Detailed modelling of the 21-cm Forest

TL;DR

This paper presents a high-resolution simulation of the 21-cm forest during the Epoch of Reionization, highlighting the importance of detailed physical processes and resolution for accurate predictions of absorption features.

Contribution

The study introduces a comprehensive simulation coupling dynamics, radiative transfer, and small-scale structure resolution to improve 21-cm forest modeling.

Findings

Soft X-ray and Lyman-alpha self-shielding affect optical depth predictions.

Peculiar velocities are critical for accurate absorption modeling.

LOFAR and SKA can detect and analyze 21-cm absorption features.

Abstract

The 21-cm forest is a promising probe of the Epoch of Reionization. The local state of the intergalactic medium (IGM) is encoded in the spectrum of a background source (radio-loud quasars or gamma ray burst afterglow) by absorption at the local 21-cm wavelength, resulting in a continuous and fluctuating absorption level. Small-scale structures (filaments and minihaloes) in the IGM are responsible for the strongest absorption features. The absorption can also be modulated on large scales by inhomogeneous heating and Wouthuysen-Field coupling. We present the results from a simulation that attempts to preserve the cosmological environment while resolving some of the small-scale structures (a few kpc resolution in a 50 Mpc/h box). The simulation couples the dynamics and the ionizing radiative transfer and includes X-ray and Lyman lines radiative transfer for a detailed physical modelling. As a result we find that soft X-ray self-shielding, Lyman-alpha self-shielding and shock heating all have an impact on the predicted values of the 21-cm optical depth of moderately overdense structures like filaments. An correct treatment of the peculiar velocities is also critical. Modelling these processes seems necessary for accurate predictions and can be done only at high enough resolution. As a result, based on our fiducial model, we estimate that LOFAR should be able to detect a few (strong) absorptions features in a frequency range of a few tens of MHz for a 20 mJy source located at z=10, while the SKA would extract a large fraction of the absorption information for the same source.