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Chandra observations of the supermassive black hole in the nucleus of IC 1459 show a weak ( L X = 8 × 10 40 ergs s -1 , 0.3-8 keV), unabsorbed nuclear X-ray source, with a slope Γ = 1.88 ± 0.09, and no strong Fe K line at 6.4 keV (EW < 382 eV). This describes a normal active galactic nucleus (AGN) X-ray spectrum but lies at 3 × 10 -7 below the Eddington limit. The spectral energy distribution of the IC 1459 nucleus is extremely radio-loud compared to normal radio-loud quasars. The nucleus is surrounded by a hot interstellar medium ( kT ~ 0.5-0.6 keV) with an average density of 0.3 cm -3 , within the central ~180 pc radius, which is comparable to the gravitational capture radius, r A ~ 140 pc. We estimate that for a standard AGN efficiency of 10%, the Bondi accretion would correspond to a luminosity of ~6 × 10 44 ergs s -1 , nearly 4 orders of magnitude higher than L X . ADAF solutions can explain the X-ray spectrum, but not the high radio/X-ray ratio. A jet model fits the radio-100 μm and X-ray spectra well. The total power in this jet is ~10% of L Bondi , implying that accretion close to the Bondi rate is needed.
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Fabbiano et al. (2003) studied this question.
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