Upper limits on the masses of 105 supermassive black holes from Hubble Space Telescope / space telescope imaging spectrograph archival data
Based on the modeling of the central emission-line width measured over subarcsecond apertures with the Hubble Space Telescope, we present stringent upper bounds on the mass of the central supermassive black hole, M •, for a sample of 105 nearby galaxies (D < 100 Mpc) spanning a wide range of Hubble types (E–Sc) and values of the central stellar velocity dispersion, σc (58-419 km s–1). For the vast majority of the objects, the derived M • upper limits run parallel and above the well-known M •-σc relation independently of the galaxy distance, suggesting that our nebular line-width measurements trace rather well the nuclear gravitational potential. For values of σc between 90 and 220 km s–1, 68% of our upper limits falls immediately above the M •-σc relation without exceeding the expected M • values by more than a factor 4.1. No systematic trends or offsets are observed in this σc range as a function of the galaxy Hubble type or with respect to the presence of a bar. For 6 of our 12 M • upper limits with σc <90 km s–1, our line-width measurements are more sensitive to the stellar contribution to the gravitational potential, either due to the presence of a nuclear stellar cluster or because of a greater distance compared to the other galaxies at the low-σc end of the M •-σc relation. Conversely, our M • upper bounds appear to lie closer to the expected M • in the most massive elliptical galaxies with values of σc above 220 km s–1. Such a flattening of the M •-σc relation at its high-σc end would appear consistent with a coevolution of supermassive black holes and galaxies driven by dry mergers, although better and more consistent measurements for σc and K-band luminosity are needed for these kinds of objects before systematic effects can be ruled out.
Item Type | Article |
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Uncontrolled Keywords | black hole physics |
Date Deposited | 14 Nov 2024 11:22 |
Last Modified | 14 Nov 2024 11:22 |