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An off-axis relativistic jet seen in the long lasting delayed radio flare of the TDE AT 2018hyz

Published 3 Aug 2023 in astro-ph.HE | (2308.01965v1)

Abstract: The Tidal Disruption Event (TDE) AT 2018hyz exhibited a delayed radio flare almost three years after the stellar disruption. Here we report new radio observations of the TDE AT 2018hyz with the AMI-LA and ATCA spanning from a month to more than four years after the optical discovery and 200 days since the last reported radio observation. We detected no radio detection from 30-220 days after the optical discovery in our observations at 15.5 GHz down to a 3σ3\sigma level of < 0.14 mJy. The fast-rising, delayed, radio flare is observed in our radio data set and continues to rise almost ~1580 days after the optical discovery. We find that the delayed radio emission, first detected $972$ days after optical discovery, evolves as t<sup>4.2</sup>±0.9t<sup>{4.2</sup> \pm 0.9}, at 15.5 GHz. Here, we present an off-axis jet model that can explain the full set of radio observations. In the context of this model, we require a powerful narrow jet with an isotropic equivalent kinetic energy Ek,iso∼10<sup>55E_{\rm k,iso} \sim 10<sup>{55} erg, an opening angle of ∼7<sup>∘ \rm \sim 7<sup>{\circ}, and a relatively large viewing angle of ∼42<sup>∘ \rm \sim 42<sup>{\circ}, launched at the time of the stellar disruption. Within our framework, we find that the minimal collimated energy possible for an off-axis jet from AT 2018hyz is Ek≥3×10<sup>52E_k \geq 3 \times 10<sup>{52} erg. Finally, we provide predictions based on our model for the light curve turnover time, and for the proper motion of the radio emitting source.

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