2021ApJ...906...92S


Query : 2021ApJ...906...92S

2021ApJ...906...92S - Astrophys. J., 906, 92-92 (2021/January-2)

Confrontation of observation and theory: high-frequency QPOs in X-ray binaries, tidal disruption events, and active galactic nuclei.

SMITH K.L., TANDON C.R. and WAGONER R.V.

Abstract (from CDS):

We compile observations of high-frequency quasi-periodic oscillations (QPOs) around black holes, both stellar and supermassive, and compare their positions in the parameter space of black hole mass, spin, and oscillation frequency. We find that supermassive black holes occupy a separate region of parameter space than stellar, and further, that QPOs seen around tidal disruption events rather than Seyfert-type active galactic nuclei (AGN) occupy an entirely different space. We then compare these results to the orbital resonance, diskoseismic, warped disk, and disk-jet coupling theoretical models for the origin of high-frequency QPOs. We find that while oscillations around stellar mass black holes are generally consistent with the above models, supermassive black holes are decidedly not. Oscillations seen in tidal disruption events are consistent with oscillations near the frequency of the innermost stable circular orbit, while QPOs in AGN are not accounted for by any of the physical models in consideration. This indicates that despite the scale invariance of accretion processes implied by a decades-wide correlation between QPO frequency and black hole mass, any theory of high-frequency QPOs must relate the frequency to more than just the mass and spin.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Active galactic nuclei - Black holes - X-ray binary stars - High energy astrophysics - Tidal disruption - General relativity

Simbad objects: 21

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Number of rows : 21
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 Ton S 180 Sy1 00 57 20.2040816832 -22 22 56.575212564   14.60 14.34 15.23   ~ 320 0
2 ESO 113-10 Sy2 01 05 16.8746925168 -58 26 15.260456148   14.63 14.6 13.35   ~ 71 0
3 LB 1727 Sy1 04 26 00.7188165240 -57 12 01.769902992 13.68 14.58 14.37 14.8   ~ 307 0
4 LEDA 3095692 Sy1 04 37 28.1562436872 -47 11 29.481984132 14.68 16.61 14.95 15.43   ~ 93 0
5 LEDA 88588 Sy1 07 08 41.4886614696 -49 33 06.308921700   16.02 15.7 12.7   ~ 566 0
6 2CXO J095550.1+694046 HXB 09 55 50.12 +69 40 46.4           ~ 294 1
7 Z 212-25 Sy1 10 34 38.5982990352 +39 38 28.187042604   17.37 16.90     ~ 402 1
8 NGC 4253 Sy1 12 18 26.5163572920 +29 48 46.531535472   14.34 13.57     ~ 1106 1
9 2XMM J123103.2+110648 AG? 12 31 03.239 +11 06 48.60           ~ 56 0
10 ZW VIII 211 rG 12 48 15.2253025968 +17 46 26.475426228   16.5       ~ 360 0
11 MCG-06-30-015 Sy1 13 35 53.7691256160 -34 17 44.160716796   13.89 13.61 8.9   ~ 1559 0
12 2XMM J134736.4+173404 Sy2 13 47 36.3997510944 +17 34 04.578759300           ~ 32 0
13 [FK2005] 25 ULX 14 03 19.63 -41 22 58.7           ~ 252 0
14 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
15 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
16 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60           K4V 422 0
17 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
18 NAME XTE J17464-3213 LXB 17 46 15.59637 -32 14 00.8600           ~ 805 0
19 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
20 RX J1929.8+4622 Sy1 19 29 50.4012314496 +46 22 22.728003024           ~ 23 1
21 LEDA 3096712 Sy1 22 57 39.0250746096 -36 56 06.528333048   16.59 16.0 15.64   ~ 81 0

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