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The time formation for massive stars is so short they reach the zero-age Main Sequence (ZAMS) while still embedded in their birth clouds (Feldt, 2003). This makes it quite difficult to follow the birth and development of massive stars. Moreover, massive star formation takes place in distant complex molecular clouds. It is thought massive stars form almost exclusively in a clustered mode (Beuther, 2004). Observational and theoretical work has shown that massive stars can be formed via disk accretion (McKee, 2003; Yorke, 2002). It is also possible intermediate-mass protostars may merge to form more massive stars through collisions and interactions in the molecular clouds. Recent, high-spatial-resolution interferometric dust continuum observations have enabled the derivation of a protocluster mass distribution function for the massive star forming region IRAS 19410+2336 (Beuther, 2004). The initial results show a mass distribution consistent with the commonly accepted stellar initial mass function. Fragmentation of the initial mass cores in stellar forming regions probably determines the masses of the final stars. According to Beuther (2004): “This implies that stars of all masses can form via accretion processes, and coalescence of intermediate-mass protostars appears not to be necessary.”

Massive stars generally end their lives as type II supernovae. The yields of Type II supernovae alpha elements, such as, O, Mg, and Ne, are a function of the progenitor’s mass, whereas the yield of a supernova’s explosive reaction elements, such as Fe, Si, and Ca is not as closely related to the star’s original mass prior to its explosion (Gibson, 1998). Looking at the yields of these two groups of elements for various Type II supernovae and tying these yields to element abundances in metal poor stars in the Galactic halo gives an “indirect probe for the upper mass limit to the IMF” (Gibson, 1998). Unfortunately, there are substantial uncertainties for these yields. Looking at this question in detail, Gibson (1998) states: “…we simply cannot constrain the upper limit to mU to anything better than ~ 60-200 Mo.”
 

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