Journal
ASTROPHYSICAL JOURNAL
Volume 711, Issue 2, Pages 1263-1279Publisher
IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/711/2/1263
Keywords
galaxies: individual (Magellanic Clouds); galaxies: star clusters: general; stars: formation
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We compare the observed bivariate distribution of masses (M) and ages (tau) of star clusters in the Large Magellanic Cloud (LMC) with the predicted distributions g(M, tau) from three idealized models for the disruption of star clusters: (1) sudden mass-dependent disruption, (2) gradual mass- dependent disruption, and ( 3) gradual mass- independent disruption. The model with mass- independent disruption provides a good, first-order description of these cluster populations, with g(M, tau) proportional to M(beta)tau(gamma), beta = -1.8 +/- 0.2 and gamma = -0.8 +/- 0.2, at least for clusters with ages tau less than or similar to 10(9) yr and masses M greater than or similar to 10(3)M(circle dot) (more specifically, tau less than or similar to 10(7)(M/10(2)M(circle dot)) 1.3 yr). This model predicts that the clusters should have a power-law luminosity function, dN/dL proportional to L(-1.8), in agreement with observations. The first two models, on the other hand, fare poorly when describing the observations, refuting previous claims that mass- dependent disruption of star clusters is observed in the LMC over the studied M-tau domain. Clusters in the SMC can be described by the same g(M, tau) distribution as for the LMC, but with smaller samples and hence larger uncertainties. The successful g(M, tau) model for clusters in the Magellanic Clouds is virtually the same as the one for clusters in the merging Antennae galaxies, but extends the domain of validity to lower masses and to older ages. This indicates that the dominant disruption processes are similar in these very different galaxies over at least tau less than or similar to 10(8) yr and possibly tau less than or similar to 10(9) yr. The mass functions for young clusters in the LMC are power laws, while that for ancient globular clusters is peaked. We show that the observed shapes of these mass functions are consistent with expectations from the simple evaporation model presented by McLaughlin & Fall.
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