4.6 Article

X-RAY OUTFLOWS AND SUPER-EDDINGTON ACCRETION IN THE ULTRALUMINOUS X-RAY SOURCE HOLMBERG IX X-1

Journal

ASTROPHYSICAL JOURNAL LETTERS
Volume 773, Issue 1, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/2041-8205/773/1/L9

Keywords

black hole physics; X-rays: binaries; X-rays: individual (Holmberg IX X-1)

Funding

  1. Science and Technology Facilities Council [ST/J001538/1, ST/K000861/1, ST/K000985/1, ST/F00723X/1] Funding Source: researchfish
  2. STFC [ST/K000861/1, ST/K000985/1, ST/J001538/1, ST/F00723X/1] Funding Source: UKRI

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Studies of X-ray continuum emission and flux variability have not conclusively revealed the nature of ultraluminous X-ray sources (ULXs) at the high-luminosity end of the distribution (those with L-X >= 10(40) erg s(-1)). These are of particular interest because the luminosity requires either super-Eddington accretion onto a black hole of mass similar to 10 M-circle dot or more standard accretion onto an intermediate-mass black hole. Super-Eddington accretion models predict strong outflowing winds, making atomic absorption lines a key diagnostic of the nature of extreme ULXs. To search for such features, we have undertaken a long, 500 ks observing campaign on Holmberg IX X-1 with Suzaku. This is the most sensitive data set in the iron K bandpass for a bright, isolated ULX to date, yet we find no statistically significant atomic features in either emission or absorption; any undetected narrow features must have equivalent widths less than 15-20 eV at 99% confidence. These limits are far below the greater than or similar to 150 eV lines expected if observed trends between mass inflow and outflow rates extend into the super-Eddington regime and in fact rule out the line strengths observed from disk winds in a variety of sub-Eddington black holes. We therefore cannot be viewing the central regions of Holmberg IX X-1 through any substantial column of material, ruling out models of spherical super-Eddington accretion. If Holmberg IX X-1 is a super-Eddington source, any associated outflow must have an anisotropic geometry. Finally, the lack of iron emission suggests that the stellar companion cannot be launching a strong wind and that Holmberg IX X-1 must primarily accrete via Roche-lobe overflow.

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