2025ApJ...983...29H


Query : 2025ApJ...983...29H

2025ApJ...983...29H - Astrophys. J., 983, 29 (2025/April-2)

Eight Years of Light from ASASSN-15oi: Toward Understanding the Late-time Evolution of TDEs.

HAJELA A., ALEXANDER K.D., MARGUTTI R., CHORNOCK R., BIETENHOLZ M., CHRISTY C.T., STROH M., TERRERAN G., SAXTON R., KOMOSSA S., BRIGHT J.S., RAMIREZ-RUIZ E., COPPEJANS D.L., LEUNG J.K., CENDES Y., WISTON E., LASKAR T., HORESH A., SCHROEDER G., NAYANA A.J., WIERINGA M.H., VELEZ N., BERGER E., BLANCHARD P.K., EFTEKHARI T., GOMEZ S., NICHOLL M., SEARS H. and ZAUDERER B.A.

Abstract (from CDS):

We present results from an extensive follow-up campaign of the tidal disruption event (TDE) ASASSN-15oi spanning δt ∼ 10-3000 days, offering an unprecedented window into the multiwavelength properties of a TDE during its first ≈8 yr of evolution. ASASSN-15oi is one of the few TDEs with strong detections at X-ray, optical/UV, and radio wavelengths and it also featured two delayed radio flares at δt ∼ 180 days and δt ∼ 1400 days. Our observations at δt > 1400 days reveal an absence of thermal X-rays, a late-time variability in the nonthermal X-ray emission, and sharp declines in the nonthermal X-ray and radio emission at δt ∼ 2800 days and ∼3000 days, respectively. The UV emission shows no significant evolution at δt > 400 days and remains above the pre-TDE level. We show that a cooling envelope model can explain the thermal emission consistently across all epochs. We also find that a scenario involving episodic ejection of material due to stream-stream collisions can possibly explain the first radio flare. Given the peculiar spectral and temporal evolution of the late-time emission, however, constraining the origins of the second radio flare and the nonthermal X-rays remains challenging. Our study underscores the critical role of long-term, multiwavelength follow-up to fully characterize the extended evolutionary phases of a TDE.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Tidal disruption - Accretion - Radio transient sources - Ultraviolet transient sources - X-ray transient sources

Simbad objects: 20

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Number of rows : 20
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 CNSS J001947.3+003527 cm 00 19 47.335038 +00 35 26.81020           ~ 32 0
2 Z 500-36 AG? 00 29 57.0542865144 +32 53 37.265932104           ~ 155 0
3 2MASS J01580475-0052221 Sy1 01 58 04.7506373016 -00 52 21.927742716   18.84 18.34     SNII 114 1
4 Z 387-34 Sy1 02 06 15.9896281128 -00 17 29.221733688   15.90 15.50 10.3   ~ 405 0
5 AT 2021ehb ev 03 07 47.806 +40 18 40.57           ~ 42 0
6 AT 2019qiz ev 04 46 37.880 -10 13 34.92           ~ 143 0
7 AT 2019ahk ev 07 00 11.410 -66 02 25.16           ~ 57 0
8 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
9 2MASS J10065085+0141342 G 10 06 50.8773292152 +01 41 34.006164648   18.082   17.032   SNII 127 0
10 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
11 IGR J12580+0134 gam 12 58 05.1 +01 34 26           ~ 50 0
12 AT 2022cmc ev 13 34 43.207 +33 13 00.54           ~ 79 0
13 AT 2020vwl ev 15 30 37.800 +26 58 56.90           ~ 40 0
14 AT 2020opy ev 15 56 25.728 +23 22 21.15           ~ 28 0
15 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
16 ASASSN -15oi SN* 20 39 09.096 -30 45 20.71           ~ 184 0
17 2MASX J20390918-3045201 G 20 39 09.1218039995 -30 45 20.984581933           ~ 10 0
18 PS1-1000789 SN* 20 42 44.7490 +15 30 32.240           SNIIn 39 0
19 2MASX J20570298+1412165 G 20 57 02.9650698480 +14 12 16.295014080           ~ 162 0
20 AT 2018fyk ev 22 50 16.10 -44 51 53.5           ~ 114 0

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