We show that the globular cluster mass function (GCMF) in the Milky Way depends on cluster half-mass density, ρ h , in the sense that the turnover mass M TO increases with ρ h while the width of the GCMF decreases. We argue that this is the expected signature of the slow erosion of a mass function that initially rose toward low masses, predominantly through cluster evaporation driven by internal two-body relaxation. We find excellent agreement between the observed GCMF—including its dependence on internal density ρ h , central concentration c , and Galactocentric distance r gc —and a simple model in which the relaxation-driven mass-loss rates of clusters are approximated by – dM /dt = μ ev ∝ ρ h 1/2 . In particular, we recover the well-known insensitivity of M TO to r gc . This feature does not derive from a literal ``universality'' of the GCMF turnover mass, but rather from a significant variation of M TO with ρ h —the expected outcome of relaxation-driven cluster disruption—plus significant scatter in ρ h as a function of r gc . Our conclusions are the same if the evaporation rates are assumed to depend instead on the mean volume or surface densities of clusters inside their tidal radii, as μ ev ∝ ρ t 1/2 or μ ev ∝ Σ t 3/4 —alternative prescriptions that are physically motivated but involve cluster properties (ρ t and Σ t ) that are not as well defined or as readily observable as ρ h . In all cases the normalization of μ ev required to fit the GCMF implies cluster lifetimes that are within the range of standard values (although falling toward the low end of this range). Our analysis does not depend on any assumptions or information about velocity anisotropy in the globular cluster system.
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A 2008 study studied this question.