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| Query : 2024ApJ...964L..22H |
2024ApJ...964L..22H - Astrophys. J., 964, L22 (2024/April-1)
AT 2023lli: A Tidal Disruption Event with Prominent Optical Early Bump and Delayed Episodic X-Ray Emission.
HUANG S., JIANG N., ZHU J., WANG Y., WANG T., WANG S.-Q., GAN W.-P., LIANG E.-W., QIN Y.-J., LIN Z., XU L.-N., CAI M.-X., JIANG J.-A., KONG X., LI J., LI L., WANG J.-G., XU Z.-L., XUE Y., YUAN Y.-F., CHENG J., FAN L., GAO J., HU L., HU W., LI B., LI F., LIANG M., LIU H., LIU W., LOU Z., LUO W., QIAN Y., TANG J., WAN Z., WANG H., WANG J., YANG J., YAO D., ZHANG H., ZHANG X., ZHAO W., ZHENG X., ZHU Q. and ZUO Y.
Abstract (from CDS):
Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.
Journal keyword(s): Tidal disruption - Supermassive black holes - Black hole physics - Accretion
Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.
Simbad objects: 12
| Number of rows : 12 |
| 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 | M 31 | AGN | 00 42 44.330 | +41 16 07.50 | 4.86 | 4.36 | 3.44 | ~ | 13622 | 1 | ||
| 2 | SN 2018gn | SN* | 01 46 42.385 | +32 30 27.18 | SNII | 17 | 0 | |||||
| 3 | AT 2019qiz | ev | 04 46 37.880 | -10 13 34.92 | ~ | 143 | 0 | |||||
| 4 | ASASSN -14ko | ev | 05 25 18.13 | -46 00 20.3 | SNIIn | 84 | 0 | |||||
| 5 | AT 2019ahk | ev | 07 00 11.410 | -66 02 25.16 | ~ | 57 | 0 | |||||
| 6 | Z 119-12 | SyG | 08 13 16.9505119752 | +22 38 53.905852212 | ~ | 156 | 0 | |||||
| 7 | AT 2019avd | Sy1 | 08 23 36.80 | +04 23 03.4 | ~ | 47 | 0 | |||||
| 8 | AT 2020wey | ev | 09 05 25.88 | +61 48 09.2 | ~ | 45 | 0 | |||||
| 9 | AT 2020vdq | ev | 10 08 53.440 | +42 43 00.23 | ~ | 37 | 0 | |||||
| 10 | Z 160-104 | SyG | 13 02 00.1383745104 | +27 46 57.854731080 | 15.4 | ~ | 159 | 0 | ||||
| 11 | AT 2019mha | ev | 16 16 27.799 | +56 25 56.29 | ~ | 19 | 0 | |||||
| 12 | AT 2023lli | ev | 22 57 39.470 | +40 32 40.02 | ~ | 9 | 0 |
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