Accurate masses for dispersion-supported galaxies

• Published in: Monthly notices of the Royal Astronomical Society Vol. 406; no. 2; pp. 1220 - 1237
• Main Authors: Wolf, Joe, Martinez, Gregory D., Bullock, James S., Kaplinghat, Manoj, Geha, Marla, Muñoz, Ricardo R., Simon, Joshua D., Avedo, Frank F.
• Format: Journal Article
• Language: English
• Published: Oxford, UK Blackwell Publishing Ltd 01.08.2010; Wiley-Blackwell; Oxford University Press
• Subjects: Astronomy; dark matter; Dispersion; Earth, ocean, space; Exact sciences and technology; galaxies: dwarf; galaxies: elliptical and lenticular; galaxies: elliptical and lenticular, cD; galaxies: formation; galaxies: kinematics and dynamics; Stars & galaxies; galaxies: dwarf; galaxies: elliptical and lenticular, cD; galaxies: formation; galaxies: kinematics and dynamics; dark matter; Luminosity; Spatial variation; Dwarf spheroidal galaxies; Dynamics; Galaxy formation; Cold dark matter; Kinematics; Stellar systems; Virial theorem; Elliptical galaxies; Mass to light ratio; Dispersion relations; Estimator; Globular clusters; Star clusters; Milky Way; Velocity dispersion; Galaxy clusters; Dark matter; Anisotropy; Dwarf galaxies; Cosmology
• ISSN: 0035-8711; 1365-2966
• DOI: 10.1111/j.1365-2966.2010.16753.x

We derive an accurate mass estimator for dispersion-supported stellar systems and demonstrate its validity by analysing resolved line-of-sight velocity data for globular clusters, dwarf galaxies and elliptical galaxies. Specifically, by manipulating the spherical Jeans equation we show that the mass enclosed within the 3D deprojected half-light radius r1/2 can be determined with only mild assumptions about the spatial variation of the stellar velocity dispersion anisotropy as long as the projected velocity dispersion profile is fairly flat near the half-light radius, as is typically observed. We find M1/2= 3 G−1〈σ2los〉r1/2≃ 4 G−1〈σ2los〉Re, where 〈σ2los〉 is the luminosity-weighted square of the line-of-sight velocity dispersion and Re is the 2D projected half-light radius. While deceptively familiar in form, this formula is not the virial theorem, which cannot be used to determine accurate masses unless the radial profile of the total mass is known a priori. We utilize this finding to show that all of the Milky Way dwarf spheroidal galaxies (MW dSphs) are consistent with having formed within a halo of a mass of approximately 3 × 109 M⊙, assuming a Λ cold dark matter cosmology. The faintest MW dSphs seem to have formed in dark matter haloes that are at least as massive as those of the brightest MW dSphs, despite the almost five orders of magnitude spread in luminosity between them. We expand our analysis to the full range of observed dispersion-supported stellar systems and examine their dynamical I-band mass-to-light ratios ϒI1/2. The ϒI1/2 versus M1/2 relation for dispersion-supported galaxies follows a U shape, with a broad minimum near ϒI1/2≃ 3 that spans dwarf elliptical galaxies to normal ellipticals, a steep rise to ϒI1/2≃ 3200 for ultra-faint dSphs and a more shallow rise to ϒI1/2≃ 800 for galaxy cluster spheroids.