72 research outputs found

    Microkelvin thermometry with Bose-Einstein condensates of magnons and applications to studies of the AB interface in superfluid 3^3He

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    Coherent precession of trapped Bose-Einstein condensates of magnons is a sensitive probe for magnetic relaxation processes in superfluid 3He-B down to the lowest achievable temperatures. We use the dependence of the relaxation rate on the density of thermal quasiparticles to implement thermometry in 3He-B at temperatures below 300 ΞΌ\muK. Unlike popular vibrating wire or quartz tuning fork based thermometers, magnon condensates allow for contactless temperature measurement and make possible an independent in situ determination of the residual zero-temperature relaxation provided by the radiation damping. We use this magnon-condensate-based thermometry to study the thermal impedance of the interface between A and B phases of superfluid 3He. The magnon condensate is also a sensitive probe of the orbital order-parameter texture. This has allowed us to observe for the first time the non-thermal signature of the annihilation of two AB interfaces.Comment: 26 pages, 7 figures, manuscript prepared for EU Microkelvin Collaboration Workshop 2013. Accepted for publication in Journal of Low Temperature Physic

    Quasiparticle transport in a two-dimensional boundary superfluid

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    The B phase of superfluid 3He can be cooled into the "pure" superfluid regime, characterised by negligible thermal quasiparticle density. Here, the bulk superfluid is bounded by a two-dimensional quantum well at the boundaries of the container, where creating quasiparticles requires much less energy. In this Article, we carry out experiments where we create a non-equilibrium state within the quantum well and show that the induced quasiparticle currents flow diffusively in the two-dimensional system. We conclude that the bulk of superfluid 3He is wrapped by an independent two-dimensional superfluid that interacts with mechanical probes instead of the bulk superfluid, only providing access to the bulk superfluid if given a sudden burst of energy. That is, superfluid 3He at the lowest temperatures and applied energies is thermo-mechanically two dimensional. Our work opens this two-dimensional quantum condensate and the interface it forms between the observer and the bulk superfluid for exploration, and provides the possibility of creating two-dimensional condensates of arbitrary topology.Comment: 11 pages, 9 figure

    Apoptosis in the liver of male <em>db/db</em> mice during the development of obesity and type 2 diabetes

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    Obesity and diabetes mellitus are known to lead to the development of metabolic syndrome and non-alcoholic fatty liver disease (NAFLD). The mechanisms of programmed cell death are actively involved in maintaining cellular homeostasis along development of NAFLD. Proteins of the BCL-2 family are key regulators of physiological and pathological apoptosis. Homozygous males of BKS.Cg-Dock7mLeprdb/+/+/J mice (db/db mice) are characterized by progressive obesity and the development of type 2 diabetes mellitus (DM2) with severe hyperglycemia at 4–8 weeks and organ lesions at 8–10 weeks of age. The aim of this research was to study the expression of molecular cell regulators of apoptosis in liver cells of db/db mice males at different stages of obesity and diabetes development (at the age of 10 and 18 weeks). Immunohistochemical analysis (using the indirect avidin-biotin peroxidase method) and morphometric evaluation of the expression of the antiapoptotic protein Bcl-2 and the proapoptotic protein Bad in liver cells of studied animals at different stages of obesity and DM2 were carried out. An excess of the value of the Bcl-2 protein staining area over the Bad protein staining area was revealed in the liver of 10-week-old animals. The Bcl-2/Bad expression area ratio in 10-week-old animals was twice as high as in 18-week-old animals, which indicates the presence of conditions for blocking apoptosis in the liver of younger db/db mice. At the 18th week of life, db/db mice displayed an almost threefold increase in the expression area of the Bad protein against the background of an unchanged expression of the Bcl-2 protein. The decrease in the Bcl-2/Bad staining area ratio in 18-week-old animals was due to the increase in the Bad expression area, which indicates the absence of antiapoptotic cell protection and creates conditions for activation of the mitochondrial pathway of apoptosis in the liver of male db/db mice with pronounced signs of obesity and DM2

    ΠžΠΏΡ‚ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΡ Ρ„ΠΎΡ€ΠΌΡ‹ сигналов с ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠΉ Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Π½ΠΎΠΉ модуляциСй с использованиСм критСрия Π·Π°Π΄Π°Π½Π½ΠΎΠΉ скорости спада уровня внСполосных ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠΉ

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    Introduction. The growth in the volume of information transmitted through communication channels leads to their significant congestion. Almost all methods conventionally used to increase the data transfer rate in given frequency bands have been exhausted. In this regard, it is of interest to use new approaches aimed at improving the spectral efficiency of radio engineering and telecommunication systems by applying optimal signals that make it possible to use the bandwidth reserves of transmission channels given by Shannon's theory.Aim. Improvement of the spectral efficiency of digital messaging systems by using signals with a compact spectrum and increased volume of the channel alphabet at the same time as minimizing energy losses.Materials and methods. When searching for optimal signals, the mathematical apparatus of communication theory and functional analysis, as well as the methods of calculus of variations, were used. The evaluation of bit error rate performance of the obtained optimal signals transmitted in a channel with additive white Gaussian noise was performed in the MatLab environment. Results. It was established that, in a channel with additive white Gaussian noise, optimal signals with a signal constellation size of 64 in the case of quadrature amplitude-phase modulation provide an energy gain of more than 1 dB relative to signals obtained by narrowband filtering under the conditions of uncontrolled intersymbol interference. Optimal signals were shown to provide for an energy gain of 4.9 dB with respect to signals based on narrow-band filtering at a fixed spectral efficiency of 7 (bit/s)/Hz.Conclusion. The paper proposes a method for improving the spectral efficiency of quadrature signals with amplitudephase modulation, based on the use of optimal pulse shapes obtained as a result of solving an optimization problem. The optimization problem was solved according to the criterion of minimizing out-of-band emissions with the constraint on bit error rate performance in case of amplitude-phase modulation. The energy and spectral efficiency of signals with optimal pulse shapes and signals based on narrow-band filtering were compared.Π’Π²Π΅Π΄Π΅Π½ΠΈΠ΅. Рост объСмов ΠΏΠ΅Ρ€Π΅Π΄Π°Π²Π°Π΅ΠΌΠΎΠΉ ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ ΠΏΠΎ ΠΊΠ°Π½Π°Π»Π°ΠΌ связи ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ ΠΈΡ… сущСствСнной пСрСгруТСнности. ΠŸΡ€Π°ΠΊΡ‚ΠΈΡ‡Π΅ΡΠΊΠΈ всС ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΡ‹Π΅ Ρ‚Ρ€Π°Π΄ΠΈΡ†ΠΈΠΎΠ½Π½Ρ‹Π΅ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡ скорости ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡ΠΈ Π΄Π°Π½Π½Ρ‹Ρ… Π² Π·Π°Π΄Π°Π½Π½Ρ‹Ρ… полосах частот исчСрпаны. Π’ этой связи прСдставляСт интСрСс использованиС Π½ΠΎΠ²Ρ‹Ρ… ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ², Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Π½Ρ‹Ρ… Π½Π° ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΠ΅ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ эффСктивности радиотСхничСских ΠΈ Ρ‚Π΅Π»Π΅ΠΊΠΎΠΌΠΌΡƒΠ½ΠΈΠΊΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹Ρ… систСм ΠΏΡƒΡ‚Π΅ΠΌ примСнСния ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… сигналов, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰ΠΈΡ… Π·Π°Π΄Π΅ΠΉΡΡ‚Π²ΠΎΠ²Π°Ρ‚ΡŒ Ρ€Π΅Π·Π΅Ρ€Π²Ρ‹ пропускной способности ΠΊΠ°Π½Π°Π»ΠΎΠ² ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡ΠΈ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Π΄Π°Π΅Ρ‚ тСория Π¨Π΅Π½Π½ΠΎΠ½Π°.ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹. ΠŸΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΠ΅ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ эффСктивности систСм ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡ΠΈ Ρ†ΠΈΡ„Ρ€ΠΎΠ²Ρ‹Ρ… сообщСний ΠΏΡƒΡ‚Π΅ΠΌ примСнСния сигналов с ΠΊΠΎΠΌΠΏΠ°ΠΊΡ‚Π½Ρ‹ΠΌ спСктром ΠΈ увСличСния объСма канального Π°Π»Ρ„Π°Π²ΠΈΡ‚Π° ΠΏΡ€ΠΈ ΠΌΠΈΠ½ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΈ энСргСтичСских ΠΏΠΎΡ‚Π΅Ρ€ΡŒ.ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. ΠŸΡ€ΠΈ поискС ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… сигналов ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅Ρ‚ΡΡ матСматичСский Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚ Ρ‚Π΅ΠΎΡ€ΠΈΠΈ связи ΠΈ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π°, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ Π²Π°Ρ€ΠΈΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ исчислСния. ΠžΡ†Π΅Π½ΠΊΠ° помСхоустойчивости ΠΏΡ€ΠΈΠ΅ΠΌΠ° ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… сигналов ΠΏΡ€ΠΈ ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡Π΅ Π² ΠΊΠ°Π½Π°Π»Π΅ с Π°Π΄Π΄ΠΈΡ‚ΠΈΠ²Π½Ρ‹ΠΌ Π±Π΅Π»Ρ‹ΠΌ гауссовским ΡˆΡƒΠΌΠΎΠΌ Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π° Π² срСдС MatLab.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. УстановлСно, Ρ‡Ρ‚ΠΎ Π² ΠΊΠ°Π½Π°Π»Π΅ с Π°Π΄Π΄ΠΈΡ‚ΠΈΠ²Π½Ρ‹ΠΌ Π±Π΅Π»Ρ‹ΠΌ гауссовским ΡˆΡƒΠΌΠΎΠΌ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ сигналы ΠΏΡ€ΠΈ Ρ€Π°Π·ΠΌΠ΅Ρ€Π΅ сигнального созвСздия 64 Π² случаС ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠΉ Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Π½ΠΎ-Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ модуляции ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‚ энСргСтичСский Π²Ρ‹ΠΈΠ³Ρ€Ρ‹Ρˆ Π±ΠΎΠ»Π΅Π΅ 1 Π΄Π‘ ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ сигналов, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΠΎΠ»ΡƒΡ‡Π°ΡŽΡ‚ΡΡ ΠΏΡƒΡ‚Π΅ΠΌ узкополосной Ρ„ΠΈΠ»ΡŒΡ‚Ρ€Π°Ρ†ΠΈΠΈ Π² условиях Π½Π΅ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΠΈΡ€ΡƒΠ΅ΠΌΠΎΠΉ мСТсимвольной ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠΈ. Показано, Ρ‡Ρ‚ΠΎ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ сигналы ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΠΏΠΎΠ»ΡƒΡ‡ΠΈΡ‚ΡŒ энСргСтичСский Π²Ρ‹ΠΈΠ³Ρ€Ρ‹Ρˆ 4.9 Π΄Π‘ ΠΏΠΎ ΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΡŽ ΠΊ сигналам, построСнным Π½Π° основС узкополосной Ρ„ΠΈΠ»ΡŒΡ‚Ρ€Π°Ρ†ΠΈΠΈ, ΠΏΡ€ΠΈ фиксированной ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ эффСктивности 7 (Π±ΠΈΡ‚/с)/Π“Ρ†.Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΠ΅Ρ‚ΠΎΠ΄ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ эффСктивности ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚ΡƒΡ€Π½Ρ‹Ρ… сигналов с Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Π½ΠΎ-Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ модуляциСй, основанный Π½Π° ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΈ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… Ρ„ΠΎΡ€ΠΌ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠΎΠ², ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… Π² Ρ…ΠΎΠ΄Π΅ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ ΠΎΠΏΡ‚ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ Π·Π°Π΄Π°Ρ‡ΠΈ. ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Π° ΠΏΡ€ΠΎΡ†Π΅Π΄ΡƒΡ€Π° Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ ΠΎΠΏΡ‚ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ Π·Π°Π΄Π°Ρ‡ΠΈ ΠΏΠΎ ΠΊΡ€ΠΈΡ‚Π΅Ρ€ΠΈΡŽ ΠΌΠΈΠ½ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΈ внСполосных ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠΉ ΠΏΡ€ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠΈ ограничСния Π½Π° ΠΏΠΎΠΌΠ΅Ρ…ΠΎΡƒΡΡ‚ΠΎΠΉΡ‡ΠΈΠ²ΠΎΡΡ‚ΡŒ ΠΏΡ€ΠΈΠ΅ΠΌΠ° Π² случаС Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Π½ΠΎ-Ρ„Π°Π·ΠΎΠ²ΠΎΠΉ модуляции. Π’Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΎ сравнСниС энСргСтичСской ΠΈ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ эффСктивности, обСспСчиваСмой сигналами с ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ Ρ„ΠΎΡ€ΠΌΠ°ΠΌΠΈ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠΎΠ² ΠΈ сигналами, построСнными Π½Π° основС узкополосной Ρ„ΠΈΠ»ΡŒΡ‚Ρ€Π°Ρ†ΠΈΠΈ

    The expression of apoptosis-regulating proteins Bcl-2 and Bad in liver cells of C57Bl/6 mice under light-induced functional pinealectomy and after correction with melatonin

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    The presence of humans and animals under long-term continuous lighting leads to a suppression of melatonin synthesis, that is, to light-induced functional pinealectomy (LIFP), and the development of desynchronosis. To create LIFP, C57Bl/6 mice were kept under 24-hour lighting (24hL) for 14 days. The animals in the control group were kept under standard lighting conditions. In the next series of experiments, mice with LIFP received daily intragastrically either melatonin (1 mg/kg body weight in 200 ΞΌl of distilled water) or 200 ΞΌl of water as a placebo. The comparison group consisted of intact animals that received placebo under standard lighting conditions. Immunohistochemical analysis (using an indirect avidin-biotin peroxidase method) revealed the expression of the antiapoptotic protein Bcl-2 and the proapoptotic protein Bad in sinusoid liver cells (a heterogeneous population consisting of the endotheliocytes, Kupffer cells, Ito cells, and Pit cells) and in individual hepatocytes. The Bad expression area in the liver of LIFP mice increased 4 times against a background of the unchanged Bcl-2 expression area. Changes in the brightness (a parameter inversely proportional to the marker concentration) of Bad and Bcl-2 areas did not reach significance. Our results indicate a weakening of the antiapoptotic protection of liver cells of LIFP animals, which creates conditions for activation of the β€œmitochondrial branch” of apoptosis. Melatonin treatment of LIFP mice resulted in a 3.3-fold increase in Bcl-2 expression area and a 2.7 % decrease in Bcl-2 region brightness compared with the experimental untreated group. Bad protein parameters were unreliable. Thus, melatonin treatment of animals cancels the effect of LIFP, restoring the Bcl-2 expression area and increasing this protein concentration, which indicates an increase in antiapoptotic protection and creates conditions for blocking the development of the β€œmitochondrial branch” of apoptosis in liver cells

    ΠšΠΎΠ³Π΅Ρ€Π΅Π½Ρ‚Π½Ρ‹ΠΉ ΠΏΡ€ΠΈΠ΅ΠΌ Π½Π΅ΠΎΡ€Ρ‚ΠΎΠ³ΠΎΠ½Π°Π»ΡŒΠ½Ρ‹Ρ… ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎ-эффСктивных многочастотных сигналов ΠΏΡ€ΠΈ использовании Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° с ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ связью ΠΏΠΎ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡŽ

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    Introduction. Spectrally efficient frequency division multiplexing (SEFDM) is a promising technology for improving spectral efficiency. Since SEFDM signals transmitted on subcarriers are not orthogonal, interchannel interference occurs due to the mutual influence of signals transmitted on adjacent subcarriers. Algorithms for receiving SEFDM signals can be distinguished into element-by-element coherent detection and maximum-likelihood sequence estimation (MLSE). The former method, although being simpler, is characterized by a low bit error rate performance. The latter method, although providing for a higher energy efficiency, is more complicated and does not allow high absolute message rates.Aim. To consider a trade-off solution to the problem of coherent detection of SEFDM signals under the condition of significant interchannel interference, namely, the use of an iterative algorithm of element-by-element processing with decision feedback at each subcarrier frequency.Materials and methods. Analytical expressions for the operation of a demodulator solver were derived. A simulation model for transmission of SEFDM signals was built in the MatLab environment, including element-by-element detection with decision feedback.Results. The simulation results confirmed the efficiency of the proposed algorithm. For error probabilities p =102…103, the energy gains reach values from 0.2 to 7.5 dB for different values of the non-orthogonal subcarrier spacing. At the same time, the efficiency of the detection algorithm with decision feedback turns out to be significantly lower than that when using the detection algorithm MLSE.Conclusion. The proposed detection algorithm can be used in future generations of mobile communications, which require high transmission rates. By reducing the computational complexity of the algorithm, it is possible to provide for a lower power consumption of mobile devices.Π’Π²Π΅Π΄Π΅Π½ΠΈΠ΅. Π’ настоящСС врСмя ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎ-эффСктивноС частотноС ΠΌΡƒΠ»ΡŒΡ‚ΠΈΠΏΠ»Π΅ΠΊΡΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ (Spectrally efficient frequency division multiplexing – SEFDM) являСтся ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±Π΅Ρ‰Π°ΡŽΡ‰Π΅ΠΉ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠ΅ΠΉ, ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΠΎΠΉ для ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡ ΡΠΏΠ΅ΠΊΡ‚Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ эффСктивности ΠΈ скорости ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡ΠΈ ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ. Алгоритмы ΠΏΡ€ΠΈΠ΅ΠΌΠ° SEFDMсигналов ΠΌΠΎΠΆΠ½ΠΎ Ρ€Π°Π·Π΄Π΅Π»ΠΈΡ‚ΡŒ Π½Π° 2 класса: поэлСмСнтный ΠΊΠΎΠ³Π΅Ρ€Π΅Π½Ρ‚Π½Ρ‹ΠΉ ΠΏΡ€ΠΈΠ΅ΠΌ ΠΈ ΠΏΡ€ΠΈΠ΅ΠΌ всСй ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ посылки. ΠŸΠ΅Ρ€Π²Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ Π±ΠΎΠ»Π΅Π΅ прост, Π½ΠΎ ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ‚ Π½ΠΈΠ·ΠΊΠΎΠΉ ΠΏΠΎΠΌΠ΅Ρ…ΠΎΡƒΡΡ‚ΠΎΠΉΡ‡ΠΈΠ²ΠΎΡΡ‚ΡŒΡŽ. ΠŸΡ€ΠΈ ΠΏΡ€ΠΈΠ΅ΠΌΠ΅ всСй посылки Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΈΠ΅ высокой энСргСтичСской эффСктивности, Π½ΠΎ рСализация Ρ‚Π°ΠΊΠΎΠ³ΠΎ ΠΏΡ€ΠΈΠ΅ΠΌΠ° ΠΎΡ‡Π΅Π½ΡŒ слоТна ΠΈ Π½Π΅ позволяСт Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Ρ‚ΡŒ высокиС Π°Π±ΡΠΎΠ»ΡŽΡ‚Π½Ρ‹Π΅ скорости ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡ΠΈ сообщСний.ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹. РассмотрСниС компромиссного Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ Π·Π°Π΄Π°Ρ‡ΠΈ ΠΊΠΎΠ³Π΅Ρ€Π΅Π½Ρ‚Π½ΠΎΠ³ΠΎ ΠΏΡ€ΠΈΠ΅ΠΌΠ° SEFDM-сигналов Π² условиях сущСствСнной мСТканальной ΠΈΠ½Ρ‚Π΅Ρ€Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠΈ, Π° ΠΈΠΌΠ΅Π½Π½ΠΎ использованиС Π½Π° ΠΊΠ°ΠΆΠ΄ΠΎΠΉ поднСсущСй частотС ΠΈΡ‚Π΅Ρ€Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° поэлСмСнтной ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ с ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ связью ΠΏΠΎ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡŽ.ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. ОписаниС Ρ€Π°Π±ΠΎΡ‚Ρ‹ дСмодулятора Ρ€Π΅ΡˆΠ°ΡŽΡ‰Π΅Π³ΠΎ устройства Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΎ аналитичСским ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ. Π˜ΠΌΠΈΡ‚Π°Ρ†ΠΈΠΎΠ½Π½Π°Ρ модСль ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡ΠΈ SEFDM-сигналов с использованиСм Π² ΠΏΡ€ΠΈΠ΅ΠΌΠ½ΠΈΠΊΠ΅ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° поэлСмСнтной ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ с ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ связью ΠΏΠΎ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡŽ построСна Π² срСдС MatLab.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ модСлирования ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, Ρ‡Ρ‚ΠΎ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π½Ρ‹ΠΉ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌ являСтся достаточно эффСктивным. ΠŸΡ€ΠΈ допустимой вСроятности ошибок p =102…103 энСргСтичСский Π²Ρ‹ΠΈΠ³Ρ€Ρ‹Ρˆ достигаСт Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΉ 0.2…7.5 Π΄Π‘ для Ρ€Π°Π·Π»ΠΈΡ‡Π½ΠΎΠ³ΠΎ Π½Π΅ΠΎΡ€Ρ‚ΠΎΠ³ΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ разноса поднСсущих частот. Π’ Ρ‚ΠΎ ΠΆΠ΅ врСмя ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° обнаруТСния с ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ связью ΠΏΠΎ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡŽ оказываСтся сущСствСнно Π½ΠΈΠΆΠ΅, Ρ‡Π΅ΠΌ ΠΏΡ€ΠΈ ΠΏΡ€ΠΈΠ΅ΠΌΠ΅ всСй ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ посылки.Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π½Ρ‹ΠΉ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌ ΠΏΡ€ΠΈΠ΅ΠΌΠ° ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ использован Π² Π±ΡƒΠ΄ΡƒΡ‰ΠΈΡ… поколСниях мобильной связи, Π² ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Ρ‚Ρ€Π΅Π±ΡƒΡŽΡ‚ΡΡ высокиС скорости ΠΏΠ΅Ρ€Π΅Π΄Π°Ρ‡ΠΈ. Благодаря сниТСнию Π²Ρ‹Ρ‡ΠΈΡΠ»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ слоТности Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ мСньшСС энСргопотрСблСниС ΠΌΠΎΠ±ΠΈΠ»ΡŒΠ½Ρ‹Ρ… устройств

    Magnetic resonance spectroscopy of hippocampal and striatal neurometabolites inΒ experimental PTSD rat modeling

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    The spectrum of the metabolites in the dorsal region of the hippocampus and striatum was studied using the method of 1H magnetic resonance spectroscopy at experimental modeling of the posttraumatic stress disorder syndrome (PTSD) in rats. PTSD was reproduced by exposure of the cat cue to rats daily along 10 day by 10 minutes at once. The anxiety level of animals was estimated 12 days later after the end of the experimental series of stress. Based on the anxiety index, the rats were divided into 3 phenotypes. The animals with an anxiety index &gt; 0.8 (group 1) had lower plasma corticosterone compared with rats form the control group. In animals with an anxiety index in the range 0.7–0.8 (group 2), an elevated corticosterone level was noted. The rats with an anxiety index &lt; 0.7 (group 3) had a lower plasma corticosterone level compared with animals from the control group. Rats of group 2 were characterized by an increased level of GABA in the hippocampus compared with controls. In the remaining groups, the percentages of GABA in the hippocampus and striatum did not differ significantly from the control. The distribution of NAA differed form that of GABA. The highest level of NAA was found in the striatum for rats from group 1, whereas NAA in animals form groups 1 or 3 did not differ from the control. The NAA level in the hippocampus was similar between all groups, including the control. The results obtained indicate that multiple exposures to psychological stress associated with the sense of proximity of a natural enemy in some animals cause an anxiolyticΒ reaction. These animals are characterized by a stable corticosterone level and a stable level of neurometabolites in the studied structures of the brain. For rats with the highest level of anxiety, a lowered level of corticosterone with a constant level of neurometabolites in the hippocampus and striatum is characteristic. And only in rats with an intermediate level of anxiety, synchronization was observed between the increase in plasma corticosterone and the increase in hippocampal GABA content. The results obtained are in good agreement with the ideas of the protective action of glucocorticoids under PTSD manifested inΒ  restraining violations of the psycho-physiological status. The mate rials allow the neurobiological mechanisms of the protective action of glucocorticoids to be detailed
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