Petr Kubánek
Spanish National Research Council
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Publication
Featured researches published by Petr Kubánek.
Nature | 2011
Bruno Sicardy; Jose Luis Ortiz; M. Assafin; Emmanuel Jehin; A. Maury; E. Lellouch; R. Gil Hutton; F. Braga-Ribas; François Colas; Daniel Hestroffer; J. Lecacheux; F. Roques; P. Santos-Sanz; Thomas Widemann; N. Morales; R. Duffard; A. Thirouin; A. J. Castro-Tirado; Martin Jelinek; Petr Kubánek; A. Sota; R. Sánchez-Ramírez; Alexandre Humberto Andrei; J. I. B. Camargo; D. N. da Silva Neto; A. Ramos Gomes; R. Vieira Martins; Michaël Gillon; Jean Manfroid; G. P. Tozzi
The dwarf planet Eris is a trans-Neptunian object with an orbital eccentricity of 0.44, an inclination of 44 degrees and a surface composition very similar to that of Pluto. It resides at present at 95.7 astronomical units (1 au is the Earth-Sun distance) from Earth, near its aphelion and more than three times farther than Pluto. Owing to this great distance, measuring its size or detecting a putative atmosphere is difficult. Here we report the observation of a multi-chord stellar occultation by Eris on 6 November 2010 ut. The event is consistent with a spherical shape for Eris, with radius 1,163 ± 6 kilometres, density 2.52 ± 0.05 grams per cm3 and a high visible geometric albedo, . No nitrogen, argon or methane atmospheres are detected with surface pressure larger than ∼1 nanobar, about 10,000 times more tenuous than Plutos present atmosphere. As Plutos radius is estimated to be between 1,150 and 1,200 kilometres, Eris appears as a Pluto twin, with a bright surface possibly caused by a collapsed atmosphere, owing to its cold environment. We anticipate that this atmosphere may periodically sublimate as Eris approaches its perihelion, at 37.8 astronomical units from the Sun.
The Astrophysical Journal | 2012
W. Zheng; Rongfeng Shen; Takanori Sakamoto; A. P. Beardmore; M. De Pasquale; Xue-Feng Wu; J. Gorosabel; Yuji Urata; Satoshi Sugita; Bin-Bin Zhang; Alexei S. Pozanenko; M. Nissinen; D. K. Sahu; Myungshin Im; T. N. Ukwatta; M. Andreev; E. Klunko; A. Volnova; C. Akerlof; P. Anto; S. D. Barthelmy; Alice A. Breeveld; U. Carsenty; Sebastián Castillo-Carrión; A. J. Castro-Tirado; M. M. Chester; C.-J. Chuang; Ronan Cunniffe; A. de Ugarte Postigo; R. Duffard
We present a comprehensive analysis of a bright, long-duration (T-90 similar to 257 s) GRB 110205A at redshift z = 2.22. The optical prompt emission was detected by Swift/UVOT, ROTSE-IIIb, and BOOTES telescopes when the gamma-ray burst (GRB) was still radiating in the gamma-ray band, with optical light curve showing correlation with gamma-ray data. Nearly 200 s of observations were obtained simultaneously from optical, X-ray, to gamma-ray (1 eV to 5 MeV), which makes it one of the exceptional cases to study the broadband spectral energy distribution during the prompt emission phase. In particular, we clearly identify, for the first time, an interesting two-break energy spectrum, roughly consistent with the standard synchrotron emission model in the fast cooling regime. Shortly after prompt emission (similar to 1100 s), a bright (R = 14.0) optical emission hump with very steep rise (alpha similar to 5.5) was observed, which we interpret as the reverse shock (RS) emission. It is the first time that the rising phase of an RS component has been closely observed. The full optical and X-ray afterglow light curves can be interpreted within the standard reverse shock (RS) + forward shock (FS) model. In general, the high-quality prompt and afterglow data allow us to apply the standard fireball model to extract valuable information, including the radiation mechanism (synchrotron), radius of prompt emission (R-GRB similar to 3 x 10(13) cm), initial Lorentz factor of the outflow (Gamma(0) similar to 250), the composition of the ejecta (mildly magnetized), the collimation angle, and the total energy budget.
Nature | 2008
A. J. Castro-Tirado; A. de Ugarte Postigo; J. Gorosabel; Martin Jelinek; T. A. Fatkhullin; V. V. Sokolov; P. Ferrero; D. A. Kann; Sylvio Klose; Dominique Sluse; M. Bremer; J. M. Winters; D. Nuernberger; D. Pérez-Ramírez; M. A. Guerrero; James C. French; G. Melady; L. Hanlon; Brian McBreen; K. Leventis; Sera Markoff; S. Leon; Alexander Kraus; F. J. Aceituno; Ronan Cunniffe; Petr Kubánek; Stanislav Vitek; S. Schulze; A. C. Wilson; Rene Hudec
Magnetars are young neutron stars with very strong magnetic fields of the order of 1014–1015 G. They are detected in our Galaxy either as soft γ-ray repeaters or anomalous X-ray pulsars. Soft γ-ray repeaters are a rare type of γ-ray transient sources that are occasionally detected as bursters in the high-energy sky. No optical counterpart to the γ-ray flares or the quiescent source has yet been identified. Here we report multi-wavelength observations of a puzzling source, SWIFT J195509+261406. We detected more than 40 flaring episodes in the optical band over a time span of three days, and a faint infrared flare 11 days later, after which the source returned to quiescence. Our radio observations confirm a Galactic nature and establish a lower distance limit of ∼3.7 kpc. We suggest that SWIFT J195509+261406 could be an isolated magnetar whose bursting activity has been detected at optical wavelengths, and for which the long-term X-ray emission is short-lived. In this case, a new manifestation of magnetar activity has been recorded and we can consider SWIFT J195509+261406 to be a link between the ‘persistent’ soft γ-ray repeaters/anomalous X-ray pulsars and dim isolated neutron stars.A. J. Castro-Tirado, A. de Ugarte Postigo, J. Gorosabel, M. Jeĺınek, T. A. Fatkhullin, V. V. Sokolov, P. Ferrero, D. A. Kann, S. Klose, D. Sluse, M. Bremer, J. M. Winters, D. Nuernberger, D. Pérez-Ramı́rez, M. A. Guerrero, J. French, G. Melady, L. Hanlon, B. McBreen, F. J. Aceituno, R. Cunniffe, P. Kubánek, S. Vitek, S. Schulze, A. C. Wilson, R. Hudec, J. M. González-Pérez, T. Shahbaz, S. Guziy, S. B. Pandey L. Pavlenko, E. Sonbas, S. A. Trushkin, N. N. Bursov, N. A. Nizhelskij and L. Sabau-Graziati
Astronomy and Astrophysics | 2006
Martin Jelinek; Michael Prouza; Petr Kubánek; Rene Hudec; Martin Nekola; J. Řídký; J. Grygar; M. Boháčová; A. J. Castro-Tirado; J. Gorosabel; M. Hrabovský; D. Mandát; D. Nosek; L. Nožka; M. Palatka; S. B. Pandey; M. Pech; P. Schovánek; R. Šmída; P. Trávníček; A. de Ugarte Postigo; Stanislav Vitek
We present a discovery and observation of an extraordinarily bright prompt optical emission of the GRB 0601 17 obtained by a wide-field camera atop the robotic telescope FRAM of the Pierre Auger Observatory from 2 to 10 min after the GRB. We found rapid average temporal flux decay of a = -1.7 ± 0.1 and a peak brightness R = 10.1 mag. Later observations by other instruments set a strong limit on the optical and radio transient fluxes, unveiling an unexpectedly rapid further decay. We present an interpretation featuring a relatively steep electron-distribution parameter p ≃ 3.0 and providing a straightforward solution for the overall fast decay of this optical transient as a transition between reverse and forward shock.
GAMMA-RAY BURSTS: 30 YEARS OF DISCOVERY: Gamma-Ray Burst Symposium | 2004
Petr Kubánek; Martin Jelinek; Martin Nekola; Martin Topinka; Jan Štrobl; R. Hudec; Tomas J. Mateo Sanguino; Antonio de Ugarte Postigo; A. J. Castro-Tirado
BART is a small remote controlled robotic CCD telescope, devoted to rapid observation of prompt gamma ray burst transients. During its operation since early 2001, it had three prompt observations with world‐competitive response time. The constraints to object magnitude were estimated and published in GCN circulars. Telescope is located in Astronomical Institute of the Czech Academy of Sciences in Ondřejov. This poster describes its new control system, named RTS2, which has been in service since February 2003.
Proceedings of SPIE | 2010
I.V. Kotov; A.I. Kotov; J. S. Frank; Petr Kubánek; M. Prouza; P. O'Connor; V. Radeka; Peter Z. Takacs
Future wide field astronomical surveys, like Large Synoptic Survey Telescope (LSST), require photometric precision on the percent level. The accuracy of sensor calibration procedures should match these requirements. Pixel size variations found in CCDs from different manufacturers are the source of systematic errors in the flat field calibration procedure. To achieve the calibration accuracy required to meet the most demanding science goals this effect should be taken into account. The study of pixel area variations was performed for fully depleted, thick CCDs produced in a technology study for LSST. These are n-channel, 100μm thick devices. We find pixel size variations in both row and column directions. The size variation magnitude is smaller in the row direction. In addition, diffusion is found to smooth out electron density variations. It is shown that the characteristic diffusion width can be extracted from the flat field data. Results on pixel area variations and diffusion, data features, analysis technique and modeling technique are presented and discussed.
Advances in Astronomy | 2010
M. Prouza; Martin Jelinek; Petr Kubánek; J. Ebr; P. Travnicek; Radomir Smida
FRAM—F/(Ph)otometric Robotic Atmospheric Monitor is one of the atmospheric monitoring instruments at the Pierre Auger Observatory in Argentina. FRAM is an optical telescope equipped with CCD cameras and photometer, and it automatically observes a set of selected standard stars. Primarily, FRAM observations are used to obtain the wavelength dependence of the light extinction. FRAM telescope is also able to observe secondary astronomical targets, and namely the detection of optical counterparts of gamma-ray bursts has already proven to be successful. Finally, a wide-field CCD camera of FRAM can be used for rapid monitoring of atmospheric conditions along the track of particularly interesting cosmic ray showers. The hardware setup of the telescope, its software system, data taking procedures, and results of analysis are described in this paper.
Proceedings of SPIE | 2008
Petr Kubánek; Martin Jelinek; John French; Michal Prouza; Stanislav Vitek; A. J. Castro-Tirado; V. Reglero
Remote Telescope System 2nd version (RTS2) is an open source project aimed at developing a software environment to control a fully robotic observatory. RTS2 consists of various components, which communicate via an ASCII based protocol. As the protocol was from the beginning designed as an observatory control system, it provides some unique features, which are hard to find in the other communication systems. These features include advanced synchronisation mechanisms and strategies for setting variables. This presentation describes the protocol and its unique features. It also assesses protocol performance, and provides examples how the RTS2 library can be used to quickly build an observatory control system.
Proceedings of SPIE | 2012
Christopher R. Klein; Petr Kubánek; Nathaniel R. Butler; Ori D. Fox; Alexander S. Kutyrev; David A. Rapchun; Joshua S. Bloom; Alejandro Farah; Neil Gehrels; L. Georgiev; J. Gonzalez; William H. Lee; Gennadiy N. Lotkin; S. H. Moseley; J. Xavier Prochaska; Enrico Ramirez-Ruiz; Michael G. Richer; Frederick D. Robinson; Carlos G. Román-Zúñiga; Mathew V. Samuel; Leroy M. Sparr; Corey Tucker; Alan M. Watson
The Reionization And Transients InfraRed (RATIR) camera has been built for rapid Gamma-Ray Burst (GRB) followup and will provide quasi-simultaneous imaging in ugriZY JH. The optical component uses two 2048 × 2048 pixel Finger Lakes Imaging ProLine detectors, one optimized for the SDSS u, g, and r bands and one optimized for the SDSS i band. The infrared portion incorporates two 2048 × 2048 pixel Teledyne HgCdTe HAWAII-2RG detectors, one with a 1.7-micron cutoff and one with a 2.5-micron cutoff. The infrared detectors are controlled by Teledynes SIDECAR (System for Image Digitization Enhancement Control And Retrieval) ASICs (Application Specific Integrated Circuits). While other ground-based systems have used the SIDECAR before, this system also utilizes Teledynes JADE2 (JWST ASIC Drive Electronics) interface card and IDE (Integrated Development Environment). Here we present a summary of the software developed to interface the RATIR detectors with Remote Telescope System, 2nd Version (RTS2) software. RTS2 is an integrated open source package for remote observatory control under the Linux operating system and will autonomously coordinate observatory dome, telescope pointing, detector, filter wheel, focus stage, and dewar vacuum compressor operations. Where necessary we have developed custom interfaces between RTS2 and RATIR hardware, most notably for cryogenic focus stage motor drivers and temperature controllers. All detector and hardware interface software developed for RATIR is freely available and open source as part of the RTS2 distribution.
Monthly Notices of the Royal Astronomical Society | 2012
L. Resmi; Kuntal Misra; G. Jóhannesson; A. J. Castro-Tirado; J. Gorosabel; Martin Jelinek; D. Bhattacharya; Petr Kubánek; G. C. Anupama; A. Sota; D. K. Sahu; A. de Ugarte Postigo; S. B. Pandey; R. Sánchez-Ramírez; M. Bremer; Ram Sagar
The Swift era has posed a challenge to the standard blast-wave model of gamma-ray burst (GRB) afterglows. The key observational features expected within the model are rarely observed, such as the achromatic steepening (‘jet break’) of light curves. The observed afterglow light curves showcase additional complex features requiring modifications within the standard model. Here we present optical/near-infrared observations, millimetre upper limits and comprehensive broad-band modelling of the afterglow of the bright GRB 0505025A, detected by Swift. This afterglow cannot be explained by the simplistic form of the standard blast-wave model. We attempt modelling multiwavelength light curves using (i) a forward–reverse shock model, (ii) a two-component outflow model and (iii) a blast-wave model with a wind termination shock. The forward–reverse shock model cannot explain the evolution of the afterglow. The two-component model is able to explain the average behaviour of the afterglow very well but cannot reproduce the fluctuations in the early X-ray light curve. The wind termination shock model reproduces the early light curves well but deviates from the global behaviour of the late-time afterglow.