2025A&A...704A...3K


Query : 2025A&A...704A...3K

2025A&A...704A...3K - Astronomy and Astrophysics, volume 704A3 (2025/12-1)

Identifying tidal disruption events among radio transient galaxies.

KUNERT-BAJRASZEWSKA M., KOZIEL-WIERZBOWSKA D., STERN D., KRAUZE A., ZAFAR N., CONNOR T. and GRAHAM M.J.

Abstract (from CDS):

We present the optical and infrared properties of a sample of 24 radio transient sources discovered in the Very Large Array Sky Survey (VLASS). Previous studies of their radio emission showed that these sources resemble young gigahertz-peaked spectrum (GPS) radio sources, but they are less powerful and characterized by low-power jets. The bursts of radio activity in most cases are likely due to intrinsic changes in the accretion processes. However, for a few sources in this sample, we cannot rule out the possibility that their radio variability results from a tidal disruption event (TDE). In this work, we extended our analysis to the optical and infrared regimes, confirming that our sample of radio transients is not homogeneous in terms of their optical and infrared properties either. The host galaxies of most of these sources are massive ellipticals with emission dominated by active galactic nuclei (AGNs). They host supermassive black holes (SMBHs) with masses typical of radio-loud AGNs (> 107 M⊙), but they exhibit very low accretion activity. In contrast, the sources for which a TDE origin is suspected are either pure star-forming galaxies or show significant ongoing star formation, similar to radio-selected, optically detected TDEs. Additionally, two of them exhibit infrared flares characteristic of TDEs, while the remaining sources do not display significant variability outside the radio regime. Moreover, the evolution of their radio brightness in the W3-radio diagnostic diagram - which we employed in our analysis - also sets our TDE candidates apart from the rest of the sample and resembles the radio variability seen in optically discovered TDEs with radio emission. Finally, based on our findings, we hypothesize that the W3-radio relation can serve as a tool to distinguish between radio transients caused by TDEs and those originating from intrinsic AGN variability.

Abstract Copyright: © The Authors 2025

Journal keyword(s): galaxies: active - quasars: supermassive black holes - galaxies: Seyfert

Simbad objects: 38

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Number of rows : 38
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 SDSS J010733.63+232834.2 G 01 07 33.6367520523 +23 28 34.282762347           ~ 37 0
3 2MASS J01580475-0052221 Sy1 01 58 04.7506373016 -00 52 21.927742716   18.84 18.34     SNII 114 1
4 2dFGRS TGS314Z138 LIN 02 43 45.6935985144 -28 40 39.948028755   18.155   16.932   ~ 7 0
5 2MASX J02460935+3408206 G 02 46 09.3256375363 +34 08 20.289195826           ~ 3 0
6 2MASS J03111549+0851323 G 03 11 15.4892402152 +08 51 32.464850106           ~ 2 0
7 2MASS J05351028+8345412 rG 05 35 10.1988837658 +83 45 41.433065772           ~ 3 0
8 2MASX J06400181+2803068 AGN 06 40 01.8128674433 +28 03 06.873391175           ~ 2 0
9 2MASS J07083784+3204208 AGN 07 08 37.84056 +32 04 20.8992           ~ 2 0
10 2MASX J07182930+5942517 LIN 07 18 29.3162839984 +59 42 52.142657497           ~ 2 0
11 SDSS J075654.53+341543.6 G 07 56 54.5382395520 +34 15 43.641537336           ~ 96 0
12 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
13 2MASS J09514158+3703344 AGN 09 51 41.6102314438 +37 03 34.562964260           ~ 3 0
14 2MASS J10065085+0141342 G 10 06 50.8773292152 +01 41 34.006164648   18.082   17.032   SNII 127 0
15 6dFGS gJ101841.4-130007 Sy2 10 18 41.4362482368 -13 00 06.858725940   16.65   15.43   ~ 8 0
16 2MASX J10503574-0745028 G 10 50 35.7381104125 -07 45 02.296418892           ~ 3 0
17 PSO J165.6631-06.1973 QSO 11 02 39.1595023349 -06 11 50.627004168           ~ 2 0
18 2MASS J11084011+3405523 G 11 08 40.1149579272 +34 05 52.337925924           ~ 142 0
19 SDSS J112849.64+154022.3 G 11 28 49.6469654133 +15 40 22.339118003           ~ 18 0
20 2MASX J11293994+3900468 G 11 29 40.022 +39 00 46.57           ~ 3 0
21 2MASS J11410178+1028213 LIN 11 41 01.7904748889 +10 28 21.200429666           ~ 2 0
22 2MASX J12161962+1240274 G 12 16 19.6217296944 +12 40 27.640940808           ~ 6 0
23 LCRS B130123.2-114253 G 13 04 00.7123805160 -11 58 57.736436772   17.49   15.91   ~ 7 0
24 SDSS J140941.88+552928.0 AGN 14 09 41.8833027816 +55 29 28.058874792           ~ 55 0
25 Z 165-6 BiC 15 04 15.8762757768 +28 29 47.608342008           ~ 20 0
26 SDSS J152120.08+140410.5 G 15 21 20.0794689096 +14 04 10.555029480           ~ 36 0
27 Z 79-16 LIN 15 58 47.6808091104 +14 12 13.410944892           ~ 16 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 MCG+07-34-146 AGN 16 46 07.0044876048 +42 27 37.459823940           ~ 12 0
31 2MASX J18094050+2436408 G 18 09 40.50287 +24 36 40.8020           ~ 2 0
32 2MASS J18341542+6124007 AGN 18 34 15.4057200036 +61 24 00.754409797           ~ 2 0
33 2MASS J18590555+4731059 G 18 59 05.55432 +47 31 05.9592           ~ 20 0
34 2MASX J19533525-0452030 G 19 53 35.2089804936 -04 52 03.633017448           ~ 4 0
35 2MASX J20390918-3045201 G 20 39 09.1218039995 -30 45 20.984581933           ~ 10 0
36 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
37 2MASX J22393322-2231272 G 22 39 33.2644443571 -22 31 27.134843221           ~ 3 0
38 2MASX J23305893+1000298 G 23 30 58.8936155729 +10 00 30.064520914           ~ 4 0

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