2013MNRAS.435.1758S


Query : 2013MNRAS.435.1758S

2013MNRAS.435.1758S - Mon. Not. R. Astron. Soc., 435, 1758-1775 (2013/October-3)

The ultraluminous state revisited: fractional variability and spectral shape as diagnostics of super-Eddington accretion.

SUTTON A.D., ROBERTS T.P. and MIDDLETON M.J.

Abstract (from CDS):

Although we are nearing a consensus that most ultraluminous X-ray sources (ULXs) below 1041erg/s represent stellar mass black holes accreting in a super-Eddington `ultraluminous' accretion state, little is yet established of the physics of this extreme accretion mode. Here, we use a combined X-ray spectral and timing analysis of an XMM-Newton sample of ULXs to investigate this new accretion regime. We start by suggesting an empirical classification scheme that separates ULXs into three classes based on the spectral morphologies observed by Gladstone et al.: a singly peaked broadened disc class, and two-component hard ultraluminous and soft ultraluminous regimes, with the spectra of the latter two classes dominated by the harder and softer component, respectively. We find that at the lowest luminosities (LX < 3x1039erg/s) the ULX population is dominated by sources with broadened disc spectra, whilst ULXs with two-component spectra are seen almost exclusively at higher luminosities, suggestive of a distinction between ∼ Eddington and super-Eddington accretion modes. We find high levels of fractional variability are limited to ULXs with soft ultraluminous spectra, and a couple of the broadened disc sources. Furthermore, the variability in these sources is strongest at high energies, suggesting it originates in the harder of the two spectral components. We argue that these properties are consistent with current models of super-Eddington emission, where a massive radiatively driven wind forms a funnel-like geometry around the central regions of the accretion flow. As the wind provides the soft spectral component this suggests that inclination is the key determinant in the observed two-component X-ray spectra, which is very strongly supported by the variability results if this originates due to clumpy material at the edge of the wind intermittently obscuring our line-of-sight to the spectrally hard central regions of the ULX. The pattern of spectral variability with luminosity in two ULXs that straddle the hard/soft ultraluminous regime boundary is consistent with the wind increasing at higher accretion rates, and thus narrowing the opening angle of the funnel. Hence, this work suggests that most ULXs can be explained as stellar mass black holes accreting at and above the Eddington limit, with their observed characteristics dominated by two variables: accretion rate and inclination.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): accretion, accretion discs - black hole physics - X-rays: binaries - X-rays: galaxies

Simbad objects: 22

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Number of rows : 22
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 [BWE2015] NGC 55 119 ULX 00 15 28.89 -39 13 18.8           ~ 73 0
2 CXOM31 J004253.1+411422 ULX 00 42 53.15 +41 14 22.9           ~ 28 0
3 RX J004722.4-252051 ULX 00 47 22.59 -25 20 50.9           ~ 43 0
4 RX J004732.9-251748 ULX 00 47 32.97 -25 17 50.2           ~ 35 0
5 ChASeM33 J013350.89+303936.6 SNR 01 33 50.8965749232 +30 39 36.630403128           ~ 95 1
6 RX J031820.3-662911 UX? 03 18 20.00 -66 29 10.9           ~ 229 1
7 2E 756 ULX 03 18 22.00 -66 36 04.3   23.5 23.6     O9.5 262 3
8 [SST2011] J034555.61+680455.3 ULX 03 45 55.612 +68 04 55.29           ~ 176 1
9 2XMM J034606.5+680705 ULX 03 46 07.3 +68 07 06           ~ 16 0
10 [FK2005] 6 ULX 07 36 25.55 +65 35 40.0           ~ 44 0
11 [SST2011] J081929.00+704219.3 ULX 08 19 28.99 +70 42 19.4           ~ 213 2
12 [FK2005] 7 SNR 09 55 32.95 +69 00 33.6   23.87 23.89     ~ 86 1
13 2CXO J095550.1+694046 HXB 09 55 50.12 +69 40 46.4           ~ 294 1
14 RX J0957.9+6903 ULX 09 57 53.290 +69 03 48.20           ~ 246 4
15 CXO J121345.2+363754 ULX 12 13 45.41 +36 37 55.2           ~ 19 0
16 RX J123551+27561 ULX 12 35 51.71 +27 56 04.1           ~ 79 1
17 2XMM J125048.6+410743 ULX 12 50 48.6 +41 07 43           ~ 7 0
18 [FK2005] 23 ULX 13 29 38.62 +58 25 05.6           ~ 134 2
19 [FK2005] 25 ULX 14 03 19.63 -41 22 58.7           ~ 252 0
20 NAME NGC 5907 ULX ULX 15 15 58.60 +56 18 10.0           ~ 180 0
21 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
22 NAME NGC 6946 SNR SNR 20 35 00.74 +60 11 30.6           ~ 117 0

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