2026ApJ...998..199W


Query : 2026ApJ...998..199W

2026ApJ...998..199W - Astrophys. J., 998, 199 (2026/February-3)

Delayed Radio Emission in Tidal Disruption Events from Collisions of Outflows Driven by Disk Instabilities.

WU S.C., TSUNA D., MOCKLER B. and PIRO A.L.

Abstract (from CDS):

Delayed radio emission has been associated with a growing proportion of tidal disruption events (TDEs). For many events, the radio synchrotron emission is inferred to originate from the interaction of mildly relativistic outflows, launched with delay times of ∼100-1000 days after the TDE optical peak. The mechanism behind these outflows remains uncertain but may relate to instabilities or state transitions in the accretion disk formed from the TDE. We model the radio emission powered by the collision of mass outflows (“flares”) from TDE accretion disks, considering scenarios in which two successive disk flares collide with each other, as well as collisions between the outflow and the circumnuclear medium (CNM). For flare masses of ∼0.01-0.1 M⊙, varied CNM densities, and different time intervals between ejected flares, we demonstrate that the shocks formed by the collisions have velocities 0.05c-0.3c at ∼1017 cm and power bright radio emission of Lν ∼1027-1030 erg s–1 Hz–1, consistent with the properties inferred for observed events. We quantify how the typical peak timescale and flux varies for different properties of our models, and we compare our model predictions to a selection of TDEs with delayed radio emission. Our models successfully reproduce the light curves and spectral energy distributions for several events, supporting the idea that delayed outflows from disk instabilities and state transitions can power late-time radio emission in TDEs.

Abstract Copyright: © 2026. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Tidal disruption - Radio transient sources - Supermassive black holes - Transient sources

Simbad objects: 18

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Number of rows : 18
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 SDSS J010733.63+232834.2 G 01 07 33.6367520523 +23 28 34.282762347           ~ 37 0
2 2MASS J01580475-0052221 Sy1 01 58 04.7506373016 -00 52 21.927742716   18.84 18.34     SNII 114 1
3 AT 2019qiz ev 04 46 37.880 -10 13 34.92           ~ 143 0
4 AT 2019ahk ev 07 00 11.410 -66 02 25.16           ~ 57 0
5 SDSS J075654.53+341543.6 G 07 56 54.5382395520 +34 15 43.641537336           ~ 96 0
6 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
7 2MASS J10065085+0141342 G 10 06 50.8773292152 +01 41 34.006164648   18.082   17.032   SNII 127 0
8 2MASS J11084011+3405523 G 11 08 40.1149579272 +34 05 52.337925924           ~ 142 0
9 SDSS J112849.64+154022.3 G 11 28 49.6469654133 +15 40 22.339118003           ~ 18 0
10 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
11 AT 2022cmc ev 13 34 43.207 +33 13 00.54           ~ 79 0
12 SDSS J140941.88+552928.0 AGN 14 09 41.8833027816 +55 29 28.058874792           ~ 55 0
13 AT 2020vwl ev 15 30 37.800 +26 58 56.90           ~ 40 0
14 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
15 AT 2024tvd ev 17 10 42.585 +28 50 15.11           ~ 7 0
16 2MASS J18590555+4731059 G 18 59 05.55432 +47 31 05.9592           ~ 20 0
17 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 184 0
18 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0

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