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Vol 42, No 11 (2016)

Article

Local burst model of CMB temperature fluctuations: Scattering in the resonance lines of primordial hydrogen and helium

Dubrovich V.K., Grachev S.I.

Abstract

The propagation of an instantaneous burst of isotropic radiation from the time of its onset at some redshift z0 to the time of its detection at the present epoch (at z = 0) is considered within the framework of a flat Universe. The Thomson scattering by free electrons and the scattering in the primordial hydrogen Lα and Lβ lines and in the He I 1s2–1s2p, 1s3p (1S–1P*) lines are taken into account. It is shown that the relative amplitude of the spectral distortions due to the scattering in these lines at the corresponding frequencies can be a factor of 103−104 greater than the maximum possible amplitude from the scattering in the subordinate hydrogen lines considered previously (Dubrovich and Grachev 2015). In the linear approximation in optical depth, the distortion profiles in the resonance lines turn out to be purely absorption ones and depend neither on the direction nor on the distance to the burst center, in contrast to the profiles in the subordinate lines. The profiles contain jumps at frequencies corresponding to the instant the source (burst) appears at a given redshift z0. For example, at z0 = 5000 the jumps in the hydrogen Lα and Lβ lines lie at frequencies of 493 and 584 GHz, respectively, while in the above two helium lines they lie at frequencies of 855 and 930 GHz at z0 = 6000. The relative magnitude of the jumps ranges from 10−4 to 3 × 10−3.

Astronomy Letters. 2016;42(11):713-720
pages 713-720 views

Galactic kinematics from data on open star clusters from the MWSC catalogue

Bobylev V.V., Bajkova A.T., Shirokova K.S.

Abstract

Open star clusters from the MWSC (Milky Way Star Clusters) catalogue have been used to determine the Galactic rotation parameters. The circular rotation velocity of the solar neighborhood around the Galactic center has been found from data on more than 2000 clusters of various ages to be V0 = 236 ± 6 km s−1 for the adopted Galactocentric distance of the Sun R0 = 8.3 ± 0.2 kpc. The derived angular velocity parameters are Ω0 = 28.48 ± 0.36 km s−1 kpc−1, Ω0 = −3.50 ± 0.08 km s−1 kpc−2, and Ω0 = 0.331 ± 0.037 km s−1 kpc−3. The influence of the spiral density wave has been detected only in the sample of clusters younger than 50 Myr. For these clusters the amplitudes of the tangential and radial velocity perturbations are fθ = 5.6 ± 1.6 km s−1 and fR = 7.7 ± 1.4 km s−1, respectively; the perturbation wavelengths are λθ = 2.6 ± 0.5 kpc (iθ = −11◦ ± 2◦) and λR = 2.1 ± 0.5 kpc (iR = −9◦ ± 2◦) for the adopted four-armed model (m = 4). The Sun’s phase in the spiral density wave is (χ)θ = −62◦ ± 9◦ and (χ)R = −85◦ ± 10◦ from the residual tangential and radial velocities, respectively.

Astronomy Letters. 2016;42(11):721-733
pages 721-733 views

Evolution of the titanium and oxygen abundances from observations of FGK dwarfs in a wide metallicity range

Sitnova T.M.

Abstract

For a sample of dwarf stars close to the Sun with well-known atmospheric parameters and an iron abundance in the range −2.6 < [Fe/H] < 0.2, we have determined the titanium and oxygen abundances by taking into account the departures from LTE. The dependence of the [O/Fe] and [Ti/Fe] abundance ratios on [Fe/H] has been refined in comparison with the published data. We have established that [O/Fe] increases from −0.2 to 0.6 as the metallicity [Fe/H] decreases from 0.2 to −0.8 and remains constant at a lower metallicity. A similar behavior has been found for [Ti/Fe], but the plateau is formed by stars with [Fe/H] > −0.7, and the titanium overabundance relative to iron is 0.3. The results confirm that not only oxygen but also titanium are synthesized in the α-process. Our data can be used to test the Galactic chemical evolution models.

Astronomy Letters. 2016;42(11):734-744
pages 734-744 views

Breakdown of the Goldreich–Julian relation in a neutron star

Sob’yanin D.N.

Abstract

The electromagnetic field in a magnetized neutron star and the underlying volume charges and currents are found. A general case of a rigidly rotating neutron star with infinite conductivity, arbitrary distribution of the internal magnetic field, arbitrarily changing angular velocity, and arbitrary surface velocity less than the velocity of light is considered. Quaternions are used to describe rotation and determine the magnetic field. It is shown that the charge density is not equal to and can exceed significantly the common Goldreich–Julian density. Moreover, corrections to the magnetic field due to stellar rotation are zero. For a rotating neutron star, twisting magnetic field lines causes charge accumulation and current flows. This fact shows a possible link between changing internal magnetic field topology and observed activity of neutron stars.

Astronomy Letters. 2016;42(11):745-751
pages 745-751 views

Oblique MHD shock near the surface of young stars

Dodin A.V.

Abstract

The dependence of the spectrum of a hot spot at the surface of accreting young stars on the angle at which the material falls onto the star is considered. For typical parameters of T Tauri stars the structure of the shock at oblique incidence has been found to be no different from its structure at normal incidence, but at the same time the inclination, along with the gas density and velocity, is shown to be an independent accretion parameter the changes in which lead to noticeable changes in the hot-spot spectrum.

Astronomy Letters. 2016;42(11):752-755
pages 752-755 views

Photometric and spectroscopic study of the supergiant with an infrared excess V1027 Cygni

Arkhipova V.P., Taranova O.G., Ikonnikova N.P., Esipov V.F., Komissarova G.V., Shenavrin V.I., Burlak M.A.

Abstract

We present the results of our UBV and JHKLM photometry for the semiregular pulsating variable V1027 Cyg, a supergiant with an infrared excess, over the period from 1997 to 2015 (UBV) and in 2009–2015 (JHKLM). Together with the new data, we analyze the photometric observations of V1027 Cyg that we have obtained and published previously. Our search for a periodicity in the UBV brightness variations has led to several periods from P = 212d to 320d in different time intervals. We have found the period P = 237d based on our infrared photometry. The variability amplitude, the lightcurve shape, and themagnitude of V1027 Cyg atmaximum light change noticeably from cycle to cycle. The deepest minimum was observed in 2011, when the amplitudes of brightness variations in the star reached the following values: ΔU = 1.m28, ΔB = 1.m10, ΔV = 1.m05, ΔJ = 0.m30, ΔH = 0.m35, ΔK = 0.m32, ΔL = 0.m26, and ΔM = 0.m10. An ambiguous correlation of the BV and UB colors with the brightness has been revealed. For example, a noticeable bluing of the star was observed during the deep 1992, 2008, and 2011 minima, while the variations with smaller amplitudes show an increase in B − V at the photometric minima. The spectral energy distribution for V1027 Cyg from our photometry in the range 0.36 (U)–5.0 (M) μm corresponds to spectral types from G8I to K3I at different phases of the pulsation cycle. Low-resolution spectra of V1027 Cyg in the range λ4400–9200 ˚A were taken during 16 nights over the period 1995–2015. At the 1995 and 2011 photometric minima the star’s spectrum exhibited molecular TiO bands whose intensity corresponded to spectral types M0–M1, while the photometric data point to a considerably earlier spectral type. We hypothesize that the TiO bands are formed in the upper layers of the extended stellar atmosphere. We have measured the equivalent widths of the strongest absorption lines, in particular, the infrared Ca II triplet in the spectrum of V1027 Cyg. The calcium triplet (Ca T) with Wλ(Ca T) = 20.3 ± 1.8 ˚A as a luminosity indicator for supergiants places V1027 Cyg in the region of the brightest G–K supergiants. V1027 Cyg has been identified with the infrared source IRAS 20004+2955 and is currently believed to be a candidate for post-AGB stars. The evolutionary status of the star and its difference from other post-AGB objects are discussed.

Astronomy Letters. 2016;42(11):756-773
pages 756-773 views

On the most typical structure of three-dimensional magnetic reconnection

Dumin Y.V., Somov B.V.

Abstract

Motivated by the problem of magnetic reconnection in turbulent astrophysical plasmas with a strong magnetic field, in particular, in solar flares, we have calculated the probability of occurrence of various topological structures of three-dimensional reconnection at the null point of a random magnetic field. We have established that the peculiar nonaxisymmetric structure with six asymptotic directions, the six-tailed structure, also called the improper radial null, plays a dominant role. All the remaining structures, in particular, the axisymmetric ones (the proper radial nulls), occur with a much lower probability. The fundamental feature of the six-tailed structure is that at large distances it is approximately reduced to the classical two-dimensional X-type structure.

Astronomy Letters. 2016;42(11):774-781
pages 774-781 views