期刊
ASTRONOMY & ASTROPHYSICS
卷 494, 期 2, 页码 539-551出版社
EDP SCIENCES S A
DOI: 10.1051/0004-6361:200811212
关键词
Galaxy: open clusters and associations: general; galaxies: star clusters; galaxies: spiral
Aims. The initial cluster mass function (ICMF) in spiral discs is constrained and compared with data for old globular clusters and young clusters in starbursts. Methods. For a given absolute magnitude, the cluster age distribution depends on the ICMF. Here, the behaviour of the median age-magnitude relation is analysed in detail for Schechter ICMFs with various cut-off masses, M(c). The calculated relations are compared with observations of the brightest clusters in spiral galaxies. Schechter functions are also fitted directly to observed mass functions (MFs). Results. A single Schechter ICMF with an M(c) of a few times 10(5) M(circle dot) can reproduce the observed ages and luminosities of the brightest (and 5th brightest) clusters in the spirals if disruption of optically visible clusters is dominated by relatively slow secular evolution. A Schechter function fit to the combined cluster MF for all spirals in the sample yields M(c) = (2.1 +/- 0.4) x 10(5) M(circle dot). The MFs in cluster-poor and cluster-rich spirals are statistically indistinguishable. An M(c) = 2.1 x 10(5) M(circle dot) Schechter function also fits the MF of young clusters in the Large Magellanic Cloud. If the same ICMF applies in the Milky Way, a bound cluster with M > 10(5) M(circle dot) will form about once every 10(7) years, while an M > 10(6) M(circle dot) cluster will form only once every 50 Gyr. Luminosity functions (LFs) of model cluster populations drawn from an M(c) = 2.1 x 10(5) M(circle dot) Schechter ICMF generally agree with LFs observed in spiral galaxies. Conclusions. The ICMF in present-day spiral discs can be modelled as a Schechter function with M(c) approximate to 2 x 10(5) M(circle dot). However, the presence of significant numbers of M > 10(6) M(circle dot) ( and even M > 10(7) M(circle dot)) clusters in some starburst galaxies makes it unlikely that the M(c) value derived for spirals is universal. In high-pressure environments, such as those created by complex gas kinematics and feedback in mergers, M(c) can shift to higher masses than in quiescent discs.
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