2024A&A...681A..62M


Query : 2024A&A...681A..62M

2024A&A...681A..62M - Astronomy and Astrophysics, volume 681A62 (2024/1-1)

First upper limits on the 21 cm signal power spectrum from cosmic dawn from one night of observations with NenuFAR.

MUNSHI S., MERTENS F.G., KOOPMANS L.V.E., OFFRINGA A.R., SEMELIN B., AUBERT D., BARKANA R., BRACCO A., BRACKENHOFF S.A., CECCONI B., CECCOTTI E., CORBEL S., FIALKOV A., GEHLOT B.K., GHARA R., GIRARD J.N., GRIESSMEIER J.M., HOFER C., HOTHI I., MERIOT R., MEVIUS M., OCVIRK P., SHAW A.K., THEUREAU G., YATAWATTA S., ZARKA P. and ZAROUBI S.

Abstract (from CDS):

The redshifted 21 cm signal from neutral hydrogen is a direct probe of the physics of the early universe and has been an important science driver of many present and upcoming radio interferometers. In this study we use a single night of observations with the New Extension in Nançay Upgrading LOFAR (NenuFAR) to place upper limits on the 21 cm power spectrum from cosmic dawn at a redshift of z = 20.3. NenuFAR is a new low-frequency radio interferometer, operating in the 10-85 MHz frequency range, currently under construction at the Nançay Radio Observatory in France. It is a phased array instrument with a very dense uv coverage at short baselines, making it one of the most sensitive instruments for 21 cm cosmology analyses at these frequencies. Our analysis adopts the foreground subtraction approach, in which sky sources are modeled and subtracted through calibration and residual foregrounds are subsequently removed using Gaussian process regression. The final power spectra are constructed from the gridded residual data cubes in the uv plane. Signal injection tests are performed at each step of the analysis pipeline, the relevant pipeline settings are optimized to ensure minimal signal loss, and any signal suppression is accounted for through a bias correction on our final upper limits. We obtain a best 2σ upper limit of 2.4 × 107 mK2 at z = 20.3 and k = 0.041 h cMpc–1. We see a strong excess power in the data, making our upper limits two orders of magnitude higher than the thermal noise limit. We investigate the origin and nature of this excess power and discuss further improvements to the analysis pipeline that can potentially mitigate it and consequently allow us to reach thermal noise sensitivity when multiple nights of observations are processed in the future.

Abstract Copyright: © The Authors 2024

Journal keyword(s): methods: data analysis - techniques: interferometric - dark ages - reionization - first stars

Errata: erratum vol. 687, art. C1 (2024)

Simbad objects: 12

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Number of rows : 12
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME NCP reg 00 00 00 +90 00.0           ~ 216 0
2 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
3 NGC 1275 Bla 03 19 48.1599902040 +41 30 42.108850836   13.10 12.48 11.09   ~ 4243 3
4 3C 111 Sy1 04 18 21.2772425736 +38 01 35.801359968   19.75 18.05     ~ 1002 2
5 NAME Per B SyG 04 37 04.37535450 +29 40 13.8179631   21.7       ~ 533 2
6 3C 134 rG 05 04 42.190 +38 06 11.40   20       ~ 90 1
7 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
8 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7815 3
9 MCG+07-41-003 Bla 19 59 28.35656837 +40 44 02.0972325   16.22 15.10     ~ 2537 2
10 2C 1820 SyG 21 55 52.324 +38 00 28.51   19.20       ~ 234 1
11 3C 452 Sy2 22 45 48.7616172744 +39 41 15.906782184   17.60 16.56     ~ 391 1
12 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1

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