Towards 21-cm intensity mapping at z = 2.28 with uGMRT using the tapered gridded estimator – IV. Wide-band analysis

Author:

Elahi Khandakar Md Asif1ORCID,Bharadwaj Somnath1,Pal Srijita2,Ghosh Abhik3ORCID,Ali Sk Saiyad4,Choudhuri Samir5,Chakraborty Arnab6,Datta Abhirup7,Roy Nirupam2,Choudhury Madhurima8ORCID,Dutta Prasun9

Affiliation:

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

2. Department of Physics, Indian Institute of Science , Bangalore 560012 , India

3. Department of Physics, Banwarilal Bhalotia College , Asansol, West Bengal-713303 , India

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

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

6. Department of Physics and McGill Space Institute, McGill University , Montreal, QC H31 2T8 , Canada

7. Discipline of Astronomy, Astrophysics and Space Engineering, Indian Institute of Technology Indore , Indore 453552 , India

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

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

Abstract

ABSTRACT We present a Wide-band tapered gridded estimator (TGE), which incorporates baseline migration and variation of the primary beam pattern for neutral hydrogen ($H\, {\small I}$) 21-cm intensity mapping (IM) with large frequency bandwidth radio-interferometric observations. Here we have analysed $394-494 \, {\rm MHz}$ (z = 1.9–2.6) uGMRT data to estimate the Multifrequency Angular Power Spectrum (MAPS) Cℓ(Δν) from which we have removed the foregrounds using the polynomial fitting (PF) and Gaussian Process Regression (GPR) methods developed in our earlier work. Using the residual Cℓ(Δν) to estimate the mean-squared 21-cm brightness temperature fluctuation Δ2(k), we find that this is consistent with 0 ± 2σ in several k bins. The resulting 2σ upper limit $\Delta ^2(k) \lt (4.68)^2 \, \rm {mK^2}$ at $k=0.219\, \rm {Mpc^{-1}}$ is nearly 15 times tighter than earlier limits obtained from a smaller bandwidth ($24.4 \, {\rm MHz}$) of the same data. The 2σ upper limit $[\Omega _{H\, {\small I}} b_{H\, {\small I}}] \lt 1.01 \times 10^{-2}$ is within an order of magnitude of the value expected from independent estimates of the $H\, {\small I}$ mass density $\Omega _{H\, {\small I}}$ and the $H\, {\small I}$ bias $b_{H\, {\small I}}$. The techniques used here can be applied to other telescopes and frequencies, including $\sim 150 \, {\rm MHz}$ Epoch of Reionization observations.

Funder

SERB

Publisher

Oxford University Press (OUP)

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