Abstract
Neutral diffuse intergalactic gas that existed during the Epoch of Reionization (EoR) suppresses Lyα flux emitted by background galaxies. In this chapter I summarise the increasing observational support for the claim that Lyα photons emitted by galaxies at z > 6 are suppressed by intervening HI gas. I describe key physical processes that affect Lyα transfer during the EoR. I argue that in spite of the uncertainties associated with this complex multiscale problem, the data on Lyα emitting galaxies at \( z=0\!\!-\!\!6 \) strongly suggests that the observed reduction in Lyα flux from galaxies at z > 6 is due to additional intervening HI gas. The main question is what fraction of this additional HI gas is in the diffuse neutral IGM. I summarise how future surveys on existing and incoming instruments are expected to reduce existing observational uncertainties enormously. With these improved data we will likely be able to nail down reionization with Lyα emitting galaxies.
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Notes
- 1.
The ‘effective’ optical depth in the Lyα forest exceeds unity, τ eff > 1 at \( z\stackrel{>}{\sim }4 \) (see e.g. Fig. 3 of [21]).
- 2.
- 3.
This reduced sensitivity to CGM/IGM opacity is important as we expect its opacity to Lyα photons to increase with redshift, while observations indicate it is increasingly easy to detect Lyα flux from galaxies towards higher redshifts from z = 0 to z = 6.
- 4.
The quantity x HI will refer to the volume averaged neutral fraction of hydrogen throughout this chapter.
- 5.
During the final stages of preparation, a preprint by Choudhury et al. [10] appeared which constrained \( x_{\mathrm{HI}} \sim 0.3 \) at \( z \sim 7 \) for a model that is similar to that of Mesinger et al. [53]. Choudhury et al. [10] adopt a steeper EW-PDF P 6(EW), which makes all Lyα emitting galaxies fainter by a factor of \( \sim 0.8 \), and could explain their somewhat smaller required x HI. This further illustrates how current observational uncertainties on Lyα EW-PDFs at \( z \sim 6 \) and \( z \sim 7 \) limit our ability to constrain x HI.
- 6.
- 7.
- 8.
- 9.
- 10.
Lidz et al. [45] note that LAE-21 cm cross-correlation is actually sensitive to the characteristic HII regions size around LAEs which are detectable, which especially during the early stages of reionization is larger than the true characteristic HII bubble size. While the LAE-21 cm cross-correlation is likely easier detect, it may be more difficult to infer characteristic HII bubble size from this correlation than from the galaxy-21 cm correlation.
- 11.
- 12.
There exists significant variation in observed line profiles even at a fixed redshift and observed flux, and so we do not expect spectra of in individual galaxies to be able to distinguish between different mechanisms.
- 13.
In the most extreme case in which outflows shift all photons significantly (i.e. \( \stackrel{>}{\sim }200 \) km s−1) to the red side of the systemic velocity of the galaxy, we would expect very little scattering in the CGM.
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I would like to thank Andrei Mesinger for permission to reproduce figures from his work.
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Dijkstra, M. (2016). Constraining Reionization with Lyα Emitting Galaxies. In: Mesinger, A. (eds) Understanding the Epoch of Cosmic Reionization. Astrophysics and Space Science Library, vol 423. Springer, Cham. https://doi.org/10.1007/978-3-319-21957-8_5
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