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Tidal disruption of a low-mass star in an active galactic nucleus as the origin of the PS16dtm outburst

M. SniegowskaAstronomical Institute, Czech Academy of SciencesBożena CzernyPolish Academy of SciencesMichal ZajačekDepartment of Theoretical Physics and Astrophysics, Masaryk UniversityValentina RosaAstronomical Institute, Czech Academy of SciencesVladimír KarasAstronomical Institute, Czech Academy of SciencesT. JankovičInstitute of Physics of the Czech Academy of SciencesT. PetrushevskaCenter for Astrophysics and Cosmology, University of Nova Gorica, Vipavska 11cD. IlićDepartment of Astronomy, University of Belgrade – Faculty of MathematicsBenny TrakhtenbrotSchool of Physics and Astronomy, Tel Aviv UniversityPetr KurfürstDepartment of Theoretical Physics and Astrophysics, Masaryk University
2026en
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Litsenziya: cc-by

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Context. The event PS16dtm, which occurred in the centre of the narrow-line Seyfert 1 (NLS1) galaxy SDSS J015804.75−005221.8 ( z = 0.080440), is one of the few candidates for a tidal disruption event in an already-accreting active galactic nucleus. Aims. We wish to shed light on the character of the tidal disruption event in this source since it exhibits unusual peculiarities, such as the double-peak optical/UV light curve and a low blackbody temperature with a lack of X-ray emission. Methods. We performed a spectral analysis of the source before and during the event. We modelled the time evolution of the luminosity profile using a numerical code that describes the viscous evolution of the flow. Results. Based on the combined spectral and timing studies, we interpret the event as the disruption of a ∼0.3 M ⊙ main-sequence star or as the gradual partial disruption of a low-mass giant star. The star is likely on a circular orbit, embedded in the accretion disc. We discuss that the evolution of the star rather suggests that the orbit is counter-rotating. We observe the system at a sufficiently large viewing angle that the actual disruption process is not directly observed. The disrupted star and inner disc are shielded from the observer by a gaseous envelope. Further observations of the system as it returns to the previous NLS1 state, particularly in the X-ray band, are needed to confirm the proposed scenario and to place constraints on the return to a regular NLS1 state.

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