B. Debski
Jagiellonian University
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Featured researches published by B. Debski.
The Astrophysical Journal | 2016
Mauri J. Valtonen; S. Zola; S. Ciprini; A. Gopakumar; Katsura Matsumoto; Kozo Sadakane; M. Kidger; Kosmas D. Gazeas; K. Nilsson; A. Berdyugin; V. Piirola; H. Jermak; Kiran S. Baliyan; F. Alicavus; David Boyd; M. Campas Torrent; F. Campos; J. Carrillo Gómez; Daniel B. Caton; V. Chavushyan; J. Dalessio; B. Debski; D. Dimitrov; M. Drozdz; H. Er; A. Erdem; A. Escartin Pérez; V. Fallah Ramazani; A. V. Filippenko; Shashikiran Ganesh
OJ 287 is a quasi-periodic quasar with roughly 12 year optical cycles. It displays prominent outbursts that are predictable in a binary black hole model. The model predicted a major optical outburst in 2015 December. We found that the outburst did occur within the expected time range, peaking on 2015 December 5 at magnitude 12.9 in the optical R-band. Based on Swift/XRT satellite measurements and optical polarization data, we find that it included a major thermal component. Its timing provides an accurate estimate for the spin of the primary black hole,
Publications of the Astronomical Society of Japan | 2014
Taichi Kato; Pavol A. Dubovsky; Igor Kudzej; Franz-Josef Hambsch; Ian Miller; Tomohito Ohshima; Chikako Nakata; Miho Kawabata; Hirochika Nishino; Kazunari Masumoto; Sahori Mizoguchi; Masayuki Yamanaka; Katsura Matsumoto; Daisuke Sakai; Daiki Fukushima; Minami Matsuura; Genki Bouno; Megumi Takenaka; Shinichi Nakagawa; Ryo Noguchi; Eriko Iino; Roger D. Pickard; Yutaka Maeda; Arne A. Henden; Kiyoshi Kasai; Seiichiro Kiyota; Hidehiko Akazawa; Kazuyoshi Imamura; Enrique de Miguel; Hiroyuki Maehara
\chi =0.313\pm 0.01
Publications of the Astronomical Society of Japan | 2016
Taichi Kato; Franz-Josef Hambsch; Berto Monard; Tonny Vanmunster; Yutaka Maeda; Ian Miller; Hiroshi Itoh; Seiichiro Kiyota; Keisuke Isogai; Mariko Kimura; Akira Imada; Tamás Tordai; Hidehiko Akazawa; Kenji Tanabe; Noritoshi Otani; Minako Ogi; Kazuko Ando; Naoki Takigawa; Pavol A. Dubovsky; Igor Kudzej; Sergey Yu. Shugarov; Natalia Katysheva; Polina Golysheva; Natalia Gladilina; Drahomir Chochol; Peter Starr; Kiyoshi Kasai; Roger D. Pickard; Enrique de Miguel; Naoto Kojiguchi
. The present outburst also confirms the established general relativistic properties of the system such as the loss of orbital energy to gravitational radiation at the 2% accuracy level, and it opens up the possibility of testing the black hole no-hair theorem with 10% accuracy during the present decade.
The Astronomical Journal | 2017
Ilham Nasiroglu; Aga Słowikowska; Krzysztof Krzeszowski; Michał Żejmo; S. Zola; H. Er; W. Ogloza; M. Drozdz; D. Kozieł-Wierzbowska; B. Debski; Nazlı Görücü Karaman
Continuing the project undertaken by Kato et al. (2009), we collected times of superhump maxima for 56 SU UMa-type dwarf novae mainly observed during the 2013-2014 season and characterized these objects. We detected negative superhumps in VW Hyi and indicated that the low number of normal outbursts in some supercycles can be interpreted as a result of disk tilt. This finding, combined with the Kepler observation of V1504 Cyg and V344 Lyr, suggests that disk tilt is responsible for modulating the outburst pattern in SU UMa-type dwarf novae. We also studied the deeply eclipsing WZ Sge-type dwarf nova MASTER OT J005740.99+443101.5 and found evidence of a sharp eclipse during the phase of early superhumps. The profile can be reproduced by a combination of the eclipse of the axisymmetric disk and the uneclipsed light source of early superhumps. This finding shows the lack of evidence for a greatly enhanced hot spot during the early stage of WZ Sge-type outburst. We detected growing (stage A) superhumps in MN Dra and give a suggestion that some of SU UMa-type dwarf novae situated near the critical condition of tidal instability may show long-lasting stage A superhumps. The large negative period derivatives reported in such systems can be understood as a result of the combination of stage A and B superhumps. Two WZ Sge-type dwarf novae, AL Com and ASASSN-13ck, showed a long-lasting (plateau-type) rebrightening. In the early phase of their rebrightenings, both objects showed a precursor-like outburst, suggesting that the long-lasting rebrightening is triggered by a precursor outburst.
The Astrophysical Journal | 2018
G. Bhatta; A. Markowitz; K. Balasubramaniam; S. Zola; A. A. Zdziarski; M. Jamrozy; M. Ostrowski; A. Kuzmicz; W. Ogloza; M. Drozdz; M. Siwak; D. Kozieł-Wierzbowska; B. Debski; T. Kundera; G. Stachowski; J. Machalski; V. S. Paliya; D. B. Caton
Continuing the project described by Kato et al. (2009, arXiv:0905.1757), we collected times of superhump maxima for 128 SU UMa-type dwarf novae observed mainly during the 2015-2016 season and characterized these objects. The data have improved the distribution of orbital periods, the relation between the orbital period and the variation of superhumps, the relation between period variations and the rebrightening type in WZ Sge-type objects. Coupled with new measurements of mass ratios using growing stages of superhumps, we now have a clearer and statistically greatly improved evolutionary path near the terminal stage of evolution of cataclysmic variables. Three objects (V452 Cas, KK Tel, ASASSN-15cl) appear to have slowly growing superhumps, which is proposed to reflect the slow growth of the 3:1 resonance near the stability border. ASASSN-15sl, ASASSN-15ux, SDSS J074859.55+312512.6 and CRTS J200331.3-284941 are newly identified eclipsing SU UMa-type (or WZ Sge-type) dwarf novae. ASASSN-15cy has a short (~0.050 d) superhump period and appears to belong to EI Psc-type objects with compact secondaries having an evolved core. ASASSN-15gn, ASASSN-15hn, ASASSN-15kh and ASASSN-16bu are candidate period bouncers with superhump periods longer than 0.06 d. We have newly obtained superhump periods for 79 objects and 13 orbital periods, including periods from early superhumps. In order that the future observations will be more astrophysically beneficial and rewarding to observers, we propose guidelines how to organize observations of various superoutbursts.
Proceedings of the International Astronomical Union | 2016
B. Debski; Stanislaw Zola
The cyclic behaviour of (O-C) residuals of eclipse timings in the sdB+M eclipsing binary NSVS 14256825 was previously attributed to one or two Jovian-type circumbinary planets. We report 83 new eclipse timings that not only fill in the gaps in those already published but also extend the time span of the (O-C) diagram by three years. Based on the archival and our new data spanning over more than 17 years we re-examined the up to date system (O-C). The data revealed systematic, quasi-sinusoidal variation deviating from an older linear ephemeris by about 100 s. It also exhibits a maximum in the (O-C) near JD 2,456,400 that was previously unknown. We consider two most credible explanations of the (O-C) variability: the light propagation time due to the presence of an invisible companion in a distant circumbinary orbit, and magnetic cycles reshaping one of the binary components, known as the Applegate or Lanza-Rodono effect. We found that the latter mechanism is unlikely due to the insufficient energy budget of the M-dwarf secondary. In the framework of the third-body hypothesis, we obtained meaningful constraints on the Keplerian parameters of a putative companion and its mass. Our best-fitting model indicates that the observed quasi-periodic (O-C) variability can be explained by the presence of a brown dwarf with the minimal mass of 15 Jupiter masses rather than a planet, orbiting the binary in a moderately elliptical orbit (~ 0.175) with the period of ~ 10 years. Our analysis rules out two planets model proposed earlier.
The Astrophysical Journal | 2016
G. Bhatta; S. Zola; M. Ostrowski; M. Winiarski; W. Ogloza; M. Drozdz; M. Siwak; A. Liakos; D. Kozieł-Wierzbowska; Kosmas D. Gazeas; B. Debski; T. Kundera; G. Stachowski; V. S. Paliya
Here we explore the disk-jet connection in the broad-line radio quasar 4C+74.26, utilizing the results of the multiwavelength monitoring of the source. The target is unique in that its radiative output at radio wavelengths is dominated by a moderately-beamed nuclear jet, at optical frequencies by the accretion disk, and in the hard X-ray range by the disk corona. Our analysis reveals a correlation (local and global significance of 96\% and 98\%, respectively) between the optical and radio bands, with the disk lagging behind the jet by
Galaxies | 2016
S. Zola; Mauri J. Valtonen; G. Bhatta; A. Goyal; B. Debski; A. Baran; J. Krzesinski; Michal Siwak; S. Ciprini; A. Gopakumar; H. Jermak; K. Nilsson; Daniel E. Reichart; Katsura Matsumoto; Kozo Sadakane; Kosmas D. Gazeas; M. Kidger; V. Piirola; F. Alicavus; K. S. Baliyan; A. Berdyugin; David Boyd; M. Campas Torrent; F. Campos; J. Carrillo Gómez; Daniel B. Caton; V. Chavushyan; J. Dalessio; D. Dimitrov; M. Drozdz
250 \pm 42
Galaxies | 2017
Mauri J. Valtonen; Stanislaw Zola; H. Jermak; S. Ciprini; R. Hudec; Lankeswar Dey; Achamveedu Gopakumar; Daniel L. Reichart; Daniel B. Caton; Kosmas D. Gazeas; Katsura Matsumoto; W. Ogloza; M. Drozdz; Fahri Alicavus; Oleksandr Baransky; A. Berdyugin; Panos Boumis; Yurii Bufan; B. Debski; H. Er; Ahmet Erdem; Vira Godunova; Shirin Haque; Vivian L. Hoette; Jan Janík; M. Kidger; Tomasz Kundera; Sebastian Kurowski; Alexis Liakos; Isa Mohammed
days. We discuss the possible explanation for this, speculating that the observed disk and the jet flux changes are generated by magnetic fluctuations originating within the innermost parts of a truncated disk, and that the lag is related to a delayed radiative response of the disk when compared with the propagation timescale of magnetic perturbations along relativistic outflow. This scenario is supported by the re-analysis of the NuSTAR data, modelled in terms of a relativistic reflection from the disk illuminated by the coronal emission, which returns the inner disk radius
The Astronomical Journal | 2017
Stanislaw Zola; Paula Szkody; S. Ciprini; F. Verrecchia; B. Debski; W. Ogloza; M. Drozdz; Daniel E. Reichart; Daniel B. Caton; Vivian L. Hoette
R_{\rm in}/R_{\rm ISCO} =35^{+40}_{-16}