385 research outputs found
Process based model sheds light on climate sensitivity of Mediterranean tree-ring width
We use the process-based VS (Vaganov-Shashkin) model to investigate whether a regional <i>Pinus halepensis</i> tree-ring chronology from Tunisia can be simulated as a function of climate alone by employing a biological model linking day length and daily temperature and precipitation (AD 1959β2004) from a climate station to ring-width variations. We check performance of the model on independent data by a validation exercise in which the model's parameters are tuned using data for 1982β2004 and the model is applied to generate tree-ring indices for 1959β1981. The validation exercise yields a highly significant positive correlation between the residual chronology and estimated growth curve (<i>r</i>=0.76 <i>p</i><0.0001, <i>n</i>=23). The model shows that the average duration of the growing season is 191 days, with considerable variation from year to year. On average, soil moisture limits tree-ring growth for 128 days and temperature for 63 days. Model results depend on chosen values of parameters, in particular a parameter specifying a balance ratio between soil moisture and precipitation. Future work in the Mediterranean region should include multi-year natural experiments to verify patterns of cambial-growth variation suggested by the VS model
Effects of CMB temperature uncertainties on cosmological parameter estimation
We estimate the effect of the experimental uncertainty in the measurement of
the temperature of the cosmic microwave background (CMB) on the extraction of
cosmological parameters from future CMB surveys. We find that even for an ideal
experiment limited only by cosmic variance up to l = 2500 for both the
temperature and polarisation measurements, the projected cosmological parameter
errors are remarkably robust against the uncertainty of 1 mK in the FIRAS
instrument's CMB temperature monopole measurement. The maximum degradation in
sensitivity is 20%, for the baryon density estimate, relative to the case in
which the monopole is known infinitely well. While this degradation is
acceptable, we note that reducing the uncertainty in the current temperature
measurement by a factor of five will bring it down to the per cent level. We
also estimate the effect of the uncertainty in the dipole temperature
measurement. Assuming the overall calibration of the data to be dominated by
the dipole error of 0.2% from FIRAS, the sensitivity degradation is
insignificant and does not exceed 10% in any parameter direction.Comment: 12 pages, 2 figures, uses iopart.cls, v2: added discussion of CMB
dipole uncertainty, version accepted by JCA
Elastic Spin Relaxation Processes in Semiconductor Quantum Dots
Electron spin decoherence caused by elastic spin-phonon processes is
investigated comprehensively in a zero-dimensional environment. Specifically, a
theoretical treatment is developed for the processes associated with the
fluctuations in the phonon potential as well as in the electron procession
frequency through the spin-orbit and hyperfine interactions in the
semiconductor quantum dots. The analysis identifies the conditions (magnetic
field, temperature, etc.) in which the elastic spin-phonon processes can
dominate over the inelastic counterparts with the electron spin-flip
transitions. Particularly, the calculation results illustrate the potential
significance of an elastic decoherence mechanism originating from the
intervalley transitions in semiconductor quantum dots with multiple equivalent
energy minima (e.g., the X valleys in SiGe). The role of lattice anharmonicity
and phonon decay in spin relaxation is also examined along with that of the
local effective field fluctuations caused by the stochastic electronic
transitions between the orbital states. Numerical estimations are provided for
typical GaAs and Si-based quantum dots.Comment: 57 pages, 14 figure
Atmospheric Gravity Perturbations Measured by Ground-Based Interferometer with Suspended Mirrors
A possibility of geophysical measurements using the large scale laser
interferometrical gravitational wave antenna is discussed. An interferometer
with suspended mirrors can be used as a gradiometer measuring variations of an
angle between gravity force vectors acting on the spatially separated
suspensions. We analyze restrictions imposed by the atmospheric noises on
feasibility of such measurements. Two models of the atmosphere are invoked: a
quiet atmosphere with a hydrostatic coupling of pressure and density and a
dynamic model of moving region of the density anomaly (cyclone). Both models
lead to similar conclusions up to numerical factors. Besides the hydrostatic
approximation, we use a model of turbulent atmosphere with the pressure
fluctuation spectrum f^{-7/3} to explore the Newtonian noise in a higher
frequency domain (up to 10 Hz) predicting the gravitational noise background
for modern gravitational wave detectors. Our estimates show that this could
pose a serious problem for realization of such projects. Finally, angular
fluctuations of spatially separated pendula are investigated via computer
simulation for some realistic atmospheric data giving the level estimate
10^{-11} rad/sqrt(Hz) at frequency 10^{-4} Hz. This looks promising for the
possibility of the measurement of weak gravity effects such as Earth inner core
oscillations.Comment: 13 pages, 4 pigures, LaTeX. To be published in Classical and Quantum
Gravit
ΠΠ½Π΄ΠΎΠ²Π°ΡΠΊΡΠ»ΡΡΠ½ΡΠ΅ ΠΌΠ΅ΡΠΎΠ΄Ρ Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ½ΡΡΠ»ΡΡΠ°
Highlights. Mechanical thrombectomy is the βgold standardβ treatment of patients with large-vessel occlusions. Five randomized trials conducted in 2015 made a significant contribution to the development and introduction of mechanical thrombectomy into clinical practice. The DAWN and DEFUSE-3 trials have provided new insights into the pathophysiology of ischemic stroke and ensured the advancement in the therapeutic field.Abstract. Stroke is one of the leading causes of death and disability worldwide. The general strategy for the treatment of ischemic stroke is aimed at restoring blood flow to the ischemic regions of the brain. Intravenous thrombolysis has been the treatment for acute ischemic stroke since 1996. However, since 2015, as a result of 5 randomized trials, endovascular mechanical thrombectomy has become the gold standard for the treatment of patients with large cerebral artery occlusion. The DAWN and DEFUSE 3 trials have provided new insights into the pathophysiology of ischemic stroke, shifting the paradigm from βtime = brainβ to βcollaterals = brainβ. In this article, the authors will consider development of endovascular devices, modern mechanical thrombectomy techniques, and directions for further research of endovascular treatment for ischemic stroke.ΠΡΠ½ΠΎΠ²Π½ΡΠ΅ ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΡ. ΠΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΡΠΎΠΌΠ±ΡΠΊΡΡΡΠ°ΠΊΡΠΈΡ β Β«Π·ΠΎΠ»ΠΎΡΠΎΠΉ ΡΡΠ°Π½Π΄Π°ΡΡΒ» Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΎΠΊΠΊΠ»ΡΠ·ΠΈΠ΅ΠΉ ΠΊΡΡΠΏΠ½ΡΡ
ΡΠ΅ΡΠ΅Π±ΡΠ°Π»ΡΠ½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ. ΠΠ½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΡΠΉ Π²ΠΊΠ»Π°Π΄ Π² ΡΠ°Π·Π²ΠΈΡΠΈΠ΅ ΠΈ Π²Π½Π΅Π΄ΡΠ΅Π½ΠΈΠ΅ Π² ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΡΡ ΠΏΡΠ°ΠΊΡΠΈΠΊΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠΎΠΌΠ±ΡΠΊΡΡΡΠ°ΠΊΡΠΈΠΈ Π²Π½Π΅ΡΠ»ΠΈ ΠΏΡΡΡ ΡΠ°Π½Π΄ΠΎΠΌΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ, ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Π½ΡΡ
Π² 2015 Π³. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ DAWN ΠΈ DEFUSE 3 ΠΎΡΠΊΡΡΠ»ΠΈ Π½ΠΎΠ²ΠΎΠ΅ ΠΏΠΎΠ½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΠΏΠ°ΡΠΎΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ½ΡΡΠ»ΡΡΠ° ΠΈ ΡΠ°ΡΡΠΈΡΠ΅Π½ΠΈΡ ΡΠ΅ΡΠ°ΠΏΠ΅Π²ΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΠΊΠ½Π°.Π Π΅Π·ΡΠΌΠ΅. ΠΠ½ΡΡΠ»ΡΡ β ΠΎΠ΄Π½Π° ΠΈΠ· Π³Π»Π°Π²Π½ΡΡ
ΠΏΡΠΈΡΠΈΠ½ ΡΠΌΠ΅ΡΡΠ½ΠΎΡΡΠΈ ΠΈ ΠΈΠ½Π²Π°Π»ΠΈΠ΄ΠΈΠ·Π°ΡΠΈΠΈ Π½Π°ΡΠ΅Π»Π΅Π½ΠΈΡ Π²ΠΎ Π²ΡΠ΅ΠΌ ΠΌΠΈΡΠ΅. ΠΠ±ΡΠ°Ρ ΡΡΡΠ°ΡΠ΅Π³ΠΈΡ ΡΠ΅ΡΠ°ΠΏΠ΅Π²ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠ΅Ρ ΠΏΡΠΈ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΈΠ½ΡΡΠ»ΡΡΠ΅ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½Π° Π½Π° Π²ΠΎΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΈΠ΅ ΠΊΡΠΎΠ²ΠΎΡΠΎΠΊΠ° Π² ΠΈΡΠ΅ΠΌΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΠ΅ ΠΎΡΠ΄Π΅Π»Ρ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π°. Π‘ 1996 Π³. Π²Π½ΡΡΡΠΈΠ²Π΅Π½Π½Π°Ρ ΡΡΠΎΠΌΠ±ΠΎΠ»ΠΈΡΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠ΅ΡΠ°ΠΏΠΈΡ Π±ΡΠ»Π° ΠΏΠ΅ΡΠ²ΠΎΠΉ Π»ΠΈΠ½ΠΈΠ΅ΠΉ Π»Π΅ΡΠ΅Π½ΠΈΡ Π±ΠΎΠ»ΡΠ½ΡΡ
ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΈΠ½ΡΡΠ»ΡΡΠΎΠΌ. ΠΠ΄Π½Π°ΠΊΠΎ Ρ 2015 Π³. Π½Π° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΏΡΡΠΈ ΡΠ°Π½Π΄ΠΎΠΌΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Β«Π·ΠΎΠ»ΠΎΡΡΠΌ ΡΡΠ°Π½Π΄Π°ΡΡΠΎΠΌΒ» Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΎΠΊΠΊΠ»ΡΠ·ΠΈΠ΅ΠΉ ΠΊΡΡΠΏΠ½ΡΡ
ΡΠ΅ΡΠ΅Π±ΡΠ°Π»ΡΠ½ΡΡ
Π°ΡΡΠ΅ΡΠΈΠΉ ΡΡΠ°Π»Π° ΡΠ½Π΄ΠΎΠ²Π°ΡΠΊΡΠ»ΡΡΠ½Π°Ρ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΡΠΎΠΌΠ±ΡΠΊΡΡΡΠ°ΠΊΡΠΈΡ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ DAWN ΠΈ DEFUSE 3 ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΠΎΠ²Π°Π»ΠΈ Π½ΠΎΠ²ΠΎΠΌΡ ΠΏΠΎΠ½ΠΈΠΌΠ°Π½ΠΈΡ ΠΏΠ°ΡΠΎΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ½ΡΡΠ»ΡΡΠ° ΡΠΎ ΡΠΌΠ΅Π½ΠΎΠΉ ΠΏΠ°ΡΠ°Π΄ΠΈΠ³ΠΌΡ Β«Π²ΡΠ΅ΠΌΡ β ΠΌΠΎΠ·Π³Β» Π½Π° Β«ΠΊΠΎΠ»Π»Π°ΡΠ΅ΡΠ°Π»ΠΈ β ΠΌΠΎΠ·Π³Β». Π Π΄Π°Π½Π½ΠΎΠΉ ΡΡΠ°ΡΡΠ΅ ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Ρ ΡΡΠ°ΠΏΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠ½Π΄ΠΎΠ²Π°ΡΠΊΡΠ»ΡΡΠ½ΡΡ
ΡΡΡΡΠΎΠΉΡΡΠ², ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΠ΅ ΡΠ΅Ρ
Π½ΠΈΠΊΠΈ ΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΠΎΠΌΠ±ΡΠΊΡΡΡΠ°ΠΊΡΠΈΠΈ, Π° ΡΠ°ΠΊΠΆΠ΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠ΅ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅Π³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ½Π΄ΠΎΠ²Π°ΡΠΊΡΠ»ΡΡΠ½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² Π»Π΅ΡΠ΅Π½ΠΈΡ ΠΈΡΠ΅ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈΠ½ΡΡΠ»ΡΡΠ°
SiPM-based azimuthal position sensor in ANITA-IV Hi-Cal Antarctic balloon experiment
Hi-Cal (High-Altitude Calibration) is a balloon-borne experiment that will be launched in December, 2016 in Antarctica following ANITA-IV (Antarctic Impulsive Transient Antenna) and will generate a broad-band pulse over the frequency range expected from radiation induced by a cosmic ray shower. Here, we describe a device based on an array of silicon photomultipliers (SiPMs) for determination of the azimuthal position of Hi-Cal. The angular resolution of the device is about 3 degrees. Since at the float altitude of ~38 km the pressure will be ~0.5 mbar and temperature ~ β 20 Β°C, the equipment has been tested in a chamber over a range of corresponding pressures (0.5 Γ· 1000) mbar and temperatures (β40 Γ· +50) Β°C
Π Π΅Π°ΠΊΡΠΈΡ ΠΏΡΠ΅Π΄Π²Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π½Π°Π³ΡΡΠΆΠ΅Π½Π½ΠΎΠΉ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΈ Π²ΡΠ°ΡΠ΅Π½ΠΈΡ Ρ ΠΆΠ΅ΡΡΠΊΠΎΠΉ Π½ΠΎΡΠΎΠ²ΠΎΠΉ ΡΠ°ΡΡΡΡ Π°ΠΏΠΏΠ°ΡΠ°ΡΠ° Π½Π° ΡΠ΄Π°ΡΠ½ΡΡ Π²ΠΎΠ»Π½Ρ Π² ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ
The article investigates the problem of hydro-elastic interaction of a weak shock wave with a rigid nosed rotation shell preloaded with axial forces. The shell is enclosed in a rigid parabolic screen, i.e. the impact of the end face and the shock wave diffraction are not considered. Liquid is regarded to be perfectly compressible. Its applied summing hydrodynamic pressure during complex interaction with the shell surface can be classified into the incident, reflected and radiated waves. The problem of hydro-elastic interaction of these shock fronts with a preloaded parabolic rigid nosed shell in a related setting is reduced to the solution of the wave equations of nonlinear system of equations for shell motion under particular initial and boundary conditions, in which the dimensionless displacement of this nose section under the impact of hydrodynamic forces is determined by integrating its motion equation. The equations, describing the dependences of nose section displacements on shock wave interaction time, take into account generalized hydrodynamic forces, including the second category directly related to the mass of the attached fluid. Determination of stress-strain state in case of interaction with the shock wave in the liquid of elastic rotation paraboloid in the form of the shell containing a rigid insertion in the nose section is reduced to the solution of a nonlinear equations system of shell motion considering the boundary conditions along fastenings at the end face of the shell and interface conditions of the shell and insertion. Dimensionless displacements of the nose section caused by hydrodynamic forces are defined by integrating the equations of motion under the initial conditions along insertion offsets in the axial directions.Π ΡΡΠ°ΡΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΡΡΡ Π·Π°Π΄Π°ΡΠ° Π³ΠΈΠ΄ΡΠΎΡΠΏΡΡΠ³ΠΎΠ³ΠΎ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ ΡΠ»Π°Π±ΠΎΠΉ ΡΠ΄Π°ΡΠ½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ Ρ ΠΏΡΠ΅Π΄Π²Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π½Π°Π³ΡΡΠΆΠ΅Π½Π½ΠΎΠΉ ΠΎΡΠ΅Π²ΡΠΌΠΈ ΡΡΠΈΠ»ΠΈΡΠΌΠΈ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΎΠΉ Π²ΡΠ°ΡΠ΅Π½ΠΈΡ Ρ ΠΆΠ΅ΡΡΠΊΠΎΠΉ Π½ΠΎΡΠΎΠ²ΠΎΠΉ ΡΠ°ΡΡΡΡ. ΠΠ±ΠΎΠ»ΠΎΡΠΊΠ° Π·Π°ΠΊΠ»ΡΡΠ΅Π½Π° Π² ΠΆΠ΅ΡΡΠΊΠΈΠΉ ΠΏΠ°ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠΊΡΠ°Π½, ΡΠΎ Π΅ΡΡΡ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΡΠΎΡΡΠ° ΠΈ Π΄ΠΈΡΡΠ°ΠΊΡΠΈΡ ΡΠ΄Π°ΡΠ½ΠΎΠΉ Π²ΠΎΠ»Π½Ρ Π½Π΅ ΡΡΠΈΡΡΠ²Π°ΡΡΡΡ. ΠΠ΄Π΅Π°Π»ΡΠ½ΠΎ ΡΠΆΠΈΠΌΠ°Π΅ΠΌΠΎΠΉ ΡΡΠΈΡΠ°Π΅ΡΡΡ ΠΆΠΈΠ΄ΠΊΠΎΡΡΡ, ΠΏΠ΅ΡΠ΅Π΄Π°Π²Π°Π΅ΠΌΠΎΠ΅ ΠΏΠΎΠ»Π½ΠΎΠ΅ Π³ΠΈΠ΄ΡΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π΄Π°Π²Π»Π΅Π½ΠΈΠ΅ ΠΊΠΎΡΠΎΡΠΎΠΉ ΠΏΡΠΈ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠΌ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠΈ Ρ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΡ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΈ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΎ Π½Π° ΠΏΠ°Π΄Π°ΡΡΡΡ, ΠΎΡΡΠ°ΠΆΠ΅Π½Π½ΡΡ ΠΈ ΠΈΠ·Π»ΡΡΠ΅Π½Π½ΡΡ Π²ΠΎΠ»Π½Ρ. ΠΠ°Π΄Π°ΡΠ° Π³ΠΈΠ΄ΡΠΎΡΠΏΡΡΠ³ΠΎΠ³ΠΎ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ ΡΠΊΠ°Π·Π°Π½Π½ΡΡ
ΡΠ΄Π°ΡΠ½ΡΡ
ΡΡΠΎΠ½ΡΠΎΠ² Ρ Π½Π°Π³ΡΡΠΆΠ΅Π½Π½ΠΎΠΉ ΠΏΠ°ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΎΠΉ, ΠΈΠΌΠ΅ΡΡΠ΅ΠΉ ΠΆΠ΅ΡΡΠΊΡΡ Π½ΠΎΡΠΎΠ²ΡΡ ΡΠ°ΡΡΡ, Π² ΡΠ²ΡΠ·Π°Π½Π½ΠΎΠΉ ΠΏΠΎΡΡΠ°Π½ΠΎΠ²ΠΊΠ΅ ΡΠ²ΠΎΠ΄ΠΈΡΡΡ ΠΊ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π²ΠΎΠ»Π½ΠΎΠ²ΡΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ Π½Π΅Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΉ ΡΠΈΡΡΠ΅ΠΌΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΈ ΠΏΡΠΈ ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΡ
Π½Π°ΡΠ°Π»ΡΠ½ΡΡ
ΠΈ Π³ΡΠ°Π½ΠΈΡΠ½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΡΡ
, Π² ΠΊΠΎΡΠΎΡΡΡ
Π±Π΅Π·ΡΠ°Π·ΠΌΠ΅ΡΠ½ΠΎΠ΅ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΠ΅ ΡΡΠΎΠΉ Π½ΠΎΡΠΎΠ²ΠΎΠΉ ΡΠ°ΡΡΠΈ ΠΏΠΎΠ΄ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ Π³ΠΈΠ΄ΡΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΠ» ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ ΠΈΠ½ΡΠ΅Π³ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π΅Π΅ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ. Π£ΡΠ°Π²Π½Π΅Π½ΠΈΡ, ΠΎΠΏΠΈΡΡΠ²Π°ΡΡΠΈΠ΅ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ Π½ΠΎΡΠΎΠ²ΠΎΠΉ ΡΠ°ΡΡΠΈ ΠΎΡ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ Ρ ΡΠ΄Π°ΡΠ½ΠΎΠΉ Π²ΠΎΠ»Π½ΠΎΠΉ, ΡΡΠΈΡΡΠ²Π°ΡΡ ΠΎΠ±ΠΎΠ±ΡΠ΅Π½Π½ΡΠ΅ Π³ΠΈΠ΄ΡΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠΈΠ»Ρ, Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ Π²ΡΠΎΡΠΎΠΉ ΠΊΠ°ΡΠ΅Π³ΠΎΡΠΈΠΈ, Π½Π΅ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²Π΅Π½Π½ΠΎ ΡΠ²ΡΠ·Π°Π½Π½ΡΠ΅ Ρ ΠΌΠ°ΡΡΠΎΠΉ ΠΏΡΠΈΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½Π½ΠΎΠΉ ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ. ΠΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π½Π°ΠΏΡΡΠΆΠ΅Π½Π½ΠΎ-Π΄Π΅ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΎΡΡΠΎΡΠ½ΠΈΡ ΠΏΡΠΈ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΠΈ Ρ ΡΠ΄Π°ΡΠ½ΠΎΠΉ Π²ΠΎΠ»Π½ΠΎΠΉ Π² ΠΆΠΈΠ΄ΠΊΠΎΡΡΠΈ ΡΠΏΡΡΠ³ΠΎΠ³ΠΎ ΠΏΠ°ΡΠ°Π±ΠΎΠ»ΠΎΠΈΠ΄Π° Π²ΡΠ°ΡΠ΅Π½ΠΈΡ Π² Π²ΠΈΠ΄Π΅ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΈ, ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠ΅ΠΉ Π² Π½ΠΎΡΠΎΠ²ΠΎΠΉ ΡΠ°ΡΡΠΈ ΠΆΠ΅ΡΡΠΊΡΡ Π²ΡΡΠ°Π²ΠΊΡ, ΡΠ²ΠΎΠ΄ΠΈΡΡΡ ΠΊ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΡΠΈΡΡΠ΅ΠΌΡ Π½Π΅Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΈ Ρ ΡΡΠ΅ΡΠΎΠΌ Π³ΡΠ°Π½ΠΈΡΠ½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΠΏΠΎ Π·Π°ΠΊΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡΠΌ Π² ΡΠΎΡΡΠ΅ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΈ ΠΈ ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΡΠΎΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΈ ΠΈ Π²ΡΡΠ°Π²ΠΊΠΈ. ΠΠ΅Π·ΡΠ°Π·ΠΌΠ΅ΡΠ½ΡΠ΅ ΠΏΠ΅ΡΠ΅ΠΌΠ΅ΡΠ΅Π½ΠΈΡ Π½ΠΎΡΠΎΠ²ΠΎΠΉ ΡΠ°ΡΡΠΈ ΠΏΠΎΠ΄ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ΠΌ Π³ΠΈΠ΄ΡΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠΈΠ» ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΡΡ ΠΈΠ½ΡΠ΅Π³ΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΡ ΠΏΡΠΈ Π½Π°ΡΠ°Π»ΡΠ½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΠΏΠΎ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΡΠΌ Π²ΡΡΠ°Π²ΠΊΠΈ Π² ΠΎΡΠ΅Π²ΡΡ
Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡΡ
Thermal properties and structure of cast carbon-containing invar and superinvar alloys after two-stage annealing
The effect of carbon content on thermal properties of cast superinvar alloys subjected to two-stage annealing is studied. It is shown that carbon improves the casting properties of the alloys but raises the temperature coefficient of linear expansion (CTLE). Two-stage high-temperature annealing makes it possible to remove carbon from the solid solution and to transfer it into graphite, which is accompanied by decrease in the CTLE. Β© 2013 Springer Science+Business Media New York
HeII->HeI Recombination of Primordial Helium Plasma Including the Effect of Neutral Hydrogen
The HeII->HeI recombination of primordial helium plasma (z = 1500 - 3000) is
considered in terms of the standard cosmological model. This process affects
the formation of cosmic microwave background anisotropy and spectral
distortions. We investigate the effect of neutral hydrogen on the HeII->HeI
recombination kinetics with partial and complete redistributions of radiation
in frequency in the HeI resonance lines. It is shown that to properly compute
the HeII->HeI recombination kinetics, one should take into account not only the
wings in the absorption and emission profiles of the HeI resonance lines, but
also the mechanism of the redistribution of resonance photons in frequency.
Thus, for example, the relative difference in the numbers of free electrons for
the model using Doppler absorption and emission profiles and the model using a
partial redistribution in frequency is 1 - 1.3% for the epoch z = 1770 - 1920.
The relative difference in the numbers of free electrons for the model using a
partial redistribution in frequency and the model using a complete
redistribution in frequency is 1 - 3.8% for the epoch z = 1750 - 2350.Comment: 28 pages, 9 figures, 2 tabel
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