Towards 21-cm intensity mapping at z = 2.28 with uGMRT using the tapered gridded estimator I: Foreground avoidance

Author:

Pal Srijita1,Elahi Kh Md Asif1ORCID,Bharadwaj Somnath1,Ali Sk Saiyad2,Choudhuri Samir34,Ghosh Abhik5ORCID,Chakraborty Arnab6,Datta Abhirup7,Roy Nirupam8,Choudhury Madhurima79ORCID,Dutta Prasun10

Affiliation:

1. Department of Physics and Centre for Theoretical Studies, IIT Kharagpur , Kharagpur 721 302, India

2. Department of Physics, Jadavpur University , Kolkata 700032, India

3. Astronomy Unit, Queen Mary University of London , Mile End Road, London E1 4NS, UK

4. Centre for Strings, Gravitation and Cosmology, Department of Physics, Indian Institute of Technology Madras , Chennai 600036, India

5. Department of Physics, Banwarilal Bhalotia College , Asansol, West Bengal 713 303, India

6. Department of Physics and McGill Space Institute, McGill University , Montreal, QC H3A 2T8, Canada

7. Discipline of Astronomy, Astrophysics and Space Engineering, Indian Institute of Technology Indore , Indore 453 552, India

8. Department of Physics, Indian Institute of Science , Bangalore 560 012, India

9. ARCO (Astrophysics Research Center), Department of Natural Sciences, The Open University of Israel , 1 University Road, PO Box 808, Ra’anana 4353701, Israel

10. Department of Physics, IIT (BHU) , Varanasi, 221005 India

Abstract

ABSTRACT The post-reionization (z ≤ 6) neutral hydrogen (H i) 21-cm intensity mapping signal holds the potential to probe the large-scale structures, study the expansion history, and constrain various cosmological parameters. Here, we apply the Tapered Gridded Estimator (TGE) to estimate P(k⊥, k∥) the power spectrum of the $z = 2.28\, (432.8\, {\rm MHz})$ redshifted 21-cm signal using a $24.4\, {\rm MHz}$ sub-band drawn from uGMRT Band 3 observations of European Large-Area ISO Survey-North 1 (ELAIS-N1). The TGE allows us to taper the sky response, which suppresses the foreground contribution from sources in the periphery of the telescope’s field of view. We apply the TGE on the measured visibility data to estimate the multifrequency angular power spectrum (MAPS) Cℓ(Δν) from which we determine P(k⊥, k∥) using maximum likelihood that naturally overcomes the issue of missing frequency channels (55 per cent here). The entire methodology is validated using simulations. For the data, using the foreground avoidance technique, we obtain a $2\, \sigma$ upper limit of $\Delta ^2(k) \le (133.97)^2 \, {\rm mK}^{2}$ for the 21-cm brightness temperature fluctuation at $k = 0.347 \, \textrm {Mpc}^{-1}$. This corresponds to $[\Omega _{\rm H\, {\small I}~}b_{\rm H\, {\small I}~}] \le 0.23$, where $\Omega _{\rm H\, {\small I}~}$ and $b_{\rm H\, {\small I}~}$, respectively, denote the cosmic H i mass density and the H i bias parameter. A previous work has analysed $8 \, {\rm MHz}$ of the same data at z = 2.19, and reported $\Delta ^{2}(k) \le (61.49)^{2} \, {\rm mK}^{2}$ and $[\Omega _{\rm H\, {\small I}~} b_{\rm H\, {\small I}~}] \le 0.11$ at $k=1 \, {\rm Mpc}^{-1}$. The upper limits presented here are still orders of magnitude larger than the expected signal corresponding to $\Omega _{\rm H\, {\small I}~} \sim 10^{-3}$ and $b_{\rm H\, {\small I}~} \sim 2$.

Funder

Tata Institute of Fundamental Research

SERB

Science and Engineering Research Board

Department of Science & Technology

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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