2024ApJ...976...34Y


Query : 2024ApJ...976...34Y

2024ApJ...976...34Y - Astrophys. J., 976, 34 (2024/November-3)

Subrelativistic Outflow and Hours-timescale Large-amplitude X-Ray Dips during Super-Eddington Accretion onto a Low-mass Massive Black Hole in the Tidal Disruption Event AT2022lri.

YAO Y., GUOLO M., TOMBESI F., LI R., GEZARI S., GARCIA J.A., DAI L., CHORNOCK R., LU W., KULKARNI S.R., GENDREAU K.C., PASHAM D.R., CENKO S.B., KARA E., MARGUTTI R., AJAY Y., WEVERS T., KWAN T.M., ANDREONI I., BLOOM J.S., DRAKE A.J., GRAHAM M.J., HAMMERSTEIN E., LAHER R.R., LEBARON N., MAHABAL A.A., O'CONNOR B., PURDUM J., RAVI V., SEARS H., SHARMA Y., SMITH R., SOLLERMAN J., SOMALWAR J.J. and WOLD A.

Abstract (from CDS):

We present the tidal disruption event (TDE) AT2022lri, hosted in a nearby (≈144 Mpc) quiescent galaxy with a low-mass massive black hole (104M⊙ < MBH < 106M⊙). AT2022lri belongs to the TDE-H+He subtype. More than 1 Ms of X-ray data were collected with NICER, Swift, and XMM-Newton from 187 to 672 days after peak. The X-ray luminosity gradually declined from 1.5 × 1044 erg s–1 to 1.5 × 1043 erg s–1 and remains much above the UV and optical luminosity, consistent with a super-Eddington accretion flow viewed face-on. Sporadic strong X-ray dips atop a long-term decline are observed, with a variability timescale of ≈0.5 hr-1 days and amplitude of ≈2-8. When fitted with simple continuum models, the X-ray spectrum is dominated by a thermal disk component with inner temperature going from ∼146 to ∼86 eV. However, there are residual features that peak around 1 keV, which, in some cases, cannot be reproduced by a single broad emission line. We analyzed a subset of time-resolved spectra with two physically motivated models describing a scenario either where ionized absorbers contribute extra absorption and emission lines or where disk reflection plays an important role. Both models provide good and statistically comparable fits, show that the X-ray dips are correlated with drops in the inner disk temperature, and require the existence of subrelativistic (0.1-0.3c) ionized outflows. We propose that the disk temperature fluctuation stems from episodic drops of the mass accretion rate triggered by magnetic instabilities or/and wobbling of the inner accretion disk along the black hole's spin axis.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Tidal disruption - X-ray transient sources - Supermassive black holes - Time domain astronomy - High energy astrophysics - Accretion

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 28

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Number of rows : 28
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 OGLE16aaa ev 01 07 20.88 -64 16 20.7           ~ 72 0
2 LEDA 809836 G 02 20 08.0 -22 43 14           ~ 2 0
3 AT 2022lri ev 02 20 08.009 -22 43 15.42           ~ 9 0
4 ASASSN -20qc SN? 04 13 02.379 -53 04 21.80           ~ 16 0
5 3C 111 Sy1 04 18 21.2772425736 +38 01 35.801359968   19.75 18.05     ~ 1002 2
6 AT 2018lna ev 07 03 18.649 +23 01 44.70           ~ 29 0
7 XMMSL1 J074008.2-853927 X 07 40 08.2 -85 39 27           ~ 52 0
8 2MASX J07400785-8539307 GiG 07 40 08.2115762784 -85 39 31.349719944           ~ 18 0
9 SDSS J075654.53+341543.6 G 07 56 54.5382395520 +34 15 43.641537336           ~ 96 0
10 Z 119-12 SyG 08 13 16.9505119752 +22 38 53.905852212           ~ 156 0
11 AT 2019avd Sy1 08 23 36.80 +04 23 03.4           ~ 47 0
12 AT 2020wey ev 09 05 25.88 +61 48 09.2           ~ 45 0
13 AT 2020vdq ev 10 08 53.440 +42 43 00.23           ~ 37 0
14 2MASS J11084011+3405523 G 11 08 40.1149579272 +34 05 52.337925924           ~ 142 0
15 XMMSL1 J120135.7+300306 X 12 01 35.7 +30 03 06           ~ 3 0
16 2MASS J12013602+3003052 G 12 01 36.0281668104 +30 03 05.576406012           ~ 47 0
17 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
18 AT 2022cmc ev 13 34 43.207 +33 13 00.54           ~ 79 0
19 AT 2020ocn ev 13 53 53.803 +53 59 49.57           ~ 38 0
20 SDSS J140941.88+552928.0 AGN 14 09 41.8833027816 +55 29 28.058874792           ~ 55 0
21 2MASX J14510879+2709272 Sy1 14 51 08.7647938560 +27 09 26.962707132   15.01 15.01     ~ 239 0
22 SDSS J152120.08+140410.5 G 15 21 20.0794689096 +14 04 10.555029480           ~ 36 0
23 AT 2020vwl ev 15 30 37.800 +26 58 56.90           ~ 40 0
24 2MASX J16105891-6055250 AG? 16 10 58.8863559654 -60 55 24.411688282           ~ 78 0
25 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
26 RX J1927.3+6533 Sy2 19 27 19.5393064368 +65 33 54.335877408     15.4     ~ 147 0
27 NAME SRGe J213527.3-181634 ev 21 35 27.25 -18 16 35.5           ~ 14 0
28 eRASSt J234402.9-352640 X 23 44 02.90 -35 26 39.4           ~ 10 0

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