485 research outputs found
Dynamics of Primordial Hydrogen Recombination with Allowance for a Recoil for Scattering in the Ly-alpha Line
It is shown that taking into account a recoil for radiation scattering in the
Ly-alpha line can lead to a noticable acceleration of primordial hydrogen
recombination. Thus for LambdaCDM model a decrease of ionization degree exceeds
1% for redshifts z in a range 800 - 1050 achieving approximately 1.3% at z=900.
Corresponding corrections to the cosmic microwave background power spectra can
achieve 1.1% for TT spectra and 1.7% for EE ones. Radiative transfer in these
calculations was treated in a quasistationary approximation. Numerical
solutions are also obtained in diffusion approximation for a nonstationary
problem of Ly-alpha line radiative transfer under partial frequency
redistribution with a recoil. An evolution of a local line profile is traced to
as well as an evolution of a relative number of uncompensated transitions from
2p state down to 1s one. It is shown that taking into account nonstationarity
of Ly-alpha line radiative transfer can lead to an additional acceleration of
primordial hydrogen recombination.Comment: 9 pages, 5 figures; accepted for publication in Astronomy Letter
Optical Absorption and Raman Spectroscopy Study of the Fluorinated Double-Wall Carbon Nanotubes
Double-wall carbon nanotube (DWNT) samples have been fluorinated at room temperature with varied concentration of a fluorinating agent BrF3. Content of the products estimated from X-ray photoelectron data was equal to CF0.20 and CF0.29 in the case of deficit and excess of BrF3. Raman spectroscopy showed considerable decrease of carbon nanotube amount in the fluorinated samples. Analysis of optical absorption spectra measured for pristine and fluorinated DWNT samples revealed a selectivity of carbon nanotube fluorination. Nanotubes with large chiral angle are more inert to the fluorinating agent used
Two-Photon 2s<->1s Transitions during Recombination of Hydrogen in the Universe
Based on the standard cosmological model, we calculate the correction to the
rate of two-photon 2s1s transitions in the hydrogen atom under primordial
hydrogen plasma recombination conditions that arises when the induced
transitions under equilibrium background radiation with a blackbody spectrum
and plasma recombination radiation are taken into account.Comment: 20 pages, 9 figure
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
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
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
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
Geophysical studies with laser-beam detectors of gravitational waves
The existing high technology laser-beam detectors of gravitational waves may
find very useful applications in an unexpected area - geophysics. To make
possible the detection of weak gravitational waves in the region of high
frequencies of astrophysical interest, ~ 30 - 10^3 Hz, control systems of laser
interferometers must permanently monitor, record and compensate much larger
external interventions that take place in the region of low frequencies of
geophysical interest, ~ 10^{-5} - 3 X 10^{-3} Hz. Such phenomena as tidal
perturbations of land and gravity, normal mode oscillations of Earth,
oscillations of the inner core of Earth, etc. will inevitably affect the
performance of the interferometers and, therefore, the information about them
will be stored in the data of control systems. We specifically identify the
low-frequency information contained in distances between the interferometer
mirrors (deformation of Earth) and angles between the mirrors' suspensions
(deviations of local gravity vectors and plumb lines). We show that the access
to the angular information may require some modest amendments to the optical
scheme of the interferometers, and we suggest the ways of doing that. The
detailed evaluation of environmental and instrumental noises indicates that
they will not prevent, even if only marginally, the detection of interesting
geophysical phenomena. Gravitational-wave instruments seem to be capable of
reaching, as a by-product of their continuous operation, very ambitious
geophysical goals, such as observation of the Earth's inner core oscillations.Comment: 29 pages including 8 figures, modifications and clarifications in
response to referees' comments, to be published in Class. Quant. Gra
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