Accretion and radiation spectrum of the gas debris of a star disrupted by the tidal forces of a massive black hole

Astronomy and Astrophysics – Astronomy

Scientific paper

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Black Holes (Astronomy), Gravitational Effects, Interstellar Gas, Stellar Mass Accretion, Stellar Mass Ejection, Stellar Spectra, Galactic Nuclei, Stellar Radiation, Tides

Scientific paper

When the sustenance of the black hole of a mass Mh situated at the centre of the galactic nucleus is provided mainly by tidal disruptions of surrounding stars (this holds if 103-104 Msun < Mh < 3 108 Msun) the accretion of the gas debris of a star proceeds in a disk regime if Mh is smaller than some critical value Mcr ≍ 105 Msun. In this case the viscous evolution time-scale of the disk is smaller than the time interval between two successive star breakups, and the accretion has a non-stationary character. On the basis of the non-stationary disk model, first considered by Lynden-Bell and Pringle (1974), the main parameters of the disk debris of a disrupted star are obtained as a function of time, including the accretion luminosity of the disk. During a significant part of its evolution the disk is strongly heated by viscous energy dissipation and should be seen as an intense source of X-ray radiation.
As an example of the possible use of the non-stationary model developed, we apply it to obtain a new upper limit to the mass of a black hole presumed located at the centre of our Galaxy. Comparing the X-ray luminosity of the disk with the upper limit to the X-ray flux from the "point" source at the Galactic centre, we find that the mass of the black hole does not exceed about 6 102 Msun.

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