


Vol 45, No 10 (2019)
- Year: 2019
- Articles: 6
- URL: https://journal-vniispk.ru/1063-7737/issue/view/12028
Article
New Gamma-Ray Bursts Found in the Archival Data from the IBIS/ISGRI Telescope of the INTEGRAL Observatory
Abstract
A systematic search for cosmic gamma-ray bursts (GRBs) and other short hard X-ray events in the archival data from the IBIS/ISGRI telescope of the INTEGRAL observatory over 2003–2018 has been carried out. Seven previously unknown GRBs have been recorded in the telescope field of view; all of them have been localized with an accuracy ≤2 arcmin. These events were not revealed by the INTEGRAL burst alert system (IBAS) designed for an automatic GRB search and alert. Four more such localized events missed by IBAS, but known previously, i.e., observed in other experiments, have been found. Eight hundred and eighty six GRBs outside the field of view that arrived at large angles to the IBIS/ISGRI axis have also been recorded. All of them were previously recorded in other experiments, primarily by the anticoincidence shield (ACS) of the SPI gamma-ray spectrometer onboard the INTEGRAL observatory, the PICsIT detector of the IBIS gamma-ray telescope, and the KONUS/WIND monitor. An order of magnitude more events without any confirmations in other experiments have been recorded. Both GRBs and solar flares or magnetospheric transient events can be among them. Catalogs with the basic parameters of confirmed and previously unknown cosmic GRBs recorded by the IBIS/ISGRI telescope have been compiled. The statistical distributions of bursts in various parameters have been constructed and investigated.



Radial Pulsations of Stars at the Stage of the Final Helium Flash
Abstract
Stellar evolution calculations were performed for population I stars with masses on the main sequence 1 M⊙ ≤ M0 ≤ 1.5 M⊙ up to the stage of a cooling white dwarf. The final helium flash LTP is shown to occur in post-AGB stars with initial masses 1.3 M⊙ ≤ M0 ≤ 1.32 M⊙ for the overshooting parameter f = 0.016. In the case of more effective overshooting (f = 0.018) the final helium flash occurs at initial masses 1.28 M⊙ ≤ M0 ≤ 1.3 M⊙. Fivefold variations of the mass loss rate parameter at the post-AGB stage do not affect the occurrence of the final helium flash, but lead to noticeable changes of the evolutionary time. Selected models of two evolutionary sequences with an initial mass M0 = 1.3 M⊙ and overshooting parameters f = 0.016 and f = 0.018 were used as initial conditions in solving the equations of hydrodynamics describing the radial oscillations of stars with effective temperatures Teff < 104 K. The maximum pulsation period Π = 117 days determined for the evolutionary sequence M0 = 1.3 M⊙, f = 0.016 is in a good agreement with observational estimates of the period of FG Sge. The mass, radius, and effective temperature of the star are M = 0.565 M⊙, R = 126R⊙ and Teff = 4445 K, respectively. At the same time, the average rate of change in the period of FG Sge from 1960 to 1990 exceeds its theoretical estimate approximately by a factor of 3.



Influence of Large-Scale Perturbations in Circumstellar Disks on the Linear Polarization Parameters of UX Ori Stars
Abstract
The influence of large-scale perturbations in a circumstellar disk on the linear polarization of UX Ori stars is considered. We show that the position angle of the intrinsic linear polarization of a star surrounded by a geometrically thin flared disk cannot change significantly after the passage through the photometric minimum due to perturbations in the disk. In contrast, perturbations in a disk puffed up in the dust sublimation zone can give deflections of the plane of linear polarization of the system’s radiation up to 60°. This model allows the unusual changes in linear polarization observed in UX Ori and WW Vul after prolonged photometric minima to be explained.



Search for Evolutionary Changes in the Periods of Cepheids: V532 Cyg
Abstract
For the low-amplitude Cepheid V532 Cyg we have constructed an O − C diagram spanning a time interval of 121 years. The O − C diagram has the shape of a parabola, which has made it possible to determine for the first time the quadratic light elements and to calculate the rate of evolutionary decrease in the period, dP/dt = −0.248 (±0.067) s yr−1, which points to the second crossing of the instability strip. The pulsation stability test proposed by Lombard and Koen (1993) has confirmed that the period decrease is real.



The Mass Distribution of Transiting Exoplanets Corrected for Observational Selection Effects
Abstract
The mass distribution of transiting exoplanets has been corrected for observational selection effects: the probability of a mass determination (for planets detected by the Kepler Space Telescope) and the probability of a transiting configuration. The corrected mass distribution of exoplanets can be fitted by a power law with an exponent of \( - 2_{ - 0.16}^{ + 0.1}:\;{\textstyle{{dN} \over {dm}}} \propto {m^{ - 2_{ - 0.16}^{ + 0.1}}}\). Two minima corresponding to 0.3–0.7 and 4–7 Jupiter masses have been revealed.



Features of the Gnevyshev-Waldmeier Rule for Various Lifetimes and Areas of Sunspot Groups
Abstract
Based on a sample of 7696 nonrecurrent and 566 recurrent sunspot groups, we have investigated the Gnevyshev–Waldmeier rule using the Catalogue of Solar Activity by R.S. Gnevysheva (1954–1978). The maximum recorded sunspot group lifetime is 160 days. The general Gnevyshev–Waldmeier rule for all lifetimes is Amax = (12.1 ± 0.70)LT (Amax is the maximum sunspot group area during the lifetime and LT is the sunspot group lifetime). However, the general rule has turned out to deviate from the derived linear form for the population of small short-living sunspot groups (SSG): it has a significant nonlinear scaling form Amax = (8.02 ± 0.41)LT(1.105±0.022). For the population of large long-living sunspot groups (LLG) there is a linear form Amax = (12.9 ± 1.1)LT. Allowance only for recurrent sunspot groups with lifetimes more than 40 days gives Amax = (13.93 ± 0.41)LT.


