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Copyright by Athena Ranice Stacy 2011 - The University of Texas at ...

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leaving behind a neutron star or black hole. Thus, the masses <strong>of</strong> the first stars<br />

are the main determinant <strong>of</strong> their cosmological impact, though other factors<br />

such as the typical rot<strong>at</strong>ion r<strong>at</strong>e and the overall form<strong>at</strong>ion r<strong>at</strong>e also play a<br />

vital role.<br />

Improving our understanding <strong>of</strong> the form<strong>at</strong>ion <strong>of</strong> the first stars and<br />

their resulting initial mass function (IMF) is thus central to understanding this<br />

turning point in the universe and the environment in which the first galaxies<br />

formed. Such work is especially important now in order to prepare for up-<br />

coming observ<strong>at</strong>ions <strong>of</strong> instruments such as the James Webb Space Telescope<br />

(JW ST ), the Square Kilometer Array, and LISA, as well as the future ground-<br />

based Extremely Large Telescopes such as the E-ELT, GMT, and TMT (e.g.<br />

Greif et al. 2009; Johnson et al. 2009). In particular, JWST is expected to<br />

detect z 10 galaxies and give constraints on the IMF <strong>of</strong> their constituent<br />

stars (Pawlik et al. <strong>2011</strong>). It will also be exciting to m<strong>at</strong>ch predictions from<br />

upcoming numerical work with spectroscopic observ<strong>at</strong>ions <strong>of</strong> individual stars<br />

in near<strong>by</strong> ultra-faint dwarfs (‘dwarf archaeology’), as these stars may hold the<br />

SN abundance sign<strong>at</strong>ures <strong>of</strong> Pop III stars (Frebel and Bromm 2010).<br />

1.2 Rel<strong>at</strong>ion to Previous Work<br />

Much numerical work has already been carried out in <strong>at</strong>tempting to<br />

predict the typical mass <strong>of</strong> the first stars. <strong>The</strong> earliest simul<strong>at</strong>ions found<br />

th<strong>at</strong> Pop III stars were very massive (> ∼ 100 M⊙) due to a lack <strong>of</strong> metal and<br />

dust cooling, and th<strong>at</strong> these stars formed in isol<strong>at</strong>ion (e.g. Abel et al. 2002;<br />

Bromm et al. 2002). L<strong>at</strong>er simul<strong>at</strong>ions confirmed this (e.g. Yoshida et al.<br />

2006). However, while these cosmological simul<strong>at</strong>ions could study the initial<br />

collapse <strong>of</strong> primordial gas to very high densities, near the point when a Pop<br />

3

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