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http://hdl.handle.net/2289/8714Full metadata record
| DC Field | Value | Language |
|---|---|---|
| dc.contributor.author | Sarkar, Shouvik | - |
| dc.contributor.author | Elahi, Khandakar Md Asif | - |
| dc.contributor.author | Choudhuri, Samir | - |
| dc.contributor.author | Bharadwaj, Somnath | - |
| dc.contributor.author | Chatterjee, Suman | - |
| dc.contributor.author | Bhattacharya, Baijayanta | - |
| dc.contributor.author | Sethi, Shiv | - |
| dc.contributor.author | Patwa, Akash Kumar | - |
| dc.date.accessioned | 2026-05-25T06:04:03Z | - |
| dc.date.available | 2026-05-25T06:04:03Z | - |
| dc.date.issued | 2026-06 | - |
| dc.identifier.citation | Monthly Notices of the Royal Astronomical Society, 2026, Vol. 549 (4), AR No. 1 | en_US |
| dc.identifier.issn | 1365-2966 | - |
| dc.identifier.uri | http://hdl.handle.net/2289/8714 | - |
| dc.description | Open Access. Also available at arXiv.org (one of the alternative locations) | en_US |
| dc.description.abstract | We analyse zenith-pointing (δ = −26. 7◦) Murchison Widefield Array (MWA) νc = 154.2MHz drift scan observations covering 349.0◦ ≤ α ≤ 70. 0◦ with 163 pointing centres (PCs) spaced by 0. 5◦. We measure Dℓ, the mean-squared angular brightness temperature fluctuations, as a function of α. A broad peak at α ≈ 50. 0◦ corresponds to the bright extended source Fornax A in the main lobe of the primary beam. A smaller peak at α ≈ 5.0◦ possibly corresponds to Fornax A in the first sidelobe. For α ≤ 22. 0◦ and ℓ ≥ 200, we find Dℓ ∝ ℓ2, which we interpret as Poisson fluctuations from point sources. We present 2 (k), the mean-squared 21-cm brightness temperature fluctuations from the Epoch of Reionization, as a function of α. Fornax A causes strong contamination near α ≈ 50. 5◦, elsewhere several PCs are consistent with noise. The range 358. 5◦ ≤ α ≤ 11. 5◦ is relatively foreground-free and best suited for EoR science. The PC at α = 11. 0◦2 yields the best 2 σ upper limit 2 UL (k) = (173. 13)2 mK2 at k = 0. 161Mpc−1. We incoherently combine 23 PCs to obtain UL (k) = (98. 67)2 mK 2 at k = 0. 156Mpc −1. This is the tightest upper limit from the MWA, being ≈ 3 times lower than earlier MWA limits, but ≈ 2 and ≈ 21 times higher than the LOFAR and HERA limits, respectively, and ≈ 3 orders of magnitude above theoretical predictions. | en_US |
| dc.language.iso | en | en_US |
| dc.publisher | Oxford University Press on behalf of Royal Astronomical Society. | en_US |
| dc.relation.uri | https://arxiv.org/abs/2604.24144 | en_US |
| dc.relation.uri | https://doi.org/10.1093/mnras/stag801 | en_US |
| dc.rights | ©TheAuthor(s) 2026 | en_US |
| dc.subject | methods: data analysis | en_US |
| dc.subject | methods: statistical | en_US |
| dc.subject | techniques: interferometric | en_US |
| dc.subject | cosmology: dark ages, reioniza- tion, first stars | en_US |
| dc.subject | diffuse radiation | en_US |
| dc.subject | large-scale structure of Universe | en_US |
| dc.title | The Tracking Tapered Gridded Estimator for the 21-cm power spectrum from the Murchison Widefield Array (MWA) drift scan observations - III. Improved upper limits at z=8.2 from multiple pointings | en_US |
| dc.type | Article | en_US |
| Appears in Collections: | Research Papers (A&A) | |
Files in This Item:
| File | Description | Size | Format | |
|---|---|---|---|---|
| 2026_MNRASVol.549_p1–21.pdf Restricted Access | Open Access | 2.86 MB | Adobe PDF | View/Open Request a copy |
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