ρ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΠΠ¦Π ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ Π½Π°Π±ΠΎΡΡ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π° ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠΈ Fermentas. ΠΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΡ Π³Π΅Π½Π° ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ ΠΊ ΠΊΠ»Π°Π΄ΠΎΡΠΏΠΎΡΠΈΠ·Ρ Cf-19 ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΠΠ-ΠΌΠ°ΡΠΊΠ΅ΡΠ° Π 7. ΠΠ°Π»ΠΈΡΠΈΠ΅ Π³Π΅Π½Π° ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ ΠΊ ΡΡΠ·Π°ΡΠΈΠΎΠ·Π½ΠΎΠΌΡ ΡΠ²ΡΠ΄Π°Π½ΠΈΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΌΠ°ΡΠΊΠ΅ΡΠ° I-2/5. ΠΠΈΠ·ΡΠ°Π»ΠΈΠ·Π°ΡΠΈΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² Π°ΠΌΠΏΠ»ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΠΎΡΡΡΠ΅ΡΡΠ²Π»ΡΠ»ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠ»Π΅ΠΊΡΡΠΎΡΠΎΡΠ΅Π·Π° Π² Π°Π³Π°ΡΠΎΠ·Π½ΠΎΠΌ Π³Π΅Π»Π΅.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΡΠΈ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π±ΡΠ»Π° ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π° ΠΊΠΎΠ»Π»Π΅ΠΊΡΠΈΡ ΡΠΎΡΡΠΎΠ² ΠΈ Π³ΠΈΠ±ΡΠΈΠ΄Π½ΡΡ
ΡΠΎΡΠΌ ΡΠΎΠΌΠ°ΡΠ° ΠΠΈΡΡΡΠΈΠ½ΡΠΊΠΎΠ³ΠΎ ΠΠΠ£ Ρ ΡΠ΅Π»ΡΡ ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ Π³Π΅Π½ΠΎΠ² ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ ΠΊ ΠΊΠ»Π°Π΄ΠΎΡΠΏΠΎΡΠΈΠΎΠ·Ρ Cf-19 ΠΈ ΡΡΠ·Π°ΡΠΈΠΎΠ·Π½ΠΎΠΌΡ ΡΠ²ΡΠ΄Π°Π½ΠΈΡ I-2. ΠΡΠ΅Π³ΠΎ ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½ΠΎ 52 Π³Π΅Π½ΠΎΡΠΈΠΏΠ°. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π΄Π»Ρ Π±ΠΎΠ»ΡΡΠΈΠ½ΡΡΠ²Π° ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² (41 ΠΎΠ±ΡΠ°Π·Π΅Ρ) Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ½ΠΎ Π³Π΅ΡΠ΅ΡΠΎΠ·ΠΈΠ³ΠΎΡΠ½ΠΎΠ΅ ΡΠΎΡΡΠΎΡΠ½ΠΈΠ΅ Π³Π΅Π½Π° Cf-19. ΠΡΠ΅ ΠΈΠ½Π΄Π΅ΡΠ΅ΡΠΌΠΈΠ½Π°Π½ΡΠ½ΡΠ΅ ΠΈ ΠΏΠΎΠ»ΡΠ΄Π΅ΡΠ΅ΡΠΌΠΈΠ½Π°Π½ΡΠ½ΡΠ΅ ΡΠΎΡΠΌΡ ΠΈΠΌΠ΅Π»ΠΈ ΠΎΠ±Π° Π°Π»Π»Π΅Π»Ρ. ΠΠ· 23 ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΡΡ
Π² ΠΊΠΎΠ»Π»Π΅ΠΊΡΠΈΠΈ Π΄Π΅ΡΠ΅ΡΠΌΠΈΠ½Π°Π½ΡΠ½ΡΡ
ΡΠΎΡΠΌ Ρ 10 ΠΎΡΠΌΠ΅ΡΠ΅Π½ ΡΠΎΠ»ΡΠΊΠΎ ΠΎΠ΄ΠΈΠ½ Π°Π»Π»Π΅Π»Ρ, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠΉ ΡΠ΅ΡΠ΅ΡΡΠΈΠ²Π½ΠΎΠΉ Π³ΠΎΠΌΠΎΠ·ΠΈΠ³ΠΎΡΠ΅. Π‘ΡΠ΅Π΄ΠΈ Π²ΡΠ΅Ρ
Π°Π½Π°Π»ΠΈΠ·ΠΈΡΡΠ΅ΠΌΡΡ
Π³Π΅Π½ΠΎΡΠΈΠΏΠΎΠ² ΡΠΎΠΌΠ°ΡΠ° Π½Π΅ ΠΎΡΠΌΠ΅ΡΠ΅Π½ΠΎ Π΄ΠΎΠΌΠΈΠ½Π°Π½ΡΠ½ΡΡ
Π³ΠΎΠΌΠΎΠ·ΠΈΠ³ΠΎΡΠ½ΡΡ
ΡΠΎΡΠΌ. ΠΠ·ΡΡΠ΅Π½ΠΈΠ΅ ΠΊΠΎΠ»Π»Π΅ΠΊΡΠΈΠΈ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ»ΠΎ Π²ΡΡΠ²ΠΈΡΡ Π½Π΅ΡΠΊΠΎΠ»ΡΠΊΠΈΡ
Π°Π»Π»Π΅Π»Π΅ΠΉ Π³Π΅Π½Π° I-2. ΠΡΠ΅Π³ΠΎ Π°ΠΌΠΏΠ»ΠΈΡΠΈΡΠΈΡΠΎΠ²Π°Π½ΠΎ ΡΠ΅ΡΡΡΠ΅ ΡΡΠ°Π³ΠΌΠ΅Π½ΡΠ°, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΡ
ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌ Π°Π»Π»Π΅Π»ΡΠΌ. ΠΡΠ΅Π³ΠΎ ΡΡΡΠΎΠΉΡΠΈΠ²ΡΡ
Π³Π΅Π½ΠΎΡΠΈΠΏΠΎΠ² Π² ΠΊΠΎΠ»Π»Π΅ΠΊΡΠΈΠΈ Π²ΡΠ΄Π΅Π»Π΅Π½ΠΎ 50. Π£ 42 ΠΎΠ±ΡΠ°Π·ΡΠΎΠ² ΡΠΎΠΌΠ°ΡΠ° ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΡΠΈΡΠΎΠ²Π°Π½Ρ Π΄Π²Π° Π°Π»Π»Π΅Ρ Π³Π΅Π½Π° I-2 (633/693 ΠΏ.Π½). Π§Π΅ΡΡΡΠ΅ ΡΠΎΡΡΠ° Π³ΠΎΠΌΠΎΠ·ΠΈΠ³ΠΎΡΠ½Ρ ΠΏΠΎ ΠΎΠ΄Π½ΠΎΠΌΡ Π°Π»Π»Π΅Π»Ρ (633 ΠΏ.Π½.), ΠΎΠ±ΡΡΠ»Π°Π²Π»ΠΈΠ²Π°ΡΡΠ΅ΠΌΡ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΡ. Π’ΡΠΈ ΡΠΎΡΡΠ° ΠΈΠΌΠ΅ΡΡ Π²ΡΠΎΡΠΎΠΉ Π°Π»Π»Π΅Π»Ρ (566 ΠΏ.Π½.) ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ. ΠΠ΄ΠΈΠ½ Π³Π΅Π½ΠΎΡΠΈΠΏ ΠΈΠΌΠ΅Π΅Ρ ΡΠΎΠ»ΡΠΊΠΎ Π°Π»Π»Π΅Π»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΠΈΠΉ Π²ΠΎΡΠΏΡΠΈΠΈΠΌΡΠΈΠ²ΠΎΡΡΡ (693 ΠΏ.Π½.).ΠΠ° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π°, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΎΡΠ΅Π½ΠΊΠΈ ΡΠΈΠΏΠ° ΠΊΡΡΡΠ° ΠΈ ΠΎΠΊΡΠ°ΡΠΊΠΈ ΠΏΠ»ΠΎΠ΄Π° Π±ΡΠ» ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ ΠΎΡΠ±ΠΎΡ ΠΈΡΡ
ΠΎΠ΄Π½ΡΡ
ΡΠΎΡΠΌ Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΉ Π³ΠΈΠ±ΡΠΈΠ΄ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ. ΠΠΎΠ»ΡΡΠ΅Π½ΠΎ 67 Π³ΠΈΠ±ΡΠΈΠ΄Π½ΡΡ
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