53 research outputs found
Anomalous Zero Sound
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
ΠΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΠΌΠΎΡΡΠΎΠ»ΠΈΠ½Π° ΠΈ Π΅Π³ΠΎ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π² ΡΠ΅Π°ΠΊΡΠΈΡΡ Ρ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠΎΠΌ
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 ureaβN-(trimethylsilyl) morpholine-4-carboxamide and trimethylsilylmorpholine-4-carboximidoateβwas 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. ΠΠ·ΡΡΠΈΡΡ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΠΌΠΎΡΡΠΎΠ»ΠΈΠ½Π° ΠΈ Π΅Π³ΠΎ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π² ΡΠ΅Π°ΠΊΡΠΈΡΡ
Ρ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠΎΠΌ.ΠΠ΅ΡΠΎΠ΄Ρ. Π ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΈ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π»ΠΈΡΡ ΠΌΠ΅ΡΠΎΠ΄Ρ ΠΈΠ½ΡΡΠ°ΠΊΡΠ°ΡΠ½ΠΎΠΉ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ, ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΡΠ΄Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π·ΠΎΠ½Π°Π½ΡΠ° ΠΈ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π°.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠΌΠ΅ΡΠΈ ΡΠ°ΡΡΠΎΠΌΠ΅ΡΠ½ΡΡ
ΡΠΎΡΠΌ ΠΊΡΠ΅ΠΌΠ½ΠΈΠΉΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠ΅ΠΉ ΠΌΠΎΡΠ΅Π²ΠΈΠ½Ρ: N-(ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»)ΠΌΠΎΡΡΠΎΠ»ΠΈΠ½-4-ΠΊΠ°ΡΠ±ΠΎΠΊΡΠ°ΠΌΠΈΠ΄Π° ΠΈ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΠΌΠΎΡΡΠΎΠ»ΠΈΠ½ -4-ΠΊΠ°ΡΠ±ΠΎΠΊΡΠΈΠΌΠΈΠ΄ΠΎΠ°ΡΠ°.ΠΡΠ²ΠΎΠ΄Ρ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΡΠΎΡΡΠ°Π² ΠΈ ΡΡΡΠΎΠ΅Π½ΠΈΠ΅ ΠΎΠ±ΡΠ°Π·ΡΡΡΠΈΡ
ΡΡ ΠΏΡΠΎΠ΄ΡΠΊΡΠΎΠ² ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ ΠΊΠ°ΠΊ Π½Π°Π»ΠΈΡΠΈΠ΅ΠΌ Π·Π°ΠΌΠ΅ΡΡΠΈΡΠ΅Π»Ρ ΠΏΡΠΈ Π°ΡΠΎΠΌΠ΅ Π°Π·ΠΎΡΠ° ΠΌΠΎΡΡΠΎΠ»ΠΈΠ½Π°, ΡΠ°ΠΊ ΠΈ ΡΠΈΠΏΠΎΠΌ ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΠΌΠΎΠ³ΠΎ ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠ°. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ, Π² ΠΎΡΠ»ΠΈΡΠΈΠ΅ ΠΎΡ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΌΠΎΡΡΠΎΠ»ΠΈΠ½Π°, ΡΠ°ΠΌ ΠΌΠΎΡΡΠΎΠ»ΠΈΠ½ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΡΠ΅Ρ Ρ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠΎΠΌ Ρ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΌΠ΅ΡΠΈ ΡΠ°ΡΡΠΎΠΌΠ΅ΡΠ½ΡΡ
ΡΠΎΡΠΌ
Thermal processes of thermokarst lakes in the continuous permafrost zone of northern Siberia - observations and modeling (Lena River Delta, Siberia)
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
ΠΠ‘ΠΠΠΠΠΠΠ‘Π’Π ΠΠΠΠΠΠΠΠΠΠ‘Π’ΠΠΠ― ΠΠΠΠ¦ΠΠΠΠΠ’ΠΠ Π‘ ΠΠ ΠΠΠΠΠΠΠΠ«ΠΠ ΠΠΠΠ ΠΠΠΠΠ
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·ΠΎΡΠ΅ ΠΎΠ±ΠΎΠ±ΡΠ΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠΎ ΠΈΠ·ΡΡΠ΅Π½ΠΈΡ Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠ΅Π²ΡΠ°ΡΠ΅Π½ΠΈΠΉ ΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΠΊΡΠ΅ΠΌΠ½ΠΈΠΉΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠΎΠ² ΠΏΡΠΈ ΠΈΡ
Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠΈ Ρ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΠΌΠΈ Π³ΠΈΠ΄ΡΠ°Π·ΠΈΠ½Π°. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Ρ ΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠ°ΠΌΠΈ Π³ΠΈΠ΄ΡΠ°Π·ΠΈΠ½ ΠΈ Π΅Π³ΠΎ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΠ΅, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ ΠΈ ΠΊΡΠ΅ΠΌΠ½ΠΈΠΉΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠ΅, Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎ Π»Π΅Π³ΠΊΠΎ ΠΎΠ±ΡΠ°Π·ΡΡΡ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠ΅ ΡΠ΅ΠΌΠΈΠΊΠ°ΡΠ±Π°Π·ΠΈΠ΄Ρ. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΡΠ΅Π°ΠΊΡΠΈΠΉ, ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡΠΈΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° ΡΠΎΡΡΠ°Π², ΡΡΡΠΎΠ΅Π½ΠΈΠ΅ ΠΈ Π²ΡΡ
ΠΎΠ΄ ΠΎΠ±ΡΠ°Π·ΡΡΡΠΈΡ
ΡΡ ΡΠ΅Π»Π΅Π²ΡΡ
ΠΏΡΠΎΠ΄ΡΠΊΡΠΎΠ². ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ΅ ΠΎΡΠ»ΠΈΡΠΈΠ΅ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠ° Ρ ΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΈ ΠΊΡΠ΅ΠΌΠ½ΠΈΠΉΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΠΌΠΈ Π³ΠΈΠ΄ΡΠ°Π·ΠΈΠ½Π°. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΏΡΠΈΡΠΈΠ½ΠΎΠΉ Π½Π΅Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ Π²ΡΠ΄Π΅Π»Π΅Π½ΠΈΡ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΡΠ½ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΡΡ
ΡΠ΅ΠΌΠΈΠΊΠ°ΡΠ±Π°Π·ΠΈΠ΄Π° ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΈΡ
Π½ΠΈΠ·ΠΊΠ°Ρ Π³ΠΈΠ΄ΡΠΎΠ»ΠΈΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΡΠ°Π±ΠΈΠ»ΡΠ½ΠΎΡΡΡ, Π° ΡΠ°ΠΊΠΆΠ΅ Π²ΡΡΠΎΠΊΠ°Ρ ΡΠΈΠ»ΠΈΠ»ΠΈΡΡΡΡΠ°Ρ ΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡ. ΠΠ±ΡΡΠΆΠ΄Π΅Π½Ρ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΡΠ΅Π°ΠΊΡΠΈΠΉ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠ° ΠΈ Π΄ΠΈΠΌΠ΅ΡΠΈΠ»Ρ
Π»ΠΎΡΠΌΠ΅ΡΠΈΠ»ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠΎΡΠΈΠ»Π°Π½Π° Ρ 1,1-Π΄ΠΈΠΌΠ΅ΡΠΈΠ»Π³ΠΈΠ΄ΡΠ°Π·ΠΈΠ½ΠΎΠΌ, Π΅Π³ΠΎ ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»Π½ΡΠΌ Π°Π½Π°Π»ΠΎΠ³ΠΎΠΌ ΠΈ ΠΈΠ·ΠΎΠ½ΠΈΠ°Π·ΠΈΠ΄ΠΎΠΌ. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠ΅ Π²Π°ΡΠΈΠ°Π½ΡΡ ΡΡ
Π΅ΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ°Π½Π΅Π΅ Π½Π΅ΠΈΠ·Π²Π΅ΡΡΠ½ΠΎΠ³ΠΎ Π-ΡΡΠΈΠΌΠ΅ΡΠΈΠ»ΡΠΈΠ»ΠΈΠ»-1,1-Π΄ΠΈΠΌΠ΅ΡΠΈΠ»Π³ΠΈΠ΄ΡΠ°Π·ΠΈΠ½ΠΊΠ°ΡΠ±ΠΎΠΊΡΠΈΠΌΠΈΠ΄ΠΎΠ°ΡΠ°. ΠΠΎΠΊΠ°Π·Π°Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π² Π΄Π°Π½Π½ΡΡ
ΠΏΡΠΎΡΠ΅ΡΡΠ°Ρ
ΠΊΠ°ΡΠ±ΠΎΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΠΊΡΠ΅ΠΌΠ½ΠΈΠΉΠΎΡΠ³Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΠ·ΠΎΡΠΈΠ°Π½Π°ΡΠΎΠ². ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΠΎΡΠ½ΠΎΠ²Π½ΡΠ΅ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠ»ΡΡΠ°Π΅ΠΌΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ - Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈ Π°ΠΊΡΠΈΠ²Π½ΡΡ
ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ², Π² ΠΏΠΎΠ»ΠΈΠΌΠ΅ΡΠ½ΠΎΠΉ Ρ
ΠΈΠΌΠΈΠΈ ΠΈ Π² ΡΠ΅Π»ΡΡΠΊΠΎΠΌ Ρ
ΠΎΠ·ΡΠΉΡΡΠ²Π΅
Chiral drag force
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
ΠΠΠΠΠ’ΠΠΠ-Π₯ΠΠΠΠ§ΠΠ‘ΠΠΠ ΠΠΠΠΠΠ Π‘Π’Π Π£ΠΠ’Π£Π ΠΠΠΠ ΠΠΠΠΠΠΠΠ― ΠΠΠ ΠΠΠ‘ΠΠ«Π₯ ΠΠ ΠΠΠΠΠ‘ΠΠΠΠΠ‘ΠΠΠΠ Π ΠΠΠ’ΠΠΠΠΠΠ ΠΠΠΠΠ‘ΠΠΠΠΠ‘ΠΠΠΠ
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.ΠΠ²Π°Π½ΡΠΎΠ²ΠΎ-Ρ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ°ΡΡΠ΅ΡΠ°ΠΌΠΈ ΠΊΠ°ΡΠΊΠ°ΡΠ½ΡΡ
ΠΎΡΠ³Π°Π½ΠΎΡΠΈΠ»ΡΠ΅ΡΠΊΠ²ΠΈΠΎΠΊΡΠ°Π½ΠΎΠ² ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Π½Π°ΠΈΠ±ΠΎΠ»ΡΡΠ΅ΠΉ ΡΡΠ°Π±ΠΈΠ»ΡΠ½ΠΎΡΡΡΡ ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ ΠΊΡΠ±Π°Π½ΠΎΠ²Π°Ρ ΡΡΡΡΠΊΡΡΡΠ° (MeSiO1.5)8. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΡΠΎΡΠ½Π΅Π½ΠΈΠ΅ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠ° ΡΠ°ΡΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡ ΠΎΠ»ΠΈΠ³ΠΎΠΌΠ΅ΡΠ½ΡΡ
ΠΌΠ΅ΡΠ°Π»Π»ΠΎΠΎΡΠ³Π°Π½ΠΎΡΠΈΠ»ΠΎΠΊΡΠ°Π½ΠΎΠ² ΠΎΡΠ³Π°Π½ΠΎΡΠΈΠ»Π°Π½ΠΎΠ»ΡΡΠ°ΠΌΠΈ ΡΠ΅Π»ΠΎΡΠ½ΡΡ
ΠΌΠ΅-ΡΠ°Π»Π»ΠΎΠ², ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π° ΡΡ
Π΅ΠΌΠ° ΡΠΈΠ½ΡΠ΅Π·Π°. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ°ΡΡΠ΅ΡΠΎΠ² ΠΏΡΠ΅Π΄ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΎ, ΡΡΠΎ ΡΠ΅Π°ΠΊΡΠΈΠΈ ΠΌΠ΅ΡΠ°Π»Π»ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΡ
ΡΠΈΠ»ΠΎΠΊΡΠ°Π½ΠΎΠ² ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΡΡ ΠΊΠΎΠΎΡΠ΄ΠΈΠ½ΠΈΡΡΡΡΠΈΠΌ Π²Π»ΠΈΡΠ½ΠΈΠ΅ΠΌ ΡΠ°ΡΡΠ²ΠΎΡΠΈΡΠ΅Π»Π΅ΠΉ
ΠΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ° ΠΈ ΠΌΠΎΠ½ΠΈΡΠΎΡΠΈΠ½Π³ Π½Π΅ΠΉΡΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ ΠΏΡΠΈ ΡΡΠΆΠ΅Π»ΠΎΠΉ ΡΠ΅ΡΠ΅ΠΏΠ½ΠΎ-ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ ΡΡΠ°Π²ΠΌΠ΅
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 18β55 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.Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ β ΠΏΠΎΠΈΡΠΊ Π΄ΠΎΡΡΡΠΏΠ½ΠΎΠ³ΠΎ, Π½Π°Π΄Π΅ΠΆΠ½ΠΎΠ³ΠΎ ΠΈ ΠΏΡΠΎΡΡΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠΈ ΠΈ ΠΌΠΎΠ½ΠΈΡΠΎΡΠΈΠ½Π³Π° Π½Π΅ΠΉΡΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ ΠΏΡΠΈ Π’Π§ΠΠ’. ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΠΎΠ±ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ 33 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΈΠ·ΠΎΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΉ Π’Π§ΠΠ’ Π² Π²ΠΎΠ·ΡΠ°ΡΡΠ΅ 18β55 Π»Π΅Ρ (ΡΡΠΎΠ²Π΅Π½Ρ ΡΠΎΠ·Π½Π°Π½ΠΈΡ ΠΏΡΠΈ ΠΏΠΎΡΡΡΠΏΠ»Π΅Π½ΠΈΠΈ Π² ΡΡΠ°ΡΠΈΠΎΠ½Π°Ρ 6Β±2 Π±Π°Π»Π»Π° ΠΏΠΎ Π¨ΠΠ), Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠΈΠΌ Π°Π½Π°Π»ΠΈΠ·ΠΎΠΌ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ Π½Π΅ΠΉΡΠΎΠ½ΡΠΏΠ΅ΡΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅ΠΈΠ½Π° S-100Π Π² ΡΡΠ²ΠΎΡΠΎΡΠΊΠ΅ ΠΊΡΠΎΠ²ΠΈ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈ ΠΎΠ±ΡΡΠΆΠ΄Π΅Π½ΠΈΠ΅. ΠΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΡ ΠΌΠ°ΡΠΊΠ΅ΡΠ° ΠΊΠ»Π΅ΡΠΎΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΏΠΎΠ²ΡΡΠ°Π»Π°ΡΡ Π² ΠΎΡΡΡΠΎΠΌ ΠΏΠ΅ΡΠΈΠΎΠ΄Π΅ ΡΠ΅ΡΠ΅ΠΏΠ½ΠΎ-ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ ΡΡΠ°Π²ΠΌΡ. ΠΡΠΈ Π±Π»Π°Π³ΠΎΠΏΡΠΈΡΡΠ½ΠΎΠΌ ΡΠ΅ΡΠ΅Π½ΠΈΠΈ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΡΡΠΎΠ²Π΅Π½Ρ S-100Π Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΡΠ½ΠΈΠΆΠ°Π»ΡΡ ΡΠΆΠ΅ Π½Π° 2-Π΅ ΡΡΡΠΊΠΈ Π±ΠΎΠ»Π΅Π·Π½ΠΈ. ΠΡΠΈ ΠΎΡΡΠΈΡΠ°ΡΠ΅Π»ΡΠ½ΠΎΠΉ Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠ΅ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΡ S-100Π ΠΎΡΡΠ°Π²Π°Π»Π°ΡΡ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ΠΈΠ·ΠΌΠ΅Π½Π½ΠΎΠΉ ΠΈΠ»ΠΈ Π΄Π°ΠΆΠ΅ ΠΏΠΎΠ²ΡΡΠ°Π»Π°ΡΡ, ΡΡΠΎ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΠΎΠ²Π°Π»ΠΎ ΠΎ Π²ΡΠΎΡΠΈΡΠ½ΡΡ
ΡΠ΅ΠΏΠ΅ΡΡΡΠ·ΠΈΠΎΠ½Π½ΡΡ
ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΡΡ
Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π°. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΡΠ΅Π΄Π½ΠΈΠ΅ Π·Π½Π°ΡΠ΅Π½ΠΈΡ Π½Π°ΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΡΠΎΠ²Π½Ρ ΠΌΠ°ΡΠΊΠ΅ΡΠ° ΡΠ°Π·Π»ΠΈΡΠ°Π»ΠΈΡΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ Π²ΠΈΠ΄Π° Π§ΠΠ’, Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΠ’, ΠΏΡΠΈΡΠ΅ΠΌ Π½Π°ΠΈΠ±ΠΎΠ»ΡΡΠΈΠ΅ ΡΠΈΡΡΡ ΠΎΡΠΌΠ΅ΡΠ°Π»ΠΈΡΡ Π² Π³ΡΡΠΏΠΏΠ°Ρ
, Π³Π΄Π΅ Π²ΡΡΠ²Π»ΡΠ»ΠΎΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠ΅ ΠΏΠΎΠ²ΡΠ΅ΠΆΠ΄Π΅Π½ΠΈΠ΅ ΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ. ΠΠ»ΡΡΠ΅Π²ΡΠ΅ ΡΠ»ΠΎΠ²Π°: ΡΡΠΆΠ΅Π»Π°Ρ ΡΠ΅ΡΠ΅ΠΏΠ½ΠΎ-ΠΌΠΎΠ·Π³ΠΎΠ²Π°Ρ ΡΡΠ°Π²ΠΌΠ°, ΠΏΡΠΎΠ³Π½ΠΎΠ·, Π±Π΅Π»ΠΎΠΊ S-100Π
Quantum Gravity in Everyday Life: General Relativity as an Effective Field Theory
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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