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Marek Abramowicz (CAMK PAN)21/09/2026, 09:30
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Sabin Roman (Jožef Stefan Institute)21/09/2026, 11:30
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Serena Gambino (Scuola Superiore Meridionale)21/09/2026, 11:55
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Sakshi Maurya (Astronomical Observatory, University of Warsaw)21/09/2026, 12:20
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Debora Lančová21/09/2026, 14:15
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Piotr Płonka (Center for Theoretical Physics of the Polish Academy of Sciences)21/09/2026, 14:40
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Pulkit Ojha (Centrum Fizyki Teoretycznej PAN)21/09/2026, 15:05
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Antonios Nathanail21/09/2026, 16:00
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Stefan Jorda (HERAEUS)21/09/2026, 16:55
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Andreas Burkert21/09/2026, 17:20
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Agata Rozanska (CAMK PAN)21/09/2026, 17:35
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Monika Moscibrodzka, Monika Mościbrodzka22/09/2026, 09:30
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Eleni Antonopoulou (Academy of Athens, University of Athens)22/09/2026, 11:30
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Valentina Rosa (Astronomical Institute of the Czech Academy of Sciences)22/09/2026, 11:55
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Tintin Nguyen (Harvard University)22/09/2026, 12:20
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Aristomenis Yfantis (Instituto de Astrofisica de Andalucia)22/09/2026, 14:15
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Matúš Labaj (Masaryk University)22/09/2026, 14:40
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Dr Bestin James (Masaryk University)22/09/2026, 15:05
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Ben Hudson22/09/2026, 16:00
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Gilles Koziol (University of Geneva)22/09/2026, 16:25
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Andrey Sandomirsky (The Hebrew University of Jerusalem)22/09/2026, 16:50
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Vladimir Karas (Astronomical Institute of the Czech Academy of Sciences)23/09/2026, 09:30
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Joaquin Pelle (Max Planck Institute for Gravitational Physics (Potsdam))23/09/2026, 11:30
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Mohamad H. Naddaf (University of Liege, Belgium)23/09/2026, 11:55
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Ms Laetitia Gibaud (Faculty of Physics, University of Bialystok, Poland)23/09/2026, 12:20
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Matthew Quilt (University of Southampton)23/09/2026, 14:15
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Mr Biswaraj Palit (CAMK PAN)23/09/2026, 14:40
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Marios Kouzis (Nicolaus Copernicus Astronomical Center of the Polish Academy of Sciences)23/09/2026, 15:05
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Marzena Sniegowska (CAMK PAN, CFT PAN)23/09/2026, 16:00
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Parikshit Partha Biswas (Nicolaus Copernicus Astronomical Center, Warszawa)23/09/2026, 16:25
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Joysankar Majumdar (Astronomical Observatory, University of Warsaw)23/09/2026, 16:50
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Samaya NISSANKE24/09/2026, 09:30
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Alex Gormaz-Matamala (Astronomický ústav Akademie věd České republiky (ASU))24/09/2026, 11:30
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Antonio Matteri (Scuola Normale Superiore)24/09/2026, 11:55
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Pawan Kumar Gupta (CAMK, Warsaw, Poland)24/09/2026, 12:20
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Mr Joseph Saji (Center for Theoretical Physics, PAN)24/09/2026, 14:15
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Despina Karavola (National and Kapodistrian University of Athens)24/09/2026, 14:40
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Shivangi Pandey (Center for theoretical Physics PAS)24/09/2026, 15:05
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Mr Phillipp Podsiadlowski (University of Oxford)24/09/2026, 15:30
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Roger Blandford25/09/2026, 09:30
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Wen Xuan Sia25/09/2026, 11:30
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Jan Röder (IAA-CSIC)25/09/2026, 11:55
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Ana Laura Müller (FZU - Institute of Physics of the Czech Academy of Sciences)25/09/2026, 12:20
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Kaushik Satapathy (Instituto de Plasmas e Fusão Nuclear)25/09/2026, 14:15
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Maitrayee Gupta (Astronomical Institute of the Czech Academy of Sciences)25/09/2026, 14:40
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Simone Garrappa (Weizmann Institute of Science)25/09/2026, 15:05
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SANGEETHA KIZHAKKEKALAM (Janusz Gil Institute of Astronomy, University of Zielona Gora, Poland)25/09/2026, 16:00
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Michelle Tsirou (Institute of Physics of the Czech Academy of Sciences (FZU))25/09/2026, 16:25
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SAGAR SETHI (University of Warmia and Mazury in Olsztyn, Poland)25/09/2026, 16:50
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Michal Zajaček (Masaryk University, Brno, Czech Republic)
We investigate the possibility of detecting stellar eclipses of millimeter radio cores in nearby radio-loud active galactic nuclei. At millimeter wavelengths, the compact radio core can be partially occulted by large evolved stars orbiting the central supermassive black hole within a dense nuclear star cluster. We show that stars with radii >= 500 Rsun can produce the eclipses with relative...
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Maria Koper (Wydział Fizyki Uniwersytetu Warszawskiego)
We present magnetohydrodynamic simulations of a thin accretion disk around a Reissner–Nordström naked singularity, modeled with our pseudo-Newtonian potential. This potential accurately reproduces the orbital frequency, including the radius at which it reaches a maximum and eventually vanishes. The latter defines the zero-gravity sphere, below which the net force is repulsive. Our results show...
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Stefan Jorda (HERAEUS)
Institutional Talk
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Sanjit Debnath (Aryabhatta Research Institute of Observational Sciences (ARIES), India)
In transonic advective accretion flows, the presence of a shock gives rise to a hot, dense post-shock region that can act as the launching site of outflows. When viscosity is included, dissipation within this region increases the thermal energy of the flow, leading to a stronger pressure gradient that can drive more efficient mass ejection. The resulting outflows are not necessarily symmetric...
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Seshadri Majumder (Kyoto University)
Quasi-periodic oscillations (QPOs) are coherent X-ray timing features frequently observed in black hole X-ray binaries (BH-XRBs), originating from the innermost region of the accretion disc-corona system where general relativistic effects are expected to be in play. Among the proposed QPO models, the Lense-Thirring (LT) precession of the inner hot flow predicts a systematic modulation of the...
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Dr Marek Nikołajuk (University of Białystok, Faculty of Physics)
We investigate the tidal stripping of a cold helium white dwarf (WD) by a stellar-mass black hole (BH). Due to the degenerate nature of the WD, we expect quantum effects to play a significant role in the dynamics. To capture these effects, we use a full quantum hydrodynamic framework to simulate the formation of the accretion disk. We model the WD as a Bose–Fermi droplet consisting of...
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Agata Rozanska (CAMK PAN)
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NIKITA S ARUN (Providence Women's College)
We present a broadband X-ray spectral study of the narrow-line Seyfert 1 galaxy Ark 564 using a long-term monitoring dataset obtained with the X-Ray Telescope (XRT) onboard Neil Gehrels Swift Observatory. Ark 564 is known for its strong X-ray variability and prominent soft X-ray excess, making it an excellent laboratory for investigating accretion processes. We analyze more than 70 Swift/XRT...
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P. K. Navaneeth
The blazar B2 1420+32 (OQ 334, z = 0.682) has recently emerged as a primary laboratory for studying the "changing-look" (CL) phenomenon in jetted active galactic nuclei, characterized by transitions between FSRQ and BL Lac states. We present a detailed investigation into the complex nature of its X-ray emission using Swift-XRT observations spanning MJD 58095--60580. Using Bayesian Blocks...
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