2026MNRAS.545f2093P


Query : 2026MNRAS.545f2093P

2026MNRAS.545f2093P - Mon. Not. R. Astron. Soc., 545, part no 6, 2093 (2026/January-3)

MUSE IFU observations of galaxies hosting tidal disruption events.

PURSIAINEN M., LELOUDAS G., LYMAN J., BYRNE C.M., CHARALAMPOPOULOS P., RAMSDEN P., KIM S., SCHULZE S., ANDERSON J.P., BAUER F.E., DAI L., GALBANY L., KUNCARAYAKTI H., NICHOLL M., PESSI T., PRIETO J.L. and SANCHEZ S.F.

Abstract (from CDS):

We present an analysis of 20 tidal disruption events (TDEs) host galaxies observed with the Multi-Unit Spectroscopic Explorer (MUSE) integral-field spectrograph on European Southern Observatory (ESO) Very Large Telescope (VLT). We investigate the presence of extended emission line regions (EELRs) and study stellar populations mostly at sub-kpc scale around the host nuclei. EELRs are detected in 5/20 hosts, including two unreported systems. All EELRs are found at $z<0.045$, suggesting a distance bias and faint EELRs may be missed at higher redshift. EELRs only appear in post-merger systems and all such hosts at $z<0.045$ show them. Thus, we conclude that TDEs and galaxy mergers have a strong relation, and >45 per cent of post-merger hosts in the sample exhibit EELRs. Furthermore, we constrained the distributions of stellar masses near the central black holes (BHs), using the spectral synthesis code STARLIGHT and BPASS stellar evolution models. The youngest nuclear populations have typical ages of $\sim$1 Gyr and stellar masses below $2.5\,\mathrm{ M}_\odot$. The populations that can produce observable TDEs around non-rotating BHs are dominated by sub-solar-mass stars. 3/4 TDEs requiring larger stellar masses exhibit multipeaked light curves, possibly implying relation to repeated partial disruptions of high-mass stars. The found distributions are in tension with the masses of the stars derived using light curve models. Mass segregation of the disrupted stars can enhance the rate of TDEs from supersolar-mass stars but our study implies that low-mass TDEs should still be abundant and even dominate the distribution, unless there is a mechanism that prohibits low-mass TDEs or their detection.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): galaxies: starburst - galaxies: star formation - transients: tidal disruption events

Simbad objects: 22

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Number of rows : 22
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 2019qiz ev 04 46 37.880 -10 13 34.92           ~ 143 0
3 ASASSN -14ko ev 05 25 18.13 -46 00 20.3           SNIIn 84 0
4 AT 2019ahk ev 07 00 11.410 -66 02 25.16           ~ 57 0
5 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
6 PTF 15af SN* 08 48 28.13 +22 03 33.4           ~ 69 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 ASASSN -23bd ev 11 40 09.397 +15 19 38.54           ~ 18 0
10 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
11 2MASX J13424441+0530560 AG? 13 42 44.4175903032 +05 30 56.125206936           ~ 25 0
12 PTF 09axc SN* 14 53 13.06 +22 14 32.2           SNII 52 0
13 SDSS J152120.08+140410.5 G 15 21 20.0794689096 +14 04 10.555029480           ~ 36 0
14 2MASX J16105891-6055250 AG? 16 10 58.8863559654 -60 55 24.411688282           ~ 78 0
15 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 184 0
16 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
17 ASASSN -15lh ev 22 02 15.4 -61 39 34           ~ 187 1
18 AT 2017eqx ev 22 26 48.370 +17 08 52.40           ~ 30 0
19 AT 2018fyk ev 22 50 16.10 -44 51 53.5           ~ 114 0
20 AT 2019lwu ev 23 11 12.305 -01 00 10.71           ~ 17 0
21 LSQ 12dyw SN* 23 29 24.82 -07 23 20.4           SNIcpec 7 0
22 [GHC2009] D23H-1 G 23 31 59.5395591768 +00 17 14.595290952   20.67   19.30 18.83 ~ 27 0

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