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The Tracking Tapered Gridded Estimator for the 21-cm power spectrum from MWA drift scan observations I: Validation and preliminary results

Published 16 May 2024 in astro-ph.CO and astro-ph.IM | (2405.10080v1)

Abstract: Drift scan observations provide the broad sky coverage and instrumental stability needed to measure the Epoch of Reionization (EoR) 21-cm signal. In such observations, the telescope's pointing center (PC) moves continuously on the sky. The Tracking Tapered Gridded Estimator (TTGE) combines observations from different PC to estimate P(k⊥,k∥)P(k_{\perp}, k_{\parallel}) the 21-cm power spectrum, centered on a tracking center (TC) which remains fixed on the sky. The tapering further restricts the sky response to a small angular region around TC, thereby mitigating wide-field foregrounds. Here we consider 154.2 MHz154.2 \, {\rm MHz} (z=8.2z = 8.2) Murchison Widefield Array (MWA) drift scan observations. The periodic pattern of flagged channels, present in MWA data, is known to introduce artefacts which pose a challenge for estimating P(k⊥,k∥)P(k_{\perp}, k_{\parallel}). We demonstrate that the TTGE is able to recover P(k⊥,k∥)P(k_{\perp}, k_{\parallel}) without any artefacts, and estimate P(k)P(k) within 5%5 \% accuracy over a large kk-range. We also present preliminary results for a single PC, combining 9 nights of observation (17 min(17 \, {\rm min} total). We find that P(k⊥,k∥)P(k_{\perp}, k_{\parallel}) exhibits streaks at a fixed interval of k∥=0.29 Mpc<sup>−1k_{\parallel}=0.29 \, {\rm Mpc}<sup>{-1}, which matches Δνper=1.28 MHz\Delta \nu_{\rm per}=1.28 \, {\rm MHz} that is the period of the flagged channels. The streaks are not as pronounced at larger k∥k_{\parallel}, and in some cases they do not appear to extend across the entire k⊥k_{\perp} range. The rectangular region 0.05≤k⊥≤0.16 Mpc<sup>−10.05 \leq k_{\perp} \leq 0.16 \, {\rm Mpc<sup>{-1}} and 0.9≤k∥≤4.6 Mpc<sup>−10.9 \leq k_{\parallel} \leq 4.6 \, {\rm Mpc<sup>{-1}} is found to be relatively free of foreground contamination and artefacts, and we have used this to place the 2σ2\sigma upper limit $\Delta<sup>2(k)</sup> &lt; (1.85 \times 10<sup>4)<sup>2\,</sup></sup> {\rm mK<sup>2}$ on the EoR 21-cm mean squared brightness temperature fluctuations at k=1 Mpc<sup>−1k=1 \,{\rm Mpc}<sup>{-1}.

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