2026ApJ..1000..139A


Query : 2026ApJ..1000..139A

2026ApJ..1000..139A - Astrophys. J., 1000, 139 (2026/March-3)

The Multiwavelength Context of Delayed Radio Emission in Tidal Disruption Events: Evidence for Accretion-driven Outflows.

ALEXANDER K.D., MARGUTTI R., GOMEZ S., STROH M., CHORNOCK R., LASKAR T., CENDES Y., BERGER E., EFTEKHARI T., FRANZ N., HAJELA A., METZGER B.D., TERRERAN G., BIETENHOLZ M., CHRISTY C., DE COLLE F., KOMOSSA S., NICHOLL M., RAMIREZ-RUIZ E., SAXTON R., SCHROEDER G., WILLIAMS P.K.G. and WU W.

Abstract (from CDS):

Recent observations presented in Y. Cendes et al. show that optically selected tidal disruption events (TDEs) commonly produce delayed radio emission that can peak years after disruption. Here, we explore the multiwavelength properties of a sample of radio-observed optically selected TDEs, to shed light on the physical process(es) responsible for the late-rising radio emission. We combine new late-time X-ray observations with archival optical, UV, X-ray, and radio data to conclude that a diversity of accretion-driven outflows may power the delayed radio emission in TDEs. Our analysis suggests that some late radio outflows may be launched by a delayed phase of super-Eddington accretion onto the central supermassive black hole (SMBH), while others may result from a state transition to a “low-hard” radiatively inefficient accretion flow or the deceleration of an off-axis relativistic jet. We find that TDEs with delayed radio emission are less likely to exhibit helium emission lines at early times (p = 0.002) and may have larger optical/UV photospheric radii (p = 0.026) than other TDEs, possibly also indicating that the onset of SMBH accretion is delayed in these systems. Our results have implications for our understanding of state changes in SMBH accretion flows, the circularization timescale for TDE debris, and the prevalence of off-axis jets in TDEs, and they motivate systematic long-term monitoring of these unique transients. The objects in our sample with the brightest radio emission are also detected in the Very Large Array Sky Survey, demonstrating that all-sky radio surveys can play an important role in discovering unexpected properties of the TDE population.

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

Journal keyword(s): Tidal disruption - Radio astronomy - Radio transient sources - Accretion - X-ray transient sources - Supermassive black holes - Ultraviolet transient sources - Light curves - Photometry - Relativistic jets - Astronomy data modeling

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 36

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Number of rows : 36
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 Z 500-36 AG? 00 29 57.0542865144 +32 53 37.265932104           ~ 155 0
2 AT 2020mot ev 00 31 13.560 +85 00 31.90           ~ 28 0
3 IRAS 01003-2238 Sy2 01 02 49.9920152640 -22 21 57.262136544   18.62 18.9 17.83   ~ 192 0
4 SDSS J010733.63+232834.2 G 01 07 33.6367520523 +23 28 34.282762347           ~ 37 0
5 OGLE17aaj ev 01 56 24.93 -71 04 15.7           ~ 29 0
6 2MASS J01580475-0052221 Sy1 01 58 04.7506373016 -00 52 21.927742716   18.84 18.34     SNII 114 1
7 NAME Chandra Deep Field-South reg 03 32 28.0 -27 48 30           ~ 2282 1
8 DES14C1kia ev 03 34 47.49 -26 19 35.0           ~ 9 0
9 AT 2019qiz ev 04 46 37.880 -10 13 34.92           ~ 143 0
10 AT 2019ahk ev 07 00 11.410 -66 02 25.16           ~ 57 0
11 AT 2018lna ev 07 03 18.649 +23 01 44.70           ~ 29 0
12 SDSS J075654.53+341543.6 G 07 56 54.5382395520 +34 15 43.641537336           ~ 96 0
13 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
14 AT 2018bsi ev 08 15 26.621 +45 35 31.95           ~ 20 0
15 PTF 15af SN* 08 48 28.13 +22 03 33.4           ~ 69 0
16 AT 2020wey ev 09 05 25.88 +61 48 09.2           ~ 45 0
17 2MASS J10065085+0141342 G 10 06 50.8773292152 +01 41 34.006164648   18.082   17.032   SNII 127 0
18 SDSS J100933.13+232255.7 LIN 10 09 33.1363444488 +23 22 55.694055216           ~ 6 0
19 2MASS J11084011+3405523 G 11 08 40.1149579272 +34 05 52.337925924           ~ 142 0
20 SDSS J112849.64+154022.3 G 11 28 49.6469654133 +15 40 22.339118003           ~ 18 0
21 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
22 SDSS J140941.88+552928.0 AGN 14 09 41.8833027816 +55 29 28.058874792           ~ 55 0
23 NGC 5905 H2G 15 15 23.3280793632 +55 31 01.926808032   13.6       ~ 287 1
24 SDSS J152120.08+140410.5 G 15 21 20.0794689096 +14 04 10.555029480           ~ 36 0
25 AT 2020vwl ev 15 30 37.800 +26 58 56.90           ~ 40 0
26 AT 2020pj ev 15 31 34.960 +33 05 41.47           ~ 17 0
27 AT 2020opy ev 15 56 25.728 +23 22 21.15           ~ 28 0
28 2MASX J16105891-6055250 AG? 16 10 58.8863559654 -60 55 24.411688282           ~ 78 0
29 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
30 AT 2020nov ev 16 58 12.970 +02 07 03.04           ~ 17 0
31 iPTF 16axa ev 17 03 34.36 +30 35 36.8           ~ 54 0
32 2MASS J18590555+4731059 G 18 59 05.55432 +47 31 05.9592           ~ 20 0
33 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 184 0
34 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
35 AT 2017eqx ev 22 26 48.370 +17 08 52.40           ~ 30 0
36 AT 2018fyk ev 22 50 16.10 -44 51 53.5           ~ 114 0

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