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

Author:

Sfaradi Itai1,Beniamini Paz234ORCID,Horesh Assaf1,Piran Tsvi1ORCID,Bright Joe5,Rhodes Lauren5ORCID,Williams David R A6ORCID,Fender Rob5,Leung James K789ORCID,Murphy Tara79ORCID,Green Dave A10ORCID

Affiliation:

1. Racah Institute of Physics. The Hebrew University of Jerusalem. Jerusalem 91904 , Israel

2. Department of Natural Sciences, The Open University of Israel , P.O Box 808, Ra’anana 4353701 , Israel

3. Astrophysics Research Center of the Open University (ARCO), The Open University of Israel , P.O Box 808, Ra’anana 4353701 , Israel

4. Department of Physics, The George Washington University , 725 21st Street NW, Washington, DC 20052 , USA

5. Astrophysics, Department of Physics, University of Oxford , Keble Road, Oxford OX1 3RH , UK

6. Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, University of Manchester , Manchester M13 9PL , UK

7. Sydney Institute for Astronomy, School of Physics, The University of Sydney , NSW 2006 , Australia

8. CSIRO Space and Astronomy , PO Box 76, Epping, NSW 1710 , Australia

9. ARC Centre of Excellence for Gravitational Wave Discovery (OzGrav) , Hawthorn, Victoria , Australia

10. Astrophysics Group, Cavendish Laboratory , 19 J. J. Thomson Ave., Cambridge CB3 0HE , UK

Abstract

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 d since the last reported radio observation. We detected no radio emission from 30–220 d after the optical discovery in our observations at 15.5 GHz down to a 3σ level of <0.14 mJy. The fast-rising, delayed radio flare is observed in our radio data set and continues to rise almost ∼1580 d after the optical discovery. We find that the delayed radio emission, first detected 972 d after optical discovery, evolves as t4.2 ± 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 ∼ 1055 erg, an opening angle of ∼7°, and a relatively large viewing angle of ∼42°, 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 × 1052 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.

Funder

European Research Council

Australian Research Council

Australian Government

CSIRO

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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