The slope of the black-hole mass versus velocity dispersion correlation
(2002)
Erratum: "A Relationship between Nuclear Black Hole Mass and Galaxy Velocity Dispersion" (ApJ, 539, L13 [2000])
The Astrophysical Journal American Astronomical Society 555:1 (2001) l75-l75
Mass profiles and anisotropies of early-type galaxies
Monthly Notices of the Royal Astronomical Society 322:4 (2001) 702-714
Abstract:
We discuss the problem of using stellar kinematics of early-type galaxies to constrain the orbital anisotropies and radial mass profiles of galaxies. We demonstrate that compressing the light distribution of a galaxy along the line of sight produces approximately the same signature in the line-of-sight velocity profiles as radial anisotropy. In particular, fitting spherically symmetric dynamical models to apparently round, isotropic face-on flattened galaxies leads to a spurious bias towards radial orbits in the models, especially if the galaxy has a weak face-on stellar disc. Such face-on stellar discs could plausibly be the cause of the radial anisotropy found in spherical models of intermediate luminosity ellipticals such as NGC 2434, 3379 and 6703. In the light of this result, we use simple dynamical models to constrain the outer mass profiles of a sample of 18 round, early-type galaxies. The galaxies follow a Tully-Fisher relation parallel to that for spiral galaxies, but fainter by at least 0.8 mag (I-band) for a given mass. The most luminous galaxies show clear evidence for the presence of a massive dark halo, but the case for dark haloes in fainter galaxies is more ambiguous. We discuss the observations that would be required to resolve this ambiguity.Evidence of a supermassive black hole in the galaxy NGC 1023 from the nuclear stellar dynamics
Astrophysical Journal 550:1 PART 1 (2001) 75-86
Abstract:
We analyze the nuclear stellar dynamics of the SBO galaxy NGC 1023, utilizing observational data both from the Space Telescope Imaging Spectrograph aboard the Hubble Space Telescope and from the ground. The stellar kinematics measured from these long-slit spectra show rapid rotation (V ≈ 70 km s-1 at a distance of O″. 1 = 4.9 pc from the nucleus) and increasing velocity dispersion toward the nucleus (where σ = 295 ± 30 km s-1). We model the observed stellar kinematics assuming an axisymmetric mass distribution with both two and three integrals of motion. Both modeling techniques point to the presence of a central dark compact mass (which presumably is a supermassive black hole) with confidence greater than 99%. The isotropic two-integral models yield a best-fitting black hole mass of (6.0 ± 1.4) x 107 MA relationship between nuclear black hole mass and galaxy velocity dispersion (vol 539, pg L13, 2000)
ASTROPHYSICAL JOURNAL 555:1 (2001) L75-L75