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Stellar birth is defined as when nuclear fission begins in a star’s core. Salpeter in 1955 introduced the concept of initial mass function (IMF), which represents the number of stars with a given mass M at stellar birth per unit volume of space (Salpeter, 1955; Moore, 2002). The IMF is assumed to be a power law in the form:

IMF (M) = cM-(1+x) , where x is the parameter of the power law. Salpeter set x at 1.35.

In the Solar neighborhood the IMF = M-2.35 (Moore, 2002). This means that low mass stars are much more likely to form than high mass stars.

The exact nature of the Salpeter constant [x] remains a subject of much investigation, especially for massive stars (Kroupa, 2004). A massive star often has more than one companion which constrains their formation, and a significant fraction of all massive OB stars are found far from their probable birth site, presumably because they were ejected from cores of binary-rich star systems (Kroupa, 2004).

There are theoretical considerations and some observational evidence to suggest star formation in higher metallicity environments appears to produce more low mass stars (Kropa, 2001). Thus, we might postulate that earlier generations of massive stars, such as the purported very early Population III stars, were truly massive compared to the largest Supergiant stars we see today, because, in general, star formation today takes place in the presence of a higher metal content than in earlier epochs of star formation (Mackey, 2003). Unfortunately, there is no strong data thus far to support this conclusion. It appears that the IMF is very uniform over a wide variety of conditions from the formation of low mass brown dwarf stars to very massive stars. According to Kroupa (2004): “This general insight appears to hold for populations including present-day star formation in small molecular clouds, rich and dense massive star-clusters forming in giant clouds, through to ancient and metal-poor exotic stellar populations that may be dominated by dark matter. This apparent universality of the IMF is a challenge for star formation theory, because elementary considerations suggest that the IMF ought to systematically vary with star-forming regions.” Recent work has also shown no deficiency of massive stars at high metallicity (Schaerer, 2003).
 

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