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The effect of advection at luminosities close to Eddington: The ULX in M 31

Authors :
Matthew J. Middleton
Chris Done
Odele Straub
Laboratoire Univers et Théories (LUTH (UMR_8102))
Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de Paris
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Diderot - Paris 7 (UPD7)
High Energy Astrophys. & Astropart. Phys (API, FNWI)
Source :
Astronomy and Astrophysics-A&A, Astronomy and Astrophysics-A&A, EDP Sciences, 2013, 553, pp.A61. ⟨10.1051/0004-6361/201321324⟩, Astronomy & Astrophysics, 553. EDP Sciences
Publication Year :
2013
Publisher :
EDP Sciences, 2013.

Abstract

The transient, ultra-luminous X-ray source CXOM31 J004253.1+411422 in the Andromeda galaxy is most likely a 10 solar mass black hole, with super-Eddington luminosity at its peak. The XMM-Newton spectra taken during the decline then trace luminosities of 0.86-0.27 L_Edd. These spectra are all dominated by a hot disc component, which roughly follows a constant inner radius track in luminosity and temperature as the source declines. At the highest luminosity the disc structure should change due to advection of radiation through the disc. This advected flux can be partly released at lower radii thus modifying the spectral shape. To study the effect of advection at luminosities close to Eddington we employ a fully relativistic slim disc model, SLIMBH, that includes advective cooling and full radiative transfer through the photosphere based on TLUSTY. The model also incorporates relativistic photon ray-tracing from the proper location of the disc photosphere rather than the mid-plane as the slim disc is no longer geometrically thin. We find that these new models differ only slightly from the non-advective (standard) BHSPEC models even at the highest luminosities considered here. While both discs can fit the highest luminosity data, neither is a very good fit to the *lower* luminosities. This could indicate a missing physical process that acts in low luminosity discs and subsides as the disc luminosity approaches the Eddington limit.<br />Comment: 5 pages, 4 figures, improved figures

Details

ISSN :
14320746 and 00046361
Volume :
553
Database :
OpenAIRE
Journal :
Astronomy & Astrophysics
Accession number :
edsair.doi.dedup.....627ebf4a56d6bb3184d6c3c9592ce2f4
Full Text :
https://doi.org/10.1051/0004-6361/201321324