2022ApJ...933..176S


Query : 2022ApJ...933..176S

2022ApJ...933..176S - Astrophys. J., 933, 176-176 (2022/July-2)

A Late-time Radio Flare Following a Possible Transition in Accretion State in the Tidal Disruption Event AT 2019azh.

SFARADI I., HORESH A., FENDER R., GREEN D.A., WILLIAMS D.R.A., BRIGHT J. and SCHULZE S.

Abstract (from CDS):

We report here radio follow-up observations of the optical tidal disruption event (TDE) AT 2019azh. Previously reported X-ray observations of this TDE showed variability at early times and a dramatic increase in luminosity, by a factor of ∼10, about 8 months after optical discovery. The X-ray emission is mainly dominated by intermediate hard-soft X-rays and is exceptionally soft around the X-ray peak, which is LX ∼ 1043 erg s–1. The high cadence 15.5 GHz observations reported here show an early rise in radio emission followed by an approximately constant light curve, and a late-time flare. This flare starts roughly at the time of the observed X-ray peak luminosity and reaches its peak about 110 days after the peak in the X-ray, and a year after optical discovery. The radio flare peaks at νLν ∼ 1038 erg s–1, a factor of two higher than the emission preceding the flare. In light of the late-time radio and X-ray flares, and the X-ray spectral evolution, we speculate a possible transition in the accretion state of this TDE, similar to the observed behavior in black hole X-ray binaries. We compare the radio properties of AT 2019azh to other known TDEs, and focus on the similarities to the late-time radio flare of the TDE ASASSN-15oi.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Radio transient sources - Tidal disruption - Time domain astronomy - Transient sources - Black holes - High energy astrophysics

Simbad objects: 16

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Number of rows : 16
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 XMMSL1 J074008.2-853927 X 07 40 08.2 -85 39 27           ~ 52 0
4 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
5 4C 22.21 BLL 08 23 24.7592164368 +22 23 03.287299236   20.22 19.57 19.7   ~ 186 1
6 SWIFT J1112.2-8238 X 11 11 47.797 -82 38 44.71           ~ 81 0
7 NGC 3690 IG 11 28 31.0 +58 33 41   13.19 12.86     ~ 1015 4
8 NGC 3690B GiP 11 28 31.02 +58 33 40.7   11.8       ~ 635 4
9 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
10 IGR J12580+0134 gam 12 58 05.1 +01 34 26           ~ 50 0
11 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
12 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
13 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 184 0
14 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
15 SWIFT J2058.4+0516 X 20 58 19.898 +05 13 32.25           ~ 169 0
16 AT 2018fyk ev 22 50 16.10 -44 51 53.5           ~ 114 0

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