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Статья

Planetary Camera observations of the M87 stellar cusp

Tod R. LauerNational Optical Astronomy Observatoires, Tucson, AZS. M. FaberLick Observatory, Santa Cruz, CARoger LyndsW. A. BaumWashington, University, SeattleS. P. EwaldSpace Telescope Science Institute, Baltimore, MDE. J. GrothPrinceton University, NJJ. J. HesterCalifornia Institute of Technology, Pasadena, CAJon A. HoltzmanLowell Observatory, Flagstaff, AZJ. KristianObservatoires of the Carnegie Institution of Washington, Pasadena, CAR. M. LightLick Observatory, Santa Cruz, CAJr. O'Neil E. J.Donald P. SchneiderE. Shaya-James A. Westphal-
1992en
ABI

Аннотация

Analysis of V and I band HST Planetary Camera images of the giant elliptical galaxy M87 show that its central starlight distribution is consistent with the black hole M_black hole_ = 2.6 X 10^9^ M_sun_ cusp model proposed for M87 by Young et al, [ApJ, 221,721(1978)]. A combined approach of image deconvolution and modeling is used to investigate the starlight distribution into limiting radii of ~0.04" (3 pc at 16 Mpc). The central structure of M87 can be described by three components: a power-law starlight profile of the form μ(r) is proportional to r^- 1/4^ for r < 3", a central nonthermal point source, and optical counterparts of the jet knots N1 and M identified by VLBI observations. M87 lacks a constant surface brightness core, and its central starlight luminosity density exceeds 10^3^L_sun_ pc^-3^ (I band) for r < 10 pc. The profile strongly resembles a stellar cusp associated with a massive black hole. A review of existing velocity dispersion observations suggests that the Young et al. black hole mass can be accommodated to the observations with minor adjustments of dynamical models. The central luminosity spike itself remains unresolved at HST resolution, with r_c_ < 1 pc. The spike has optical spectral index α = - 0.46+/-0.20 and is at least as blue if not bluer than the rest of the M87 jet. The total nonthermal flux in the inner 1" of M87 agrees well with the central radio flux and the radio-optical spectral index of the rest of the jet. It is also consistent with the spectral-line dilution seen by Dressler & Richstone [ApJ, 348,120(1990); we thus argue that the spike is completely nonthermal.

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