2025A&A...703A..81F


Query : 2025A&A...703A..81F

2025A&A...703A..81F - Astronomy and Astrophysics, volume 703A81 (2025/11-1)

Polarimetric diversity in tidal disruption events: Comparative study of low-polarised sources with AT2020mot.

FLORIS A., LIODAKIS I., KOLJONEN K.I.I., LINDFORS E., AGIS-GONZALEZ B., PAGGI A., BLINOV D., NILSSON K., AGUDO I., CHARALAMPOPOULOS P., DIAZ TEODORI M.A., ESCUDERO PEDROSA J., OTERO-SANTOS J., PIIROLA V., NEWSOME M. and VAN VELZEN S.

Abstract (from CDS):

Context. Tidal disruption events (TDEs) occur when a star is disrupted by the tidal forces of a supermassive black hole (SMBH), which produces bright multi-wavelength flares. Among these events, AT2020mot has so far exhibited the highest recorded optical polarisation, with tidal shocks proposed as the primary source of its polarised emission.
Aims. We present a comprehensive analysis of 13 TDEs with available polarimetric observations, aiming to determine whether the unusually high polarisation of AT2020mot stems from unique physical processes or arises from mechanisms shared by other TDEs.
Methods. We present new optical polarisation measurements of TDEs obtained from multiple ground-based telescopes, combining them with optical, UV, and X-ray light curves from the Zwicky Transient Facility and the Swift observatory. We derived intrinsic TDE properties - such as SMBH and stellar masses - using MOSFiT and TDEMass, and compared them with those of the sample population.
Results. Our population study reveals that AT2020mot aligns with the broader TDE sample in terms of most physical properties, including blackbody temperature, luminosity, and rise timescales. However, its optical polarisation degree is exceptionally high compared to the low or undetected polarisation observed in other events. Additionally, according to our MOSFiT fit, AT2020mot has an elevated column density, which suggests a more complex environment than is typically assumed.
Conclusions. We conclude that although AT2020mot fits well within the general TDE population in terms of global characteristics, its extraordinarily high polarisation and higher column density challenge current models based purely on shock or reprocessing mechanisms. More extensive, time-resolved polarimetric monitoring of newly discovered TDEs will be critical to determine whether AT2020mot represents an outlier or the extreme end of a continuum of TDE properties.

Abstract Copyright: © The Authors 2025

Journal keyword(s): techniques: polarimetric - galaxies: active - galaxies: nuclei

Simbad objects: 29

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Number of rows : 29
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 AT 2022upj ev 00 23 56.846 -14 25 23.22           ~ 30 0
2 LEDA 924801 G 00 23 56.88045 -14 25 24.0431           ~ 4 0
3 WISEA J003113.52+850031.8 G 00 31 13.54 +85 00 31.8   18.84 17.90     ~ 4 0
4 AT 2020mot ev 00 31 13.560 +85 00 31.90           ~ 28 0
5 LEDA 145386 Sy2 03 13 35.6910091320 -02 09 06.352638264   16.75   15.54   ~ 5 0
6 AT 2020afhd ev 03 13 35.700 -02 09 06.37           TDE 9 0
7 AT 2019qiz ev 04 46 37.880 -10 13 34.92           ~ 143 0
8 AT 2022gri ev 07 18 20.778 +33 59 41.58           TDE 3 0
9 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
10 2MASX J09440480-0412051 G 09 44 04.7682617544 -04 12 04.944317976           ~ 2 0
11 AT 2024bgz ev 09 44 04.770 -04 12 04.93           TDE 2 0
12 AT 2022hvp ev 09 54 45.240 +55 26 25.37           ~ 4 0
13 SDSS J095445.23+552625.2 G 09 54 45.2424475267 +55 26 25.322391834           ~ 2 0
14 SDSS J103138.88+345430.0 G 10 31 38.88468 +34 54 30.0097           ~ 1 0
15 AT 2024gre ev 10 31 38.891 +34 54 30.00           TDE 1 0
16 NGC 3799 LIN 11 40 09.3859877328 +15 19 38.408206368   14.4       ~ 80 0
17 ASASSN -23bd ev 11 40 09.397 +15 19 38.54           ~ 18 0
18 NGC 3800 GiC 11 40 13.51680 +15 20 32.4920   13.1       ~ 111 1
19 ASASSN -22ci ev 12 20 45.010 +49 33 04.68           ~ 31 0
20 LEDA 2346329 EmG 12 20 45.0551530248 +49 33 04.623464556           ~ 8 0
21 AT 2022fpx ev 15 31 03.700 +53 24 19.26           ~ 19 0
22 2MASX J16105891-6055250 AG? 16 10 58.8863559654 -60 55 24.411688282           ~ 78 0
23 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
24 SDSS J214044.01+210058.4 G 21 40 44.01584 +21 00 58.4675           ~ 1 0
25 AT 2023ugy ev 21 40 44.020 +21 00 58.57           TDE 3 0
26 AT 2023lli ev 22 57 39.470 +40 32 40.02           ~ 9 0
27 SDSS J232323.37+104101.7 G 23 23 23.41167 +10 41 02.0251           ~ 2 0
28 AT 2022wtn ev 23 23 23.778 +10 41 07.99           ~ 8 0
29 SDSS J232323.79+104107.7 G 23 23 23.79078 +10 41 07.7552           ~ 2 0

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