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THE SIZES OF THE X-RAY AND OPTICAL EMISSION REGIONS OF RXJ 1131-1231

X. DaiDepartment of Astronomy, University of Michigan, 500 Church Street, Ann Arbor, MI 48109, USAC. S. KochanekCenter for Cosmology and Astroparticle Physics, The Ohio State University, 140 West 18th Avenue, Columbus, OH 43210, USAG. ChartasDepartment of Astronomy and Astrophysics, Pennsylvania State University, University Park, PA 16802, USAS. KozłowskiDepartment of Astronomy, The Ohio State University, 140 West 18th Avenue, Columbus, OH 43210, USAC. W. MorganDepartment of Physics, United States Naval Academy, 572C Holloway Road, Annapolis, MD 21402, USAG. GarmireDepartment of Astronomy and Astrophysics, Pennsylvania State University, University Park, PA 16802, USAE. AgolDepartment of Astronomy, University of Washington, 3910 15th Avenue, Seattle, WA 98105, USA
2009en
ABI

Аннотация

We use gravitational microlensing of the four images of the z=0.658 quasar RXJ1131-1231 to measure the sizes of the optical and X-ray emission regions of the quasar. The (face-on) scale length of the optical disk at rest frame 400 nm is 1.3 10^15cm, while the half-light radius of the rest frame 0.3-17 keV X-ray emission is 2.3 10^14cm. The formal uncertainties are factors of 1.6 and 2.0, respectively. With the exception of the lower limit on the X-ray size, the results are very stable against any changes in the priors used in the analysis. Based on the Hbeta line-width, we estimate that the black hole mass is ~10^8 Msun, which corresponds to a gravitational radius of r_g~2 10^13 cm. Thus, the X-ray emission is emerging on scales of ~10r_g and the 400 nm emission on scales of ~70 r_g. A standard thin disk of this size should be significantly brighter than observed. Possible solutions are to have a flatter temperature profile or to scatter a large fraction of the optical flux on larger scales after it is emitted. While our calculations were not optimized to constrain the dark matter fraction in the lens galaxy, dark matter dominated models are favored. With well-sampled optical and X-ray light curves over a broad range of frequencies there will be no difficulty in extending our analysis to completely map the structure of the accretion disk as a function of wavelength.

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