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

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small multiple system forms, domin<strong>at</strong>ed <strong>by</strong> a binary with masses ∼ 40 M⊙ and<br />

∼ 10 M⊙. If Pop III stars were to form typically in binaries or small multiples,<br />

this would have crucial consequences for the observ<strong>at</strong>ional sign<strong>at</strong>ure <strong>of</strong> the<br />

first stars, such as the nucleosynthetic p<strong>at</strong>tern <strong>of</strong> the SNe they produce, and<br />

the gravit<strong>at</strong>ional-wave emission from possible Pop III black-hole binaries.<br />

In Chapter 3, we examined the growth <strong>of</strong> metal-free, Pop III stars<br />

under radi<strong>at</strong>ive feedback. Using the sink particle method within a cosmological<br />

simul<strong>at</strong>ion, we modeled the effect <strong>of</strong> LW radi<strong>at</strong>ion emitted <strong>by</strong> the protostar,<br />

and employed a ray-tracing scheme to follow the growth <strong>of</strong> the surrounding<br />

H ii region. We again find th<strong>at</strong> a disk assembles around the first protostar,<br />

and th<strong>at</strong> radi<strong>at</strong>ive feedback will not prevent further fragment<strong>at</strong>ion <strong>of</strong> the disk<br />

to form multiple Pop III stars. <strong>The</strong> resuling he<strong>at</strong>ing and ioniz<strong>at</strong>ion <strong>of</strong> the<br />

gas leads to a shut<strong>of</strong>f <strong>of</strong> accretion once the main sink has grown to 15 M⊙<br />

while the second sink has grown to 5 M⊙. <strong>The</strong>re is little further accretion<br />

or fragment<strong>at</strong>ion afterwards, indic<strong>at</strong>ing the most likely outcome is a massive<br />

Pop III binary. If Pop III stars were typically unable to grow to more than<br />

a few tens <strong>of</strong> solar masses, this would have important consequences for the<br />

occurence <strong>of</strong> pair-instability supernovae in the early universe as well as the<br />

Pop III chemical sign<strong>at</strong>ure in the oldest stars observable today.<br />

In Chapter 4 we employed a cosmological simul<strong>at</strong>ion to estim<strong>at</strong>e the<br />

rot<strong>at</strong>ion speed <strong>of</strong> Pop III stars within a minihalo. Again using sink particles,<br />

we measured the velocities and angular momenta <strong>of</strong> all particles th<strong>at</strong> fall onto<br />

these protostellar regions. This allowed us to record the angular momentum <strong>of</strong><br />

the sinks and estim<strong>at</strong>e the rot<strong>at</strong>ional velocity <strong>of</strong> the Pop III stars expected to<br />

form within them. We find th<strong>at</strong> there is sufficient angular momentum to yield<br />

rapidly rot<strong>at</strong>ing stars (> ∼ 1000 km s −1 , or near break-up speeds). This indic<strong>at</strong>es<br />

178

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