Initial mass function

In astronomy, the initial mass function (IMF) is an empirical function that describes the distribution of initial masses for a population of stars. The IMF is often given as a probability distribution function (PDF) for the mass at which a star enters the main sequence (begins hydrogen fusion). The distribution function can then be used to construct the mass distribution (the histogram of stellar masses) of a population of stars. The properties and evolution of a star are closely related to its mass, so the IMF is an important diagnostic tool for astronomers studying large quantities of stars. For example, the initial mass of a star is the primary factor determining its colour, luminosity, and lifetime. The IMF is relatively invariant from one group of stars to another, though some observations suggest that the IMF is different in different environments.[1]

Form of the IMF

Initial mass function

The IMF is often stated in terms of a series of power laws, where (sometimes also represented as ), the number of stars with masses in the range to within a specified volume of space, is proportional to , where is a dimensionless exponent. The IMF can be inferred from the present day stellar luminosity function by using the stellar mass-luminosity relation together with a model of how the star formation rate varies with time. Commonly used forms of the IMF are the Kroupa (2001) broken power law[2] and the Chabrier (2003) log-normal.[3]

Salpeter (1955)

The IMF of stars more massive than our sun was first quantified by Edwin Salpeter in 1955.[4] His work favoured an exponent of . This form of the IMF is called the Salpeter function or a Salpeter IMF. It shows that the number of stars in each mass range decreases rapidly with increasing mass. The Salpeter Initial Mass Function is

where is a constant relating to the local stellar density.

Miller-Scalo (1979)

Later authors extended the work below one solar mass (M). Glenn E. Miller and John M. Scalo suggested that the IMF "flattened" (approached ) below one solar mass.[5]

Chabrier (2003)

Chabrier 2003 for individual stars:

for
for

Chabrier 2003 for stellar systems (e.g. binaries):

for
for

Kroupa (2001)

Pavel Kroupa kept above half a solar mass, but introduced between 0.08-0.5 M and below 0.08 M.

for
for
for

Uncertainties

There are large uncertainties concerning the substellar region. In particular, the classical assumption of a single IMF covering the whole substellar and stellar mass range is being questioned in favour of a two-component IMF to account for possible different formation modes of substellar objects. I.e. one IMF covering brown dwarfs and very-low-mass stars on the one hand, and another ranging from the higher-mass brown dwarfs to the most massive stars on the other. Note that this leads to an overlap region between about 0.05 and 0.2 M where both formation modes may account for bodies in this mass range.[6]

Further reading

References

  1. http://adsabs.harvard.edu/abs/2013ApJ...771...29G
  2. Kroupa, Pavel (2001). "On the variation of the initial mass function". MNRAS. 322: 231–246. Bibcode:2001MNRAS.322..231K. arXiv:astro-ph/0009005Freely accessible. doi:10.1046/j.1365-8711.2001.04022.x.
  3. Chabrier, Gilles (2003). "Galactic stellar and substellar initial mass function". PASP. 115: 763–795. Bibcode:2003PASP..115..763C. arXiv:astro-ph/0304382Freely accessible. doi:10.1086/376392.
  4. Salpeter, Edwin (1955). "The luminosity function and stellar evolution". Astrophysical Journal. 121: 161. Bibcode:1955ApJ...121..161S. doi:10.1086/145971.
  5. Miller, Glenn; Scalo, John (1979). "The initial mass function and stellar birthrate in the solar neighborhood". Astrophysical Journal Supplement Series. 41: 513. Bibcode:1979ApJS...41..513M. doi:10.1086/190629.
  6. Kroupa, Pavel; et al. (2012). "The stellar and sub-stellar IMF of simple and composite populations". Stellar Systems and Galactic Structure, Vol. V. arXiv:1112.3340Freely accessible.
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