340 research outputs found
Universal sextic effective interaction at criticality
The renormalization group approach in three dimensions is used to estimate
the universal critical value g_6^* of the dimensionless sextic effective
coupling constant for the Ising model. The four-loop RG expansion for g_6 is
calculated and resummed by means of the Pade-Borel and Pade-Borel-Leroy
procedures resulting in g_6^* = 1.596, while the most accurate estimate for
g_6^* is argued to be equal to 1.61.Comment: 6 pages, TeX, no figure
Energy State of a Plastically Deformed Surface Layer
AbstractThe paper reports the results of experimental research on the substantiation of the criterion for steel strengthening effectiveness established on a basis of an energetic approach to the consideration of the mechanism for the surface layer formation with dynamic methods of plastic forming. Using the analogy between the processes of energy absorption of the crystal lattice under mechanical loading and under heating, the work demonstrates that the maximum specific energy which can absorb the crystal lattice corresponds to the value equal to the difference between the heat content (enthalpy) of the material in the solid state, at the melting temperature and enthalpy H_TS at 2930Π. The proposed method and experimental device allowing to estimate the stored energy in the plastically deformed surface layer as the difference between the work expended in plastic deformation of the material and the quantity of the released heat. It was established that the energy growth limit in the local plastically deformed volume of a surface occurs at making of 11-13 acts of the action force; the further increase in acts influences the energy state of the surface as it becomes stabilized
Exciton Lines in Luminescence Spectra of NixZn1-xO under Inner Shell Excitation
AbstractThe paper presents the results of the study of two narrow luminescence lines I1 and I2 at the energies of 3.339 and 3.393eV respectively in NiO and solid state solution Ni0.6Zn0.4O. The luminescence spectroscopy with a sub-nanosecond time resolution upon selective photoexcitation in the energy range of absorption of the inner shells Zn M- and Ni L2,3- edges of Zn- and Ni- ions was used to promote proposed earlier mechanism of origin of luminescence lines I1 and I2. Photoluminescence decay kinetics of NiO and solid state solution Ni0.6Zn0.4O under soft x-ray excitation are discussed. The doublet of I1 and I2 lines is believed to arise due to the radiative annihilation of p-d excitons
Electron transport in a quasi-one dimensional channel on suspended helium films
Quasi-one dimensional electron systems have been created using a suspended
helium film on a structured substrate. The electron mobility along the channel
is calculated by taking into account the essential scattering processes of
electrons by helium atoms in the vapor phase, ripplons, and surface defects of
the film substrate. It is shown that the last scattering mechanism may dominate
the electron mobility in the low temperature limit changing drastically the
temperature dependence of the mobility in comparison with that controlled by
the electron-ripplon scattering.Comment: 4 pages, 1 figur
Isotropy Properties of the Multi-Step Markov Symbolic Sequences
A new object of the probability theory, the two-sided chain of symbols
(introduced in Ref. arXiv:physics/0306170) is used to study isotropy properties
of binary multi-step Markov chains with the long-range correlations.
Established statistical correspondence between the Markov chains and certain
two-sided sequences allows us to prove the isotropy properties of three classes
of the Markov chains. One of them is the important class of weakly correlated
additive Markov chains, which turned out to be equivalent to the additive
two-sided sequences.Comment: 7 page
Reducing nonideal to ideal coupling in random matrix description of chaotic scattering: Application to the time-delay problem
We write explicitly a transformation of the scattering phases reducing the
problem of quantum chaotic scattering for systems with M statistically
equivalent channels at nonideal coupling to that for ideal coupling. Unfolding
the phases by their local density leads to universality of their local
fluctuations for large M. A relation between the partial time delays and
diagonal matrix elements of the Wigner-Smith matrix is revealed for ideal
coupling. This helped us in deriving the joint probability distribution of
partial time delays and the distribution of the Wigner time delay.Comment: 4 pages, revtex, no figures; published versio
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΎΠΏΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠ³ΠΎ Π΄Π°ΡΡΠΈΠΊΠ° ΡΠ³Π»ΠΎΠ²ΡΡ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π³Π»ΡΠ±ΠΎΠΊΠΎΠΉ ΠΎΡΡΠ°ΠΆΠ°ΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΠ°Π·ΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠ΅ΡΡΡΠΊΠΈ
An optoelectronic device for measurements of small angular displacements based on a diffraction of a laser beam on a deep reflective phasetype grating was suggested and investigated. The grating's depth is about several wavelengths. The zero diffraction order's power dependency on the incident angle of a laser beam was investigated theoretically and experimentally. There were found conditions when linear conversion of angular vibrations into changes of power of zero order took place. The experimentally measured sensitivity of the device was rad with channel bandwidth of 800 Hz and signal-to-noise ratio 10.ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ ΠΎΠΏΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΡΠΉ Π΄Π°ΡΡΠΈΠΊ ΠΌΠ°Π»ΡΡ
ΡΠ³Π»ΠΎΠ²ΡΡ
ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΡΠΊΠ° Π½Π° Π³Π»ΡΠ±ΠΎΠΊΠΎΠΉ ΠΎΡΡΠ°ΠΆΠ°ΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΠ°Π·ΠΎΠ²ΠΎΠΉ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠ΅ΡΡΡΠΊΠ΅. ΠΡΠΎΠ²Π΅Π΄ΡΠ½ ΡΠ΅ΠΎΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ Π΄Π°ΡΡΠΈΠΊΠ°
ΠΠΈΠΊΡΠΎΠ²Π΅Π·ΠΈΠΊΡΠ»Ρ Π»Π΅ΠΉΠΊΠΎΡΠΈΡΠ°ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΠΈΡΡ ΠΎΠΆΠ΄Π΅Π½ΠΈΡ
Microvesicles are a new field of biological research. They are subcellular structures ranging in size from 100 to 1000 nm and found in practically all human biological fluids. Their sources are different cells. Microvesicles have a diverse internal composition and carry a wide spectrum of molecules on their surface, which determines their participation in physiological and pathological processes. Their assumed role of biological markers of diseases has aroused great interest. At the present time, there is a lot of data in the world literature about microvesicles of platelets and endothelial cells, and there is practically no data about microvesicles of leukocytes. In this regard, the purpose of the given review was to summarize the data about microvesicles of leukocytes. The review presents data about source cells, internal and superficial composition of leukocytesβ microvesicles, their interaction with various cells, and involvement in physiological and pathological processes. Further study of microvesicles will make it possible to clarify their role in normal and pathological conditions, the possibility of using them as vectors of diseases and carriers of various biologically active molecules.ΠΠΈΠΊΡΠΎΠ²Π΅Π·ΠΈΠΊΡΠ»Ρ β Π½ΠΎΠ²ΡΠΉ ΠΎΠ±ΡΠ΅ΠΊΡ Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ. ΠΠ½ΠΈ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡ ΡΠΎΠ±ΠΎΠΉ ΡΡΠ±ΠΊΠ»Π΅ΡΠΎΡΠ½ΡΠ΅ ΡΡΡΡΠΊΡΡΡΡ ΡΠ°Π·ΠΌΠ΅ΡΠΎΠΌ ΠΎΡ 100 Π΄ΠΎ 1000 Π½ΠΌ ΠΈ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½Ρ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π²ΠΎ Π²ΡΠ΅Ρ
Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΆΠΈΠ΄ΠΊΠΎΡΡΡΡ
ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°. ΠΡ
ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ°ΠΌΠΈ ΡΠ²Π»ΡΡΡΡΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ ΠΊΠ»Π΅ΡΠΊΠΈ ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌΠ°. ΠΠΈΠΊΡΠΎΠ²Π΅Π·ΠΈΠΊΡΠ»Ρ ΠΎΠ±Π»Π°Π΄Π°ΡΡ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·Π½ΡΠΌ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠΌ ΡΠΎΡΡΠ°Π²ΠΎΠΌ ΠΈ Π½Π΅ΡΡΡ ΡΠΈΡΠΎΠΊΠΈΠΉ ΡΠΏΠ΅ΠΊΡΡ ΠΌΠΎΠ»Π΅ΠΊΡΠ» Π½Π° ΡΠ²ΠΎΠ΅ΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ, ΡΡΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅Ρ ΠΈΡ
ΡΡΠ°ΡΡΠΈΠ΅ Π² ΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΎΡΠ΅ΡΡΠ°Ρ
. ΠΡΠ΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅ΡΡΡ ΠΈΡ
ΡΠΎΠ»Ρ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠ°ΡΠΊΠ΅ΡΠΎΠ² Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ, ΡΠ΅ΠΌ ΠΈ ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»Π΅Π½ ΠΈΠ½ΡΠ΅ΡΠ΅Ρ ΠΊ Π½ΠΈΠΌ. Π Π½Π°ΡΡΠΎΡΡΠ΅Π΅ Π²ΡΠ΅ΠΌΡ Π² ΠΌΠΈΡΠΎΠ²ΠΎΠΉ Π»ΠΈΡΠ΅ΡΠ°ΡΡΡΠ΅ Π΄ΠΎΡΡΠ°ΡΠΎΡΠ½ΠΎ ΠΌΠ½ΠΎΠ³ΠΎ Π΄Π°Π½Π½ΡΡ
o ΠΌΠΈΠΊΡΠΎΠ²Π΅Π·ΠΈΠΊΡΠ»Π°Ρ
ΡΡΠΎΠΌΠ±ΠΎΡΠΈΡΠΎΠ² ΠΈ ΡΠ½Π΄ΠΎΡΠ΅Π»ΠΈΠ°Π»ΡΠ½ΡΡ
ΠΊΠ»Π΅ΡΠΎΠΊ, ΠΏΡΠΈ ΡΡΠΎΠΌ Π΄Π°Π½Π½ΡΡ
o ΠΌΠΈΠΊΡΠΎΠ²Π΅Π·ΠΈΠΊΡΠ»Π°Ρ
Π»Π΅ΠΉΠΊΠΎΡΠΈΡΠΎΠ² ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅Ρ. Π ΡΠ²ΡΠ·ΠΈ c ΡΡΠΈΠΌ ΡΠ΅Π»ΡΡ Π½Π°ΡΡΠΎΡΡΠ΅Π³ΠΎ ΠΎΠ±Π·ΠΎΡΠ° Π±ΡΠ»ΠΎ ΡΡΠΌΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π΄Π°Π½Π½ΡΡ
o ΠΌΠΈΠΊΡΠΎΠ²Π΅Π·ΠΈΠΊΡΠ»Π°Ρ
Π»Π΅ΠΉΠΊΠΎΡΠΈΡΠΎΠ². Π ΠΎΠ±Π·ΠΎΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ Π΄Π°Π½Π½ΡΠ΅ o ΠΊΠ»Π΅ΡΠΊΠ°Ρ
-ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ°Ρ
, Π²Π½ΡΡΡΠ΅Π½Π½Π΅ΠΌ ΠΈ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ½ΠΎΠΌ ΡΠΎΡΡΠ°Π²Π΅ ΠΌΠΈΠΊΡΠΎΠ²Π΅Π·ΠΈΠΊΡΠ» Π»Π΅ΠΉΠΊΠΎΡΠΈΡΠΎΠ², ΠΈΡ
Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠΈ Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ ΠΊΠ»Π΅ΡΠΊΠ°ΠΌΠΈ ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌΠ°, Π²ΠΎΠ²Π»Π΅ΡΠ΅Π½Π½ΠΎΡΡΠΈ Π² ΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ. ΠΠ°Π»ΡΠ½Π΅ΠΉΡΠ΅Π΅ ΠΈΠ·ΡΡΠ΅Π½ΠΈΠ΅ ΠΌΠΈΠΊΡΠΎΠ²Π΅Π·ΠΈΠΊΡΠ» ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ ΡΡΠΎΡΠ½ΠΈΡΡ ΠΈΡ
ΡΠΎΠ»Ρ Π² Π½ΠΎΡΠΌΠ΅ ΠΈ ΠΏΡΠΈ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΡ
, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π² ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅ ΠΌΠ°ΡΠΊΠ΅ΡΠΎΠ² Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠΉ ΠΈ ΠΏΠ΅ΡΠ΅Π½ΠΎΡΡΠΈΠΊΠΎΠ² ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈ Π°ΠΊΡΠΈΠ²Π½ΡΡ
ΠΌΠΎΠ»Π΅ΠΊΡΠ»
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