Abstract

The light-cone (LC) effect causes the mean as well as the statistical properties of the redshifted 21-cm signal Tb(n^,ν)T_{\rm b}(\hat{\bf n},ν) to change with frequency νν (or cosmic time). Consequently, the statistical homogeneity (ergodicity) of the signal along the line of sight (LoS) direction is broken. This is a severe problem particularly during the Epoch of Reionization (EoR) when the mean neutral hydrogen fraction (xˉHI\bar{x}_{\rm HI}) changes rapidly as the universe evolves. This will also pose complications for large bandwidth observations. These effects imply that the 3D power spectrum P(k)P(k) fails to quantify the entire second-order statistics of the signal as it assumes the signal to be ergodic and periodic along the LoS. As a proper alternative to P(k)P(k), we use the multi-frequency angular power spectrum (MAPS) Cℓ(ν1,ν2){\mathcal C}_{\ell}(ν_1,ν_2) which does not assume the signal to be ergodic and periodic along the LoS. Here, we study the prospects for measuring the EoR 21-cm MAPS using future observations with the upcoming SKA-Low. Ignoring any contribution from the foregrounds, we find that the EoR 21-cm MAPS can be measured at a confidence level ≥5σ\ge 5σ at angular scales ℓ∼1300\ell \sim 1300 for total observation time tobs≥128 hrst_{\rm obs} \ge 128\,{\rm hrs} across ∼44 MHz\sim 44\,{\rm MHz} observational bandwidth. We also quantitatively address the effects of foregrounds on MAPS detectability forecast by avoiding signal contained within the foreground wedge in (k⊥,k∥)(k_\perp, k_\parallel) plane. These results are very relevant for the upcoming large bandwidth EoR experiments as previous predictions were all restricted to individually analyzing the signal over small frequency (or equivalently redshift) intervals.

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