A halo model for cosmological Lyman-limit systems
ABSTRACT We present an analytical model for cosmological Lyman-limit systems (lls) that successfully reproduces the observed evolution of the mean free path (λeff) of ionizing photons. The evolution of the co-moving mean free path is predominantly a consequence of the changing meta galactic photoion...
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Published in | Monthly notices of the Royal Astronomical Society Vol. 527; no. 1; pp. 689 - 705 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
London
Oxford University Press
01.01.2024
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Subjects | |
Online Access | Get full text |
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Summary: | ABSTRACT
We present an analytical model for cosmological Lyman-limit systems (lls) that successfully reproduces the observed evolution of the mean free path (λeff) of ionizing photons. The evolution of the co-moving mean free path is predominantly a consequence of the changing meta galactic photoionization rate and the increase with cosmic time of the minimum mass below which haloes lose their gas due to photoheating. In the model, Lyman-limit absorption is caused by highly ionized gas in the outskirt of dark matter haloes. We exploit the association with haloes to compute statistical properties of λeff and of the bias, b, of lls. The latter increases from b ∼ 1.5 → 2.6 from redshifts z = 2 → 6. Combined with the rapid increase with redshift of the bias of the haloes that host a quasar, the model predicts a rapid drop in the value of λeff when measured in quasar spectra from z = 5 → 6, whereas the actual value of λeff falls more smoothly. We derive an expression for the effective optical depth due to Lyman limit absorption as a function of wavelength and show that it depends sensitively on the poorly constrained number density of lls as a function of column density. The optical depth drops below unity for all wavelengths below a redshift of ∼2.5 which is therefore the epoch when the Universe first became transparent to ionizing photons. |
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ISSN: | 0035-8711 1365-2966 |
DOI: | 10.1093/mnras/stad3176 |