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2. WHAT WE DON'T KNOW ABOUT STARS

The ``bread and butter'' of the universe is the conversion of gas into stars. We know a lot about the modes of star formation in local galaxies all along the Hubble sequence (Kennicutt 1998). We are also getting a basic idea from deep surveys of the history of star formation in the universe (Madau, Pozzetti, & Dickinson 1998). However, it is also clear that there are dim and unrecognized repositories of baryons. At low redshift, the serendipitous discovery of Malin 1 - still that largest and most gas-rich galaxy known - is a reminder that star formation in disks can be slow and very inefficient (Impey & Bothun 1989). Figure 1 shows that the lowest surface brightness galaxies have properties quite distinct from normal stellar systems on the Hubble sequence. At high redshifts, galaxies can escape detection due to the severe effects of surface brightness dimming or due to dust obscuration. We still do not know the full range of star formation histories in the universe. The luminosity-weighted integral integ phi (L) L dL appears to converge not far below L*, but there are indications of a steepening fainter than MB = -16 (see the discussion in Impey & Bothun 1997). The most abundant stellar system in the universe is a gas-rich dwarf galaxy, examples of which have rarely been studied outside the Local Supercluster. The motivation to look for additional baryons is strong; Omegalum from the integral of the galaxy luminosity function is a factor of 2-3 below the lower bound on Omegabaryon from nucleosynthesis arguments (Copi, Schramm, & Turner 1995; Persic & Salucci 1992; Bristow & Phillipps 1994).

Figure
 1
Figure 1. Collapsed structures in the universe, assuming dissipation by intercloud collisions, after Efstathiou & Rees (1983).

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