Table A.1.
Precursor sample.
| ID | TDE type | tocc.time | precursor ref. | log(MBH/M⊙) | MBH ref. | p | p ref. |
|---|---|---|---|---|---|---|---|
| (days) | |||||||
| AT2019azh | repeating | 18 ± 4 | Huang et al. (2024), Faris et al. (2024) | 6.24 ± 0.30 | Mummery et al. (2024) | ||
| AT2024pvu | repeating | 39![]() |
this work | 7.13 ± 0.80 | this work | ||
| AT2022dbl | repeating | 18 ± 3 | this work | 6.21 ± 0.52 | this work | ||
| AT2023uqm | repeating | 105![]() |
this work, Wang et al. (2025) | 7.14 ± 0.55 | Wang et al. (2025) | ||
| AT2020wey | fast | 11 ± 3 | Charalampopoulos et al. (2023) | 5.20 ± 0.52 | Mummery et al. (2024) | −2.84 ± 0.18 | Charalampopoulos et al. (2023) |
| AT2023lli | fast | 39![]() |
Huang et al. (2024) | 6.66 ± 0.34 | this work | −4.1 | Huang et al. (2024) |
| AT2019qiz | fast | 10 ± 2 | Wang et al. (2024b) | 6.35 ± 0.30 | Mummery et al. (2024) | −2.51 ± 0.03 | Charalampopoulos et al. (2023) |
| AT2019mha | fast | 24 ± 7 | Wang et al. (2024b) | 6.71 ± 0.80 | Mummery et al. (2024) | ![]() |
van Velzen et al. (2021) |
| AT2020zso | fast? TDE-AGN | 8![]() |
Wang et al. (2024b) | 6.06 ± 0.30 | Mummery et al. (2024) | ![]() |
Hammerstein et al. (2023) |
| AT2022fpx | TDE-AGN | > 125 | Koljonen et al. (2024) | 6.62 ± 0.58 | Koljonen et al. (2024) | ||
| AT2018gn | TDE-AGN | 30 ± 5 | Wang et al. (2024b) | 6.46![]() |
Wang et al. (2024b) | ||
| AT2024kmq | TDE-AGN | 48 ± 10 | Ho et al. (2025) | 8.04 ± 0.30 | this work | ||
| AT2019ahk | TDE-AGN | 32 ± 5a | Wang et al. (2024b) | 6.80 ± 0.80 | Holoien et al. (2019) | ||
| AT2019aalc | repeating TDE-AGN | 364![]() |
this work | 7.23 ± 0.30 | van Velzen et al. (2024) | ||
| AT2021aeuk | repeating TDE-AGN | 239![]() |
Sun et al. (2025) | 7.30![]() |
Bao et al. (2024) | ||
| ASASSN-14ko | repeating TDE-AGN | ∼ 20 b | Huang et al. (2025) | 7.86![]() |
Payne et al. (2021) |
Notes.tocc.time denotes the occurrence time of the precursor relative to the primary peak, while the associated uncertainties represent the precursor duration. The parameter p gives the power-law index of the bolometric light curve decay for fast TDEs.
The precursor appears only in the bolometric light curve.
The precursors appear on different timescales across different flaring episodes.
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