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THE EXTREME SPIN OF THE BLACK HOLE IN CYGNUS X-1

Lijun GouHarvard-Smithsonian Center for Astrophysics, Cambridge, MA 02138, USAJeffrey E. McClintockHarvard-Smithsonian Center for Astrophysics, Cambridge, MA 02138, USAMark J. ReidHarvard-Smithsonian Center for Astrophysics, Cambridge, MA 02138, USAJerome A. OroszDepartment of Astronomy, San Diego State University, San Diego, CA 92182, USAJames F. SteinerHarvard-Smithsonian Center for Astrophysics, Cambridge, MA 02138, USARamesh NarayanHarvard-Smithsonian Center for Astrophysics, Cambridge, MA 02138, USAJingen XiangHarvard-Smithsonian Center for Astrophysics, Cambridge, MA 02138, USARonald A. RemillardKavli Institute for Astrophysics and Space Research, MIT, Cambridge, MA 02139, USAKeith A. ArnaudAstronomy Department, University of Maryland, College Park, MD 20742, USAShane W. DavisCanadian Institute for Theoretical Astrophysics, University of Toronto, Toronto, ON M5S 3H8, Canada
2011en
ABI

Аннотация

The compact primary in the X-ray binary Cygnus X-1 was the first black hole to be established via dynamical observations. We have recently determined accurate values for its mass and distance, and for the orbital inclination angle of the binary. Building on these results, which are based on our favored (asynchronous) dynamical model, we have measured the radius of the inner edge of the black hole's accretion disk by fitting its thermal continuum spectrum to a fully relativistic model of a thin accretion disk. Assuming that the spin axis of the black hole is aligned with the orbital angular momentum vector, we have determined that Cygnus X-1 contains a near-extreme Kerr black hole with a spin parameter a/M>0.95 (3\sigma). For a less probable (synchronous) dynamical model, we find a/M>0.92 (3\sigma). In our analysis, we include the uncertainties in black hole mass, orbital inclination angle and distance, and we also include the uncertainty in the calibration of the absolute flux via the Crab. These four sources of uncertainty totally dominate the error budget. The uncertainties introduced by the thin-disk model we employ are particularly small in this case given the extreme spin of the black hole and the disk's low luminosity.

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