22 research outputs found

    Issues of legal regulation of the developed territories and space transportation in the short and medium term

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    The article is devoted to the development of law in the exploration of space by mankind. considered the issue of legal regulation of space transportation, the rights to celestial bodies, space weapons in the future. proposed options for the development of legal systems in expanding the human presence in space. Π‘Ρ‚Π°Ρ‚ΡŒΡ посвящСна вопросам развития ΠΏΡ€Π°Π²Π° ΠΏΡ€ΠΈ освоСнии чСловСчСством космоса. РассмотрСн вопрос ΠΏΡ€Π°Π²ΠΎΠ²ΠΎΠ³ΠΎ рСгулирования космичСских ΠΏΠ΅Ρ€Π΅Π²ΠΎΠ·ΠΎΠΊ, ΠΏΡ€Π°Π² Π½Π° нСбСсныС Ρ‚Π΅Π»Π°, космичСских Π²ΠΎΠΎΡ€ΡƒΠΆΠ΅Π½ΠΈΠΉ Π² Π±ΡƒΠ΄ΡƒΡ‰Π΅ΠΌ. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ‹ Π²Π°Ρ€ΠΈΠ°Π½Ρ‚Ρ‹ развития ΠΏΡ€Π°Π²ΠΎΠ²Ρ‹Ρ… систСм ΠΏΡ€ΠΈ Ρ€Π°ΡΡˆΠΈΡ€Π΅Π½ΠΈΠΈ чСловСчСского присутствия Π² космос

    The role of the state in social security law: history and development trends

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    The article is devoted to the analysis of the role of the state in social security law. Studied the historical aspect of this issue and development trends. Proposed changes to the current legislation. Π‘Ρ‚Π°Ρ‚ΡŒΡ посвящСна Π°Π½Π°Π»ΠΈΠ·Ρƒ Ρ€ΠΎΠ»ΠΈ государства Π² ΠΏΡ€Π°Π²Π΅ ΡΠΎΡ†ΠΈΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ обСспСчСния. Π˜Π·ΡƒΡ‡Π΅Π½ историчСский аспСкт Π΄Π°Π½Π½ΠΎΠ³ΠΎ вопроса ΠΈ Ρ‚Π΅Π½Π΄Π΅Π½Ρ†ΠΈΠΈ развития. ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ‹ измСнСния Π² Π΄Π΅ΠΉΡΡ‚Π²ΡƒΡŽΡ‰Π΅Π΅ Π·Π°ΠΊΠΎΠ½ΠΎΠ΄Π°Ρ‚Π΅Π»ΡŒΡΡ‚Π²ΠΎ

    ВСхнология выращивания морской микроводоросли Tetraselmis viridis ΠΏΡ€ΠΈ СстСствСнном освСщСнии ΠΈ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… тСхничСских Π·Π°Ρ‚Ρ€Π°Ρ‚Π°Ρ…

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    Π“Π»Π°Π²Π½ΠΎΠΉ ΠΏΡ€ΠΈΡ‡ΠΈΠ½ΠΎΠΉ ΠΌΠ΅Π΄Π»Π΅Π½Π½ΠΎΠ³ΠΎ внСдрСния Π½Π°ΡƒΡ‡Π½Ρ‹Ρ… Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΎΠΊ морской Π°Π»ΡŒΠ³ΠΎΡ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ Π² ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΡƒΡŽ ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΡƒ являСтся отсутствиС систСм, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰ΠΈΡ… ΠΏΠΎΠ»ΡƒΡ‡Π°Ρ‚ΡŒ биомассу микроводорослСй Π² количСствах, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΡ‹ для исслСдования ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² ΠΈ для ΠΎΡ‚Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΠΉ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈΡ… производства. Π’Π°ΠΊΠΈΠ΅ систСмы ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΡΠ½ΠΈΠ·ΠΈΡ‚ΡŒ экономичСскиС Π·Π°Ρ‚Ρ€Π°Ρ‚Ρ‹ Π½Π° созданиС ΠΈ ΠΏΠΎΠ΄Π΄Π΅Ρ€ΠΆΠ°Π½ΠΈΠ΅ благоприятных абиотичСских условий для выращивания микроводорослСй Π² ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½Ρ‹Ρ… ΠΌΠ°ΡΡˆΡ‚Π°Π±Π°Ρ…, ΠΏΠΎΡΠΊΠΎΠ»ΡŒΠΊΡƒ Π² качСствС источника освСщСния ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅Ρ‚ΡΡ энСргия солнца. Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ способ выращивания морской микроводоросли Tetraselmis viridis ΠΏΡ€ΠΈ СстСствСнном освСщСнии ΠΈ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… тСхничСских Π·Π°Ρ‚Ρ€Π°Ρ‚Π°Ρ…. Авторами Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π° мобильная установка для ΠΊΡƒΠ»ΡŒΡ‚ΠΈΠ²ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡ морских микроводорослСй ΠΈ для исслСдования ΠΈΡ… ростовых характСристик Π² условиях СстСствСнного освСщСния. Π”Π°Π½Π½ΡƒΡŽ установку прСдлагаСтся ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒ ΠΏΡ€ΠΈ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π΅ ΠΎΡ‚ Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½Ρ‹Ρ… ΠΌΠ°ΡΡˆΡ‚Π°Π±ΠΎΠ² ΠΊΡƒΠ»ΡŒΡ‚ΠΈΠ²ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡ микроводорослСй ΠΊ ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½Ρ‹ΠΌ. ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ основныС трСбования, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΌ Π΄ΠΎΠ»ΠΆΠ½Π° ΡƒΠ΄ΠΎΠ²Π»Π΅Ρ‚Π²ΠΎΡ€ΡΡ‚ΡŒ мобильная установка, ΠΈ обоснованиС Π΅Ρ‘ конструкции для ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΠ³ΠΎ выращивания Π°Π»ΡŒΠ³ΠΎΠ»ΠΎΠ³ΠΈΡ‡Π΅ΡΠΊΠΈ чистой ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Ρ‹ T. viridis. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Π° тСхнология, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰Π°Ρ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ ΠΎΡ€Π³Π°Π½ΠΈΠ·Π°Ρ†ΠΈΡŽ процСсса ΠΊΡƒΠ»ΡŒΡ‚ΠΈΠ²ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡ T. viridis с максимальной ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΡŒΡŽ ΠΊΡƒΠ»ΡŒΡ‚ΡƒΡ€Ρ‹ 5,7 Π³Β·ΠΌβˆ’2Β·ΡΡƒΡ‚βˆ’1 ΠΈ ΠΏΠ»ΠΎΡ‚Π½ΠΎΡΡ‚ΡŒΡŽ 271,6 млрд кл.Β·ΠΌβˆ’2 (RΒ² = 0,99). Π”Π°Π½Π° ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Π°Ρ ΠΎΡ†Π΅Π½ΠΊΠ° биохимичСского состава ΠΈ кинСтичСских характСристик роста T. viridis ΠΏΡ€ΠΈ Π²Ρ‹Ρ€Π°Ρ‰ΠΈΠ²Π°Π½ΠΈΠΈ Π² мобильной установкС Π² условиях СстСствСнного освСщСния ΠΈ Π² Π»Π°Π±ΠΎΡ€Π°Ρ‚ΠΎΡ€Π½Ρ‹Ρ… ΠΊΡƒΠ»ΡŒΡ‚ΠΈΠ²Π°Ρ‚ΠΎΡ€Π°Ρ… ΠΏΡ€ΠΈ постоянном искусствСнном освСщСнии

    Non-Thermal Absorption and Quantum Efficiency of SINIS Bolometer

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    We study mechanisms of absorption in two essentially different types of superconductor-insulator-normal metal-insulator-superconductor (SINIS) bolometers with absorber directly placed on Si wafer and with absorber suspended above the substrate. The figure of merit for quantum photon absorption is quantum efficiency equal to the number of detected electrons for one photon. The efficiency of absorption is dramatically dependent on phonon losses to substrate and electrodes, and electron energy losses to electrodes through tunnel junctions. The maximum quantum efficiency can approach n = hf/kT = 160 at f = 350 GHz T = 0.1 K, and current responsivity dI/dP = e/kT in quantum gain bolometer case, contrary to photon counter mode with quantum efficiency of n = 1 and responsivity dI/dP = e/hf. In experiments, we approach intrinsic quantum efficiency up to n = 80 electrons per photon in bolometer with suspended absorber, contrary to quantum efficiency of about one for absorber on the substrate. In the case of suspended Cu and Pd absorber, Kapitsa resistance protect from power leak to Al electrodes

    Superconducting Receivers for Space, Balloon, and Ground-Based Sub-Terahertz Radio Telescopes

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    We give a review of both our own original scientific results of the development of superconducting receivers for sub-terahertz astronomy and the main leading concepts of the global instrumentation. The analysis of current astronomical problems, the results of microwave astroclimate research, and the development of equipment for sub-terahertz radio astronomy studies justify the need and feasibility of a major infrastructure project in Russia to create a sub-terahertz telescope, as well as to enhance the implementation of the ongoing Millimetron and Suffa projects. The following results are discussed: i) superconducting coherent receivers and broadband subterahertz detectors for space, balloon, and ground-based radio telescopes have been developed and tested; ii) ultrasensitive receiving systems based on tunnel structures such as superconductor-insulator-superconductor (SIS) and superconductor-insulator-normal metal-insulator-superconductor (SINIS) have been created, fabricated, and examined; iii) a receiving array based on SINIS detectors and microwave readout system for such structures has been implemented; iv) methods for manufacturing high-quality tunnel structures Nb/AlOx/Nb and Nb/AlN/NbN based on niobium films with a current density of up to 30 kA/cm(2) have been developed. Receivers operated at 200 to 950 GHz and having a noise temperature only a factor of 2 to 5 higher than the quantum limit have been created and tested

    Morphological changes of adrenal cortex and medulla during the first 24 hours after acute hemorrhage

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    Experimentally established that during the first day after acute blood loss expressed morphological changes occur in the adrenal cortex and medulla, indicating a high functional stress of the organ

    Arrays of sub‐terahertz cryogenic metamaterial

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    Integrated quasi‐optical cryogenic terahertz receivers contain arrays of detectors, quasi‐optical filters, interferometers, and other metamaterials. Matrices of quasi‐optical band‐pass, low‐pass, and high‐pass filters, Fabry–Perot grid interferometers, and arrays of half‐wave and electrically small antennas with superconductor‐insulator‐normal metal‐insulator‐superconductor (SINIS) sub‐terahertz wavelength range detectors were fabricated and experimentally studied on the same computational, technological, and experimental platform. For the design of the filters, we used the periodic frequency‐selective surfaces (FSS) approach, contrary to detector arrays that can be presented in a model of distributed absorbers. The structures were fabricated using direct electron bSeam lithography, thermal shadow evaporation, lift‐off, alternatively magnetron sputtering, and chemical and plasma etching. The numerical simulation methods of such structures are sufficiently different: for the reactive matrices with low losses, the approximation of an infinite structure with periodic boundary conditions is applicable, and for the arrays of detectors with dissipative elements of absorbers, a complete analysis of the finite structure with hundreds of interacting ports is applicable. The difference is determined by the presence of dissipation in the detector arrays, the phase of the reflected or re‐emitted signal turned out to be undefined and the Floquet periodic boundary conditions are correct only for a phased array antenna. The spectral characteristics of the created filters, interferometers, and antenna arrays were measured in the frequency range 50–600 GHz
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