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The Birth of a Galaxy - III. Propelling reionisation with the faintest galaxies

, , , , , , and .
(2014)cite arxiv:1403.6123Comment: 21 pages, 15 figures, 4 tables. Submitted to MNRAS. Comments welcome.

Abstract

Starlight from galaxies plays a pivotal role throughout the process of cosmic reionisation. We present the statistics of dwarf galaxy properties at z > 7 in haloes with masses up to 10^9 solar masses, using a cosmological radiation hydrodynamics simulation that follows their buildup starting with their Population III progenitors. We find that metal-enriched star formation is not restricted to atomic cooling (T_vir > 10^4 K) haloes, but can occur in haloes down to masses ~10^6 solar masses, especially in neutral regions. Even though these smallest galaxies only host up to 10^4 solar masses of stars, they provide a significant fraction of the ionising photon budget because of their high number densities. We find that the galaxy luminosity function flattens above M_UV ~ -12 with a number density that is unchanged during reionisation. The fraction of ionising radiation escaping into the intergalactic medium is inversely dependent on halo mass, decreasing from 50 to 5 per cent in the mass range $M/M_= 7.0-8.5$. We find that low-mass galaxies are just as efficient at producing ionising photons per unit mass as atomic cooling haloes. However, they are gradually photo-suppressed as they are engulfed in ionised regions, giving way for larger galaxies to dominate the latter half of reionisation. Using our galaxy statistics in a semi-analytic reionisation model, we find a Thomson scattering optical depth consistent with the latest Planck results, while still being consistent with the UV emissivity constraints provided by Ly-alpha forest observations at z = 4-6. We find that haloes less massive than the atomic cooling limit provide nearly 30 per cent to the total ionising photon budget. Our work suggests that a yet-to-be observed population of low-mass galaxies was responsible for starting reionisation at very high redshifts.

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