Pavel Kroupa, Carsten Weidner, Jan Pflamm-Altenburg, Ingo Thies, Joerg Dabringhausen, Michael Marks, Thomas Maschberger
The current knowledge on the stellar IMF is documented. It is usually
described as being invariant, but evidence to the contrary has emerged: it
appears to become top-heavy when the star-formation rate density surpasses
about 0.1 Msun/(yr pc^3) on a pc scale and it may become increasingly
bottom-heavy with increasing metallicity. It ends quite abruptly below about
0.1 Msun with brown dwarfs (BDs) and very low mass stars having their own IMFs.
The most massive star of mass mmax formed in an embedded cluster with stellar
mass Mecl correlates strongly with Mecl being a result of gravitation-driven
but resource limited growth and fragmentation induced starvation. There is no
convincing evidence whatsoever that massive stars do form in isolation. Massive
stars form above a density threshold in embedded clusters which become
saturated when mmax = mmax\star \approx 150Msun which appears to be the
canonical physical upper mass limit of stars. Super-canonical massive stars
arise naturally due to stellar mergers induced by stellar-dynamical encounters
in very young dense clusters. Various methods of discretising a stellar
population are introduced: optimal sampling leads to a mass distribution that
perfectly represents the exact form of the desired IMF and the mmax-Mecl
relation, while random sampling results in statistical variations of the shape
of the IMF. The observed mmax-Mecl correlation and the small spread of IMF
power-law indices together suggest that optimally sampling the IMF may be the
more realistic description of star formation than random sampling. Composite
populations on galaxy scales, which are formed from many pc scale star
formatiom events, need to be described by the integrated galactic IMF. This
IGIMF varies systematically in dependence of galaxy type and star formation
rate, with dramatic implications for theories of galaxy formation and
evolution.
View original:
http://arxiv.org/abs/1112.3340
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