Igor Molotov
Keldysh Institute of Applied Mathematics
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Featured researches published by Igor Molotov.
Nature | 2016
Mariko Kimura; Keisuke Isogai; Taichi Kato; Yoshihiro Ueda; Satoshi Nakahira; Megumi Shidatsu; Teruaki Enoto; Takafumi Hori; Daisaku Nogami; Colin Littlefield; Ryoko Ishioka; Ying-Tung Chen; S.-K. King; Chih Yi Wen; Shiang-Yu Wang; M. J. Lehner; Megan E. Schwamb; Jen Hung Wang; Z.-W. Zhang; Charles Alcock; Tim Axelrod; Federica B. Bianco; Yong Ik Byun; W. P. Chen; Kem H. Cook; Dae-Won Kim; Typhoon Lee; S. L. Marshall; Elena P. Pavlenko; Oksana I. Antonyuk
How black holes accrete surrounding matter is a fundamental yet unsolved question in astrophysics. It is generally believed that matter is absorbed into black holes via accretion disks, the state of which depends primarily on the mass-accretion rate. When this rate approaches the critical rate (the Eddington limit), thermal instability is supposed to occur in the inner disk, causing repetitive patterns of large-amplitude X-ray variability (oscillations) on timescales of minutes to hours. In fact, such oscillations have been observed only in sources with a high mass-accretion rate, such as GRS 1915+105 (refs 2, 3). These large-amplitude, relatively slow timescale, phenomena are thought to have physical origins distinct from those of X-ray or optical variations with small amplitudes and fast timescales (less than about 10 seconds) often observed in other black-hole binaries—for example, XTE J1118+480 (ref. 4) and GX 339−4 (ref. 5). Here we report an extensive multi-colour optical photometric data set of V404 Cygni, an X-ray transient source containing a black hole of nine solar masses (and a companion star) at a distance of 2.4 kiloparsecs (ref. 8). Our data show that optical oscillations on timescales of 100 seconds to 2.5 hours can occur at mass-accretion rates more than ten times lower than previously thought. This suggests that the accretion rate is not the critical parameter for inducing inner-disk instabilities. Instead, we propose that a long orbital period is a key condition for these large-amplitude oscillations, because the outer part of the large disk in binaries with long orbital periods will have surface densities too low to maintain sustained mass accretion to the inner part of the disk. The lack of sustained accretion—not the actual rate—would then be the critical factor causing large-amplitude oscillations in long-period systems.
Astronomy and Astrophysics | 2008
J. Ďurech; David Vokrouhlický; Mikko Kaasalainen; Paul R. Weissman; S. Lowry; Edward C. Beshore; D. Higgins; Yurij N. Krugly; Vasilij G. Shevchenko; Ninel M. Gaftonyuk; Young-Jun Choi; R. A. Kowalski; S. M. Larson; Brian D. Warner; A. L. Marshalkina; M. A. Ibrahimov; Igor Molotov; T. Michałowski; Kohei Kitazato
Aims. Asteroid (1862) Apollo is one of two asteroids in which the YORP effect was detected. We carried out new photometric observations of Apollo in April 2007 to enlarge the time line and to derive a more precise shape and spin state model. We also observed another YORP-candidate, asteroid (25143) Itokawa, in December 2006 and January 2007 to obtain a longer time line. An estimation of the YORP strength on Itokawa based on its precise shape model from the Hayabusa mission predicted the deceleration to be already observable during the 2007 apparition. Methods. We used the lightcurve inversion method to model the shape and spin state of Apollo. For Itokawa, the shape and pole direction are known to a high degree of accuracy from the Hayabusa mission, so we used a modified version of lightcurve inversion with only two free parameters – the rotation period and its linear change in time. Results. The new model of Apollo confirms earlier results. The observed acceleration of Apollo’s rotation rate is (5.5 ± 1.2) × 10 −8 rad d −2 , which is in agreement with the theoretically predicted value. For Itokawa, the theoretical YORP value is sensitive to the resolution of the shape model and lies in the range from − 2t o−3 × 10 −7 rad d −2 . This is inconsistent with results of lightcurve inversion that place an upper limit to the change of Itokawa’s rotation rate ∼1.5 × 10 −7 rad d −2 .
Astronomy and Astrophysics | 2014
Z. Cano; A. de Ugarte Postigo; Alexei S. Pozanenko; N. Butler; C. C. Thöne; C. Guidorzi; T. Krühler; Javier Gorosabel; P. Jakobsson; G. Leloudas; Daniele Malesani; J. Hjorth; A. Melandri; Carole G. Mundell; K. Wiersema; P. D’Avanzo; S. Schulze; Andreja Gomboc; A. Johansson; W. Zheng; D. A. Kann; F. Knust; K. Varela; C. Akerlof; J. S. Bloom; O. Burkhonov; E. Cooke; J. A. de Diego; G. Dhungana; C. Fariña
We present optical and near-infrared (NIR) photometry for three gamma-ray burst supernovae (GRB-SNe): GRB 120729A, GRB 130215A/SN 2013ez, and GRB 130831A/SN 2013fu. For GRB 130215A/SN 2013ez, we also present optical spectroscopy at t − t0 = 16.1 d, which covers rest-frame 3000–6250 A. Based on Fe ii λ5169 and Si ii λ6355, our spectrum indicates an unusually low expansion velocity of ~4000–6350 km s-1, the lowest ever measured for a GRB-SN. Additionally, we determined the brightness and shape of each accompanying SN relative to a template supernova (SN 1998bw), which were used to estimate the amount of nickel produced via nucleosynthesis during each explosion. We find that our derived nickel masses are typical of other GRB-SNe, and greater than those of SNe Ibc that are not associated with GRBs. For GRB 130831A/SN 2013fu, we used our well-sampled R-band light curve (LC) to estimate the amount of ejecta mass and the kinetic energy of the SN, finding that these too are similar to other GRB-SNe. For GRB 130215A, we took advantage of contemporaneous optical/NIR observations to construct an optical/NIR bolometric LC of the afterglow. We fit the bolometric LC with the millisecond magnetar model of Zhang & Meszaros (2001, ApJ, 552, L35), which considers dipole radiation as a source of energy injection to the forward shock powering the optical/NIR afterglow. Using this model we derive an initial spin period of P = 12 ms and a magnetic field of B = 1.1 × 1015 G, which are commensurate with those found for proposed magnetar central engines of other long-duration GRBs.
Astronomy and Astrophysics | 2012
J. Ďurech; David Vokrouhlický; Alexandr Baransky; Sławomir Breiter; O. A. Burkhonov; W.R. Cooney; V. Fuller; Ninel M. Gaftonyuk; John D. Gross; R. Ya. Inasaridze; Mikko Kaasalainen; Yu. N. Krugly; O. I. Kvaratshelia; Elena Litvinenko; Bennie E. Macomber; Franck Marchis; Igor Molotov; Julian Oey; David Polishook; J. Pollock; Petr Pravec; K. Sarneczky; Vasilij G. Shevchenko; I. Slyusarev; Robert D. Stephens; Gy. M. Szabó; Dirk Terrell; Frederic Vachier; Z. Vanderplate; M. Viikinkoski
Context. The spin state of small asteroids can change on a long timescale by the Yarkovsky-O’Keefe-Radzievskii-Paddack (YORP) effect, the net torque that arises from anisotropically scattered sunlight and proper thermal radiation from an irregularly-shaped asteroid. The secular change in the rotation period caused by the YORP effect can be detected by analysis of asteroid photometric lightcurves. Aims. We analyzed photometric lightcurves of near-Earth asteroids (1865) Cerberus, (2100) Ra-Shalom, and (3103) Eger with the aim to detect possible deviations from the constant rotation caused by the YORP effect. Methods. We carried out new photometric observations of the three asteroids, combined the new lightcurves with archived data, and used the lightcurve inversion method to model the asteroid shape, pole direction, and rotation rate. The YORP effect was modeled as a linear change in the rotation rate in time dω/dt .V alues of dω/dt derived from observations were compared with the values predicted by theory. Results. We derived physical models for all three asteroids. We had to model Eger as a nonconvex body because the convex model failed to fit the lightcurves observed at high phase angles. We probably detected the acceleration of the rotation rate of Eger dω/dt = (1.4 ± 0.6) × 10 −8 rad d −2 (3σ error), which corresponds to a decrease in the rotation period by 4. 2m s yr −1 . The photometry of Cerberus and Ra-Shalom was consistent with a constant-period model, and no secular change in the spin rate was detected. We could only constrain maximum values of |dω/dt| < 8 × 10 −9 rad d −2 for Cerberus, and |dω/dt| < 3 × 10 −8 rad d −2 for Ra-Shalom.
Icarus | 2015
P. Scheirich; Petr Pravec; Seth A. Jacobson; J. Ďurech; Peter Kusnirak; Kamil Hornoch; S. Mottola; M. Mommert; S. Hellmich; Donald P. Pray; David Polishook; Yu. N. Krugly; R. Ya. Inasaridze; O. Kvaratskhelia; Vova Ayvazian; I. Slyusarev; J. Pittichová; Emmanuel Jehin; Jean Manfroid; Michaël Gillon; Adrian Galad; J. Pollock; J. Licandro; V. Alí-Lagoa; James W. Brinsfield; Igor Molotov
Abstract Using our photometric observations taken between April 1996 and January 2013 and other published data, we derived properties of the binary near-Earth Asteroid (175706) 1996 FG3 including new measurements constraining evolution of the mutual orbit with potential consequences for the entire binary asteroid population. We also refined previously determined values of parameters of both components, making 1996 FG3 one of the most well understood binary asteroid systems. With our 17-year long dataset, we determined the orbital vector with a substantially greater accuracy than before and we also placed constraints on a stability of the orbit. Specifically, the ecliptic longitude and latitude of the orbital pole are 266 ° and - 83 ° , respectively, with the mean radius of the uncertainty area of 4 ° , and the orbital period is 16.1508 ± 0.0002 h (all quoted uncertainties correspond to 3σ). We looked for a quadratic drift of the mean anomaly of the satellite and obtained a value of 0.04 ± 0.20 deg / yr 2 , i.e., consistent with zero. The drift is substantially lower than predicted by the pure binary YORP (BYORP) theory of McMahon and Scheeres (McMahon, J., Scheeres, D. [2010]. Icarus 209, 494–509) and it is consistent with the tigidity and quality factor of μ Q = 1.3 × 10 7 Pa using the theory that assumes an elastic response of the asteroid material to the tidal forces. This very low value indicates that the primary of 1996 FG3 is a ‘rubble pile’, and it also calls for a re-thinking of the tidal energy dissipation in close asteroid binary systems.
The Astronomical Journal | 2016
David Vokrouhlický; J. Ďurech; Petr Pravec; Peter Kusnirak; Kamil Hornoch; J. Vraštil; Yurij N. Krugly; Raguli Inasaridze; Vova Ayvasian; Vasili Zhuzhunadze; Igor Molotov; Donald P. Pray; Marek Husárik; J. Pollock; David Nesvorný
The Schulhof family, a tight cluster of small asteroids around the central main belt body (2384)Schulhof, belongs to a so far rare class of very young families (estimated ages less than 1Myr). Characterization of these asteroid clusters may provide important insights into the physics of the catastrophic disruption of their parent body. The case of the Schulhof family has been up to now complicated by the existence of two proposed epochs of its origin. In this paper, we first use our own photometric observations, as well as archival data, to determine the rotation rate and spin axis orientation of the largest fragment (2384)Schulhof. Our data also allow us to better constrain the absolute magnitude of this asteroid, and thus also improve the determination of its geometric albedo. Next, using the up-to-date catalog of asteroid orbits, we perform a new search of smaller members in the Schulhof family, increasing their number by 50%. Finally, the available data are used to access Schulhofʼs family age anew. We now find that the younger of the previously proposed two ages of this family is not correct, resulting from a large orbital uncertainty of single-opposition members. Our new runs reveal a single age solution of about 800 kyr with a realistic uncertainty of 200 kyr.
Astronomy and Astrophysics | 2015
W. Thuillot; David Bancelin; A. Ivantsov; Josselin Desmars; M. Assafin; Siegfried Eggl; Daniel Hestroffer; P. Rocher; B. Carry; P. David; Lyu Abe; M. Andreev; J.-E. Arlot; A. Asami; V. Ayvasian; A. Baransky; M. Belcheva; Ph. Bendjoya; Ilfan Bikmaev; O. A. Burkhonov; U. Camci; A. Carbognani; F. Colas; A. V. Devyatkin; Sh. A. Ehgamberdiev; P. Enikova; Laurent Eyer; A. I. Galeev; Enrico Gerlach; V. Godunova
Aims. Astrometric observations performed by the Gaia Follow-Up Network for Solar System Objects (Gaia-FUN-SSO) play a key role in ensuring that moving objects first detected by ESA’s Gaia mission remain recoverable after their discovery. An observation campaign on the potentially hazardous asteroid (99 942) Apophis was conducted during the asteroid’s latest period of visibility, from 12/21/2012 to 5/2/2013, to test the coordination and evaluate the overall performance of the Gaia-FUN-SSO . Methods. The 2732 high quality astrometric observations acquired during the Gaia-FUN-SSO campaign were reduced with the Platform for Reduction of Astronomical Images Automatically (PRAIA), using the USNO CCD Astrograph Catalogue 4 (UCAC4) as a reference. The astrometric reduction process and the precision of the newly obtained measurements are discussed. We compare the residuals of astrometric observations that we obtained using this reduction process to data sets that were individually reduced by observers and accepted by the Minor Planet Center. Results. We obtained 2103 previously unpublished astrometric positions and provide these to the scientific community. Using these data we show that our reduction of this astrometric campaign with a reliable stellar catalog substantially improves the quality of the astrometric results. We present evidence that the new data will help to reduce the orbit uncertainty of Apophis during its close approach in 2029. We show that uncertainties due to geolocations of observing stations, as well as rounding of astrometric data can introduce an unnecessary degradation in the quality of the resulting astrometric positions. Finally, we discuss the impact of our campaign reduction on the recovery process of newly discovered asteroids.
Proceedings of the International Astronomical Union | 2006
Yu. N. Krugly; Ninel M. Gaftonyuk; Irina N. Belskaya; V. G. Chiorny; Vasilij G. Shevchenko; F. P. Velichko; D.F. Lupishko; A. A. Konovalenko; I. S. Falkovich; Igor Molotov
The regular CCD observations of near-Earth asteroids (NEAs) in the Institute of Astronomy of Kharkiv National University were initiated in 1995 within the framework of asteroid hazard problem in collaboration with the DLR, Institute of Planetary Research (Berlin). The main aim of the study is a determination of rotation periods and shapes of NEAs as well as astrometry of newly discovered objects. We also carry out the absolute photometry of NEAs in BV RI bands in order to put constraints on surface properties and to estimate their diameters. The observations are carried out with 0.7-m telescope of the Institute of Astronomy (Kharkiv) and with 1-m telescope of the Crimean Astrophysical Observatory (Simeiz) in the standard Johnson-Cousins photometric system. Some observations were made as an optical support of radar observation of NEAs. We present the results of photometric observations of 21 NEAs obtained in 2004-2006 which include asteroid rotation properties, diameters and shapes.
Open Astronomy | 2018
Artem Mokhnatkin; Igor Molotov; Eduardo Gerardo Perez Tijerina; José Enrique Perez Leon; Tatiana Kokina; Thomas Schildknecht
Abstract ISON, being an open international project that collects and interprets data about space objects for scientific analysis and spacecraft operators, includes about 40 observational sites. An involvement of two Mexican sites participating in optical observations of geostationary and highly elliptical objects as a part of the ISON project is considered. A brief description of the facilities and their observation statistics are given. Prospects for the further development of sites for monitoring near-Earth objects in Mexico are presented, including data of astronomical observing conditions from field stations.
Icarus | 2011
Christopher Magri; Ellen Susanna Howell; Michael C. Nolan; Patrick A. Taylor; Yanga R. Fernandez; Michael Mueller; Ronald Joe Vervack; Lance A. M. Benner; Jon D. Giorgini; Steven J. Ostro; Daniel J. Scheeres; Michael D. Hicks; H. Rhoades; James M. Somers; Ninel M. Gaftonyuk; Vladimir Kouprianov; Yurij N. Krugly; Igor Molotov; Michael W. Busch; Jean-Luc Margot; Vladimir Benishek; Vojislava Protitch-Benishek; Adrian Galad; David J. Higgins; Peter Kusnirak; Donald P. Pray