4.1 Article

Galactic black-hole candidates shining at the Eddington luminosity

Journal

PUBLICATIONS OF THE ASTRONOMICAL SOCIETY OF JAPAN
Volume 52, Issue 1, Pages 133-141

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/pasj/52.1.133

Keywords

accretion, accretion disks; black holes; stars : X-rays

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We discuss distinctive features of luminous secretion disks shining at the Eddington luminosity in the context of galactic black-hole candidates (GBCs). We first note that the standard-disk picture is not applicable, although it is often postulated. Rather, the disk becomes advection-dominated while remaining optically thick (the so-called slim disk). The slim disk exhibits several noteworthy signatures: (1) The disk luminosity is insensitive to the mass-flow rates, (M) over dot, and is always kept around the Eddington luminosity, L-E, even if (M) over dot greatly exceeds L-E/c(2). This reflects the fact that radiative cooling is no longer balanced by viscous heating and excess energy is carried by accreting matter to black holes. (2) The spectra of the slim disks are multi-color blackbody characterized by (i) a high maximum temperature, kT(in) similar to a few keV, (ii) a small size of an emitting region, r(in) < 3r(g) (with r(g) being Schwarzschild radius), due to substantial radiation coming out from inside 3r(g), and (iii) flatter spectra in the soft-X bands, nu S-nu proportional to nu(0), because of a flatter effective temperature profile of the slim disk, T-eff proportional to r(-1/2) (in contrast with T-eff proportional to r(-3/4) in the standard disk). Thus, a small r(in)(much less than 3r(g)) does not necessarily mean the presence of a Kerr hole. Furthermore, (3) as (M) over dot increases, T-in increases, while r(in) decreases as r(in) proportional to (T-in)(-1) approximately. That is, the changes in r(in) derived from the fitting do not necessarily mean the changes in the physical boundary of the optically thick portions of the disk. Observational implications are discussed in relation to binary jet sources.

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