53 research outputs found

    Anomalous Zero Sound

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    We show that the anomalous term in the current, recently suggested by Son and Yamamoto, modifies the structure of the zero sound mode in the Fermi liquid in a magnetic field.Comment: 14 pages, 2 figure

    ПовСдСниС ΠΌΠΎΡ€Ρ„ΠΎΠ»ΠΈΠ½Π° ΠΈ Π΅Π³ΠΎ тримСтилсилилпроизводного Π² рСакциях с тримСтилсилилизоцианатом

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    Objectives. To study the patterns of behavior of morpholine and its trimethylsilyl derivative in reactions with trimethylsilyl isocyanate.Methods. The study employed infrared and nuclear magnetic resonance spectroscopy, as well as elemental analysis.Results. The formation of mixtures of tautomeric forms of silicon-containing ureaβ€”N-(trimethylsilyl) morpholine-4-carboxamide and trimethylsilylmorpholine-4-carboximidoateβ€”was established.Conclusions. It is shown that the composition and structure of the resulting products are determined both by the presence of a morpholine substituent at the nitrogen atom and by the type of isocyanate used. Unlike the trimethylsilyl derivative of morpholine, morpholine itself reacts with trimethylsilyl isocyanate to form a mixture of tautomeric forms.Π¦Π΅Π»ΠΈ. Π˜Π·ΡƒΡ‡ΠΈΡ‚ΡŒ закономСрности повСдСния ΠΌΠΎΡ€Ρ„ΠΎΠ»ΠΈΠ½Π° ΠΈ Π΅Π³ΠΎ тримСтилсилилпроизводного Π² рСакциях с тримСтилсилилизоцианатом.ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹. Π’ исслСдовании использовались ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ инфракрасной спСктроскопии, спСктроскопии ядСрного ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠ³ΠΎ рСзонанса ΠΈ элСмСнтного Π°Π½Π°Π»ΠΈΠ·Π°.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. УстановлСно ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ смСси Ρ‚Π°ΡƒΡ‚ΠΎΠΌΠ΅Ρ€Π½Ρ‹Ρ… Ρ„ΠΎΡ€ΠΌ крСмнийсодСрТащСй ΠΌΠΎΡ‡Π΅Π²ΠΈΠ½Ρ‹: N-(тримСтилсилил)ΠΌΠΎΡ€Ρ„ΠΎΠ»ΠΈΠ½-4-карбоксамида ΠΈ тримСтилсилилморфолин -4-карбоксимидоата.Π’Ρ‹Π²ΠΎΠ΄Ρ‹. УстановлСно, Ρ‡Ρ‚ΠΎ состав ΠΈ строСниС ΠΎΠ±Ρ€Π°Π·ΡƒΡŽΡ‰ΠΈΡ…ΡΡ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ² опрСдСляСтся ΠΊΠ°ΠΊ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ΠΌ замСститСля ΠΏΡ€ΠΈ Π°Ρ‚ΠΎΠΌΠ΅ Π°Π·ΠΎΡ‚Π° ΠΌΠΎΡ€Ρ„ΠΎΠ»ΠΈΠ½Π°, Ρ‚Π°ΠΊ ΠΈ Ρ‚ΠΈΠΏΠΎΠΌ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅ΠΌΠΎΠ³ΠΎ ΠΈΠ·ΠΎΡ†ΠΈΠ°Π½Π°Ρ‚Π°. Показано, Ρ‡Ρ‚ΠΎ, Π² ΠΎΡ‚Π»ΠΈΡ‡ΠΈΠ΅ ΠΎΡ‚ Ρ‚Ρ€ΠΈΠΌΠ΅Ρ‚ΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΡŒΠ½ΠΎΠ³ΠΎ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΌΠΎΡ€Ρ„ΠΎΠ»ΠΈΠ½Π°, сам ΠΌΠΎΡ€Ρ„ΠΎΠ»ΠΈΠ½ взаимодСйствуСт с тримСтилсилилизоцианатом с ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ смСси Ρ‚Π°ΡƒΡ‚ΠΎΠΌΠ΅Ρ€Π½Ρ‹Ρ… Ρ„ΠΎΡ€ΠΌ

    Thermal processes of thermokarst lakes in the continuous permafrost zone of northern Siberia - observations and modeling (Lena River Delta, Siberia)

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    Β© Author(s) 2015. Thermokarst lakes are typical features of the northern permafrost ecosystems, and play an important role in the thermal exchange between atmosphere and subsurface. The objective of this study is to describe the main thermal processes of the lakes and to quantify the heat exchange with the underlying sediments. The thermal regimes of five lakes located within the continuous permafrost zone of northern Siberia (Lena River Delta) were investigated using hourly water temperature and water level records covering a 3-year period (2009-2012), together with bathymetric survey data. The lakes included thermokarst lakes located on Holocene river terraces that may be connected to Lena River water during spring flooding, and a thermokarst lake located on deposits of the Pleistocene Ice Complex. Lakes were covered by ice up to 2 m thick that persisted for more than 7 months of the year, from October until about mid-June. Lake-bottom temperatures increased at the start of the ice-covered period due to upward-directed heat flux from the underlying thawed sediment. Prior to ice break-up, solar radiation effectively warmed the water beneath the ice cover and induced convective mixing. Ice break-up started at the beginning of June and lasted until the middle or end of June. Mixing occurred within the entire water column from the start of ice break-up and continued during the ice-free periods, as confirmed by the Wedderburn numbers, a quantitative measure of the balance between wind mixing and stratification that is important for describing the biogeochemical cycles of lakes. The lake thermal regime was modeled numerically using the FLake model. The model demonstrated good agreement with observations with regard to the mean lake temperature, with a good reproduction of the summer stratification during the ice-free period, but poor agreement during the ice-covered period. Modeled sensitivity to lake depth demonstrated that lakes in this climatic zone with mean depths > 5 m develop continuous stratification in summer for at least 1 month. The modeled vertical heat flux across the bottom sediment tends towards an annual mean of zero, with maximum downward fluxes of about 5 W m-2 in summer and with heat released back into the water column at a rate of less than 1 W m-2 during the ice-covered period. The lakes are shown to be efficient heat absorbers and effectively distribute the heat through mixing. Monthly bottom water temperatures during the ice-free period range up to 15 Β°C and are therefore higher than the associated monthly air or ground temperatures in the surrounding frozen permafrost landscape. The investigated lakes remain unfrozen at depth, with mean annual lake-bottom temperatures of between 2.7 and 4 Β°C

    ΠžΠ‘ΠžΠ‘Π•ΠΠΠžΠ‘Π’Π˜ Π’Π—ΠΠ˜ΠœΠžΠ”Π•Π™Π‘Π’Π’Π˜Π― Π˜Π—ΠžΠ¦Π˜ΠΠΠΠ’ΠžΠ’ Π‘ ΠŸΠ ΠžΠ˜Π—Π’ΠžΠ”ΠΠ«ΠœΠ˜ Π“Π˜Π”Π ΠΠ—Π˜ΠΠ

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    The results of studies on chemical transformations of organic and organosilicon isocyanates in their interaction with hydrazine derivatives have been summarized in this review. It is shown that hydrazine and its derivatives including organosilicon compounds reacting with organic isocyanates form corresponding semicarbazides readily enough. The reaction conditions that effect the composition, structure and yield of the resulting target products are presented. A significant difference in the interaction of trimethylsilyl isocyanate with organic and organosilicon derivatives of hydrazine is demonstrated. It is demonstrated that the reason for the impossibility to isolate trimethylsilyl derivatives of semicarbazide is their low hydrolytic stability, as well as high silylating ability. Peculiarities of the reaction of trimethylsilyl isocyanate and dimethylchloromethyl isocyanate silane with 1,1-dimethylhydrazine, its trimethylsilyl analog and isoniazid are given. Possible schemes for the formation of a previously unknown O-trimethylsilyl-1,1-dimethylhydrazinecarboximidoate are presented. The results of using carbofunctional organosilicon isocyanates in these processes are discussed. Basic trends in practical use of the prepared compounds as physiologically active preparations in polymer chemistry and agriculture are shown.Π’ ΠΎΠ±Π·ΠΎΡ€Π΅ ΠΎΠ±ΠΎΠ±Ρ‰Π΅Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдований ΠΏΠΎ ΠΈΠ·ΡƒΡ‡Π΅Π½ΠΈΡŽ химичСских ΠΏΡ€Π΅Π²Ρ€Π°Ρ‰Π΅Π½ΠΈΠΉ органичСских ΠΈ крСмнийорганичСских ΠΈΠ·ΠΎΡ†ΠΈΠ°Π½Π°Ρ‚ΠΎΠ² ΠΏΡ€ΠΈ ΠΈΡ… взаимодСйствии с ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹ΠΌΠΈ Π³ΠΈΠ΄Ρ€Π°Π·ΠΈΠ½Π°. Показано, Ρ‡Ρ‚ΠΎ с органичСскими ΠΈΠ·ΠΎΡ†ΠΈΠ°Π½Π°Ρ‚Π°ΠΌΠΈ Π³ΠΈΠ΄Ρ€Π°Π·ΠΈΠ½ ΠΈ Π΅Π³ΠΎ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Π΅, Π² Ρ‚ΠΎΠΌ числС ΠΈ крСмнийорганичСскиС, достаточно Π»Π΅Π³ΠΊΠΎ ΠΎΠ±Ρ€Π°Π·ΡƒΡŽΡ‚ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠ΅ сСмикарбазиды. ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ условия провСдСния Ρ€Π΅Π°ΠΊΡ†ΠΈΠΉ, ΠΎΠΊΠ°Π·Ρ‹Π²Π°ΡŽΡ‰ΠΈΠ΅ влияниС Π½Π° состав, строСниС ΠΈ Π²Ρ‹Ρ…ΠΎΠ΄ ΠΎΠ±Ρ€Π°Π·ΡƒΡŽΡ‰ΠΈΡ…ΡΡ Ρ†Π΅Π»Π΅Π²Ρ‹Ρ… ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΎΠ². Показано сущСствСнноС ΠΎΡ‚Π»ΠΈΡ‡ΠΈΠ΅ взаимодСйствия тримСтилсилилизоцианата с органичСскими ΠΈ крСмнийорганичСскими ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹ΠΌΠΈ Π³ΠΈΠ΄Ρ€Π°Π·ΠΈΠ½Π°. Показано, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈΡ‡ΠΈΠ½ΠΎΠΉ нСвозмоТности выдСлСния Ρ‚Ρ€ΠΈΠΌΠ΅Ρ‚ΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΡŒΠ½Ρ‹Ρ… ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… сСмикарбазида являСтся ΠΈΡ… низкая гидролитичСская ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΡΡ‚ΡŒ, Π° Ρ‚Π°ΠΊΠΆΠ΅ высокая ΡΠΈΠ»ΠΈΠ»ΠΈΡ€ΡƒΡŽΡ‰Π°Ρ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒ. ΠžΠ±ΡΡƒΠΆΠ΄Π΅Π½Ρ‹ особСнности Ρ€Π΅Π°ΠΊΡ†ΠΈΠΉ взаимодСйствия тримСтилсилилизоцианата ΠΈ димСтилхлормСтилизоцианатосилана с 1,1-Π΄ΠΈΠΌΠ΅Ρ‚ΠΈΠ»Π³ΠΈΠ΄Ρ€Π°Π·ΠΈΠ½ΠΎΠΌ, Π΅Π³ΠΎ тримСтилсилилным Π°Π½Π°Π»ΠΎΠ³ΠΎΠΌ ΠΈ ΠΈΠ·ΠΎΠ½ΠΈΠ°Π·ΠΈΠ΄ΠΎΠΌ. ΠŸΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹Π΅ Π²Π°Ρ€ΠΈΠ°Π½Ρ‚Ρ‹ схСм образования Ρ€Π°Π½Π΅Π΅ нСизвСстного О-тримСтилсилил-1,1-димСтилгидразинкарбоксимидоата. ΠŸΠΎΠΊΠ°Π·Π°Π½Ρ‹ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ использования Π² Π΄Π°Π½Π½Ρ‹Ρ… процСссах ΠΊΠ°Ρ€Π±ΠΎΡ„ΡƒΠ½ΠΊΡ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½Ρ‹Ρ… крСмнийорганичСских ΠΈΠ·ΠΎΡ†ΠΈΠ°Π½Π°Ρ‚ΠΎΠ². ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Ρ‹ основныС направлСния практичСского использования ΠΏΠΎΠ»ΡƒΡ‡Π°Π΅ΠΌΡ‹Ρ… соСдинСний - Π² качСствС физиологичСски Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ΠΎΠ², Π² ΠΏΠΎΠ»ΠΈΠΌΠ΅Ρ€Π½ΠΎΠΉ Ρ…ΠΈΠΌΠΈΠΈ ΠΈ Π² сСльском хозяйствС

    Chiral drag force

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    We provide a holographic evaluation of novel contributions to the drag force acting on a heavy quark moving through strongly interacting plasma. The new contributions are chiral in that they act in opposite directions in plasmas containing an excess of left- or right-handed quarks and in that they are proportional to the coefficient of the axial anomaly. These new contributions to the drag force act either parallel to or antiparallel to an external magnetic field or to the vorticity of the fluid plasma. In all these respects, these contributions to the drag force felt by a heavy quark are analogous to the chiral magnetic effect on light quarks. However, the new contribution to the drag force is independent of the electric charge of the heavy quark and is the same for heavy quarks and antiquarks. We show that although the chiral drag force can be non-vanishing for heavy quarks that are at rest in the local fluid rest frame, it does vanish for heavy quarks that are at rest in a suitably chosen frame. In this frame, the heavy quark at rest sees counterpropagating momentum and charge currents, both proportional to the axial anomaly coefficient, but feels no drag force. This provides strong concrete evidence for the absence of dissipation in chiral transport, something that has been predicted previously via consideration of symmetries. Along the way to our principal results, we provide a general calculation of the corrections to the drag force due to the presence of gradients in the flowing fluid in the presence of a nonzero chemical potential. We close with a consequence of our result that is at least in principle observable in heavy ion collisions, namely an anticorrelation between the direction of the CME current for light quarks in a given event and the direction of the kick given to the momentum of all the heavy quarks and antiquarks in that event.Comment: 28 pages, small improvement to the discussion of gravitational anomaly, references adde

    ΠšΠ’ΠΠΠ’ΠžΠ’Πž-Π₯Π˜ΠœΠ˜Π§Π•Π‘ΠšΠ˜Π™ ΠΠΠΠ›Π˜Π— Π‘Π’Π Π£ΠšΠ’Π£Π ΠžΠžΠ‘Π ΠΠ—ΠžΠ’ΠΠΠ˜Π― КАРКАБНЫΠ₯ ΠžΠ Π“ΠΠΠžΠ‘Π˜Π›ΠžΠšΠ‘ΠΠΠžΠ’ И ΠœΠ•Π’ΠΠ›Π›ΠžΠžΠ Π“ΠΠΠžΠ‘Π˜Π›ΠžΠšΠ‘ΠΠΠžΠ’

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    Several ab initio (DFT-B3PW91/6-31g(d,p)) calculations of cage-like siloxanes (MeSiO1.5)n (n = 4-12) have been made. It was shown that cubane-like structure (MeSiO1.5)8 is the most stable one. Refined mechanism of polymeric metallasiloxanes cleavage by the silanolates has been suggested. It has been shown that isomerisation of Cu-containing siloxanes (rearrangement of sandwich-like form into globule-like form) is mostly governed by the coordination properties of solvates.ΠšΠ²Π°Π½Ρ‚ΠΎΠ²ΠΎ-химичСскими расчСтами каркасных органосилсСсквиоксанов ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ наибольшСй ΡΡ‚Π°Π±ΠΈΠ»ΡŒΠ½ΠΎΡΡ‚ΡŒΡŽ ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ‚ кубановая структура (MeSiO1.5)8. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡƒΡ‚ΠΎΡ‡Π½Π΅Π½ΠΈΠ΅ ΠΌΠ΅Ρ…Π°Π½ΠΈΠ·ΠΌΠ° расщСплСния ΠΎΠ»ΠΈΠ³ΠΎΠΌΠ΅Ρ€Π½Ρ‹Ρ… мСталлоорганосилоксанов органосиланолятами Ρ‰Π΅Π»ΠΎΡ‡Π½Ρ‹Ρ… ΠΌΠ΅-Ρ‚Π°Π»Π»ΠΎΠ², ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π° схСма синтСза. На основании расчСтов ΠΏΡ€Π΅Π΄ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΎ, Ρ‡Ρ‚ΠΎ Ρ€Π΅Π°ΠΊΡ†ΠΈΠΈ мСталлсодСрТащих силоксанов ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΡΡŽΡ‚ΡΡ ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌ влияниСм растворитСлСй

    Диагностика ΠΈ ΠΌΠΎΠ½ΠΈΡ‚ΠΎΡ€ΠΈΠ½Π³ Π½Π΅ΠΉΡ€ΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ поврСТдСния ΠΏΡ€ΠΈ тяТСлой Ρ‡Π΅Ρ€Π΅ΠΏΠ½ΠΎ-ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ Ρ‚Ρ€Π°Π²ΠΌΠ΅

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    Objective: to search for an accessible, valid, and easy-to-use method for the diagnosis and monitoring of a neuronal lesion in severe brain injury (SBI). Subjects and methods. Thirty-three patients aged 18β€”55 years with isolated SBI (the Glasgow coma scores for admission consciousness were 6Β±2) were examined; the serum content of neuron-specific protein S-100B was further analyzed. Results and discussion. The cell damage marker concentration was substantially increased in the acute period of brain injury. When the pathological process followed a favorable course, S-100B was considerably decreased just on day 2 of the disease. When the changes were negative, S-100B concentrations remained virtually unchanged or even increased, which was indicative of secondary brain reperfusion/ischemic lesions. The mean baseline marker level varied with the type of brain injury diagnosed by computed tomography; the highest figures being noted in the groups where significant brain tissue lesion was detected. Key words: severe brain injury, prognosis, S-100B protein.ЦСль исслСдования β€” поиск доступного, Π½Π°Π΄Π΅ΠΆΠ½ΠΎΠ³ΠΎ ΠΈ простого ΠΌΠ΅Ρ‚ΠΎΠ΄Π° диагностики ΠΈ ΠΌΠΎΠ½ΠΈΡ‚ΠΎΡ€ΠΈΠ½Π³Π° Π½Π΅ΠΉΡ€ΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ поврСТдСния ΠΏΡ€ΠΈ ВЧМВ. ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ обслСдованиС 33 ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚ΠΎΠ² с ΠΈΠ·ΠΎΠ»ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠΉ ВЧМВ Π² возрастС 18β€”55 Π»Π΅Ρ‚ (ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ сознания ΠΏΡ€ΠΈ поступлСнии Π² стационар 6Β±2 Π±Π°Π»Π»Π° ΠΏΠΎ Π¨ΠšΠ“), с ΠΏΠΎΡΠ»Π΅Π΄ΡƒΡŽΡ‰ΠΈΠΌ Π°Π½Π°Π»ΠΈΠ·ΠΎΠΌ содСрТания нСйронспСцифичСского ΠΏΡ€ΠΎΡ‚Π΅ΠΈΠ½Π° S-100Π’ Π² сывороткС ΠΊΡ€ΠΎΠ²ΠΈ. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΈ обсуТдСниС. ΠšΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΡ ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π° ΠΊΠ»Π΅Ρ‚ΠΎΡ‡Π½ΠΎΠ³ΠΎ поврСТдСния Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΏΠΎΠ²Ρ‹ΡˆΠ°Π»Π°ΡΡŒ Π² остром ΠΏΠ΅Ρ€ΠΈΠΎΠ΄Π΅ Ρ‡Π΅Ρ€Π΅ΠΏΠ½ΠΎ-ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ Ρ‚Ρ€Π°Π²ΠΌΡ‹. ΠŸΡ€ΠΈ благоприятном Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠΈ патологичСского процСсса ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ S-100Π’ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ сниТался ΡƒΠΆΠ΅ Π½Π° 2-Π΅ сутки Π±ΠΎΠ»Π΅Π·Π½ΠΈ. ΠŸΡ€ΠΈ ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ΅ концСнтрация S-100Π’ ΠΎΡΡ‚Π°Π²Π°Π»Π°ΡΡŒ практичСски Π½Π΅ΠΈΠ·ΠΌΠ΅Π½Π½ΠΎΠΉ ΠΈΠ»ΠΈ Π΄Π°ΠΆΠ΅ ΠΏΠΎΠ²Ρ‹ΡˆΠ°Π»Π°ΡΡŒ, Ρ‡Ρ‚ΠΎ ΡΠ²ΠΈΠ΄Π΅Ρ‚Π΅Π»ΡŒΡΡ‚Π²ΠΎΠ²Π°Π»ΠΎ ΠΎ Π²Ρ‚ΠΎΡ€ΠΈΡ‡Π½Ρ‹Ρ… Ρ€Π΅ΠΏΠ΅Ρ€Ρ„ΡƒΠ·ΠΈΠΎΠ½Π½Ρ‹Ρ… поврСТдСниях Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π°. Показано, Ρ‡Ρ‚ΠΎ срСдниС значСния Π½Π°Ρ‡Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ уровня ΠΌΠ°Ρ€ΠΊΠ΅Ρ€Π° Ρ€Π°Π·Π»ΠΈΡ‡Π°Π»ΠΈΡΡŒ Π² зависимости ΠΎΡ‚ Π²ΠΈΠ΄Π° ЧМВ, диагностированного КВ, ΠΏΡ€ΠΈΡ‡Π΅ΠΌ наибольшиС Ρ†ΠΈΡ„Ρ€Ρ‹ ΠΎΡ‚ΠΌΠ΅Ρ‡Π°Π»ΠΈΡΡŒ Π² Π³Ρ€ΡƒΠΏΠΏΠ°Ρ…, Π³Π΄Π΅ Π²Ρ‹ΡΠ²Π»ΡΠ»ΠΎΡΡŒ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ΅ ΠΏΠΎΠ²Ρ€Π΅ΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ Ρ‚ΠΊΠ°Π½ΠΈ. ΠšΠ»ΡŽΡ‡Π΅Π²Ρ‹Π΅ слова: тяТСлая Ρ‡Π΅Ρ€Π΅ΠΏΠ½ΠΎ-мозговая Ρ‚Ρ€Π°Π²ΠΌΠ°, ΠΏΡ€ΠΎΠ³Π½ΠΎΠ·, Π±Π΅Π»ΠΎΠΊ S-100Π’

    Quantum Gravity in Everyday Life: General Relativity as an Effective Field Theory

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    This article is meant as a summary and introduction to the ideas of effective field theory as applied to gravitational systems. Contents: 1. Introduction 2. Effective Field Theories 3. Low-Energy Quantum Gravity 4. Explicit Quantum Calculations 5. ConclusionsComment: 56 pages, 2 figures, JHEP style, Invited review to appear in Living Reviews of Relativit
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