2024MNRAS.527.7672S


Query : 2024MNRAS.527.7672S

2024MNRAS.527.7672S - Mon. Not. R. Astron. Soc., 527, 7672-7680 (2024/January-3)

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

SFARADI I., BENIAMINI P., HORESH A., PIRAN T., BRIGHT J., RHODES L., WILLIAMS D.R.A., FENDER R., LEUNG J.K., MURPHY T. and GREEN D.A.

Abstract (from CDS):

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 t^4.2 ± 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 E_k, 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.

Abstract Copyright: © The Author(s) 2023. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): radio continuum: transients - transients: tidal disruption events

Simbad objects: 20

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Number of rows : 20
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 CNSS J001947.3+003527 cm 00 19 47.335038 +00 35 26.81020           ~ 32 0
2 Z 500-36 AG? 00 29 57.0542865144 +32 53 37.265932104           ~ 155 0
3 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
4 2MASS J10065085+0141342 G 10 06 50.8773292152 +01 41 34.006164648   18.082   17.032   SNII 127 0
5 QSO B1004-018 Bla 10 07 04.34992476 -02 07 10.9189605   19.56 19.24 18.73   ~ 79 1
6 QSO J1008+0621 BLL 10 08 00.81616040 +06 21 21.2160257 17.61 17.17 17.85 16.73   ~ 123 1
7 SWIFT J1112.2-8238 X 11 11 47.797 -82 38 44.71           ~ 81 0
8 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
9 IGR J12580+0134 gam 12 58 05.1 +01 34 26           ~ 50 0
10 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
11 AT 2022cmc ev 13 34 43.207 +33 13 00.54           ~ 79 0
12 Z 49-155 Sy1 15 24 16.6702264008 +04 51 19.027331064   16.70 16.26     ~ 70 0
13 AT 2020vwl ev 15 30 37.800 +26 58 56.90           ~ 40 0
14 AT 2020opy ev 15 56 25.728 +23 22 21.15           ~ 28 0
15 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
16 SN 2019fdr SN* 17 09 06.859 +26 51 20.50           SLSN-II 48 0
17 ICRF J193925.0-634245 Sy2 19 39 25.0245304992 -63 42 45.640373400   18.87 18.37 17.64   ~ 1332 2
18 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 184 0
19 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
20 SWIFT J2058.4+0516 X 20 58 19.898 +05 13 32.25           ~ 169 0

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