Towards 21-cm intensity mapping at z = 2.28 with uGMRT using the tapered gridded estimator - II. Cross-polarization power spectrum

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dc.contributor.author Elahi, Kh.Md. Asif
dc.contributor.author Bharadwaj, Somnath
dc.contributor.author Ghosh, Abhik
dc.contributor.author Pal, Srijita
dc.contributor.author Ali, Sk. Saiyad
dc.contributor.author Choudhuri, Samir
dc.contributor.author Chakraborty, Arnab
dc.contributor.author Datta, Abhirup
dc.contributor.author Roy, Nirupam
dc.contributor.author Choudhury, Madhurima
dc.contributor.author Dutta, Prasun
dc.date.accessioned 2024-03-26T07:33:38Z
dc.date.available 2024-03-26T07:33:38Z
dc.date.issued 2023-04-01
dc.identifier.issn 00358711
dc.identifier.uri http://localhost:8080/xmlui/handle/123456789/3017
dc.description This paper published with affiliation IIT (BHU), Varanasi in open access mode. en_US
dc.description.abstract Neutral hydrogen (H I) 21-cm intensity mapping (IM) offers an efficient technique for mapping the large-scale structures in the Universe. We introduce the 'Cross' Tapered Gridded Estimator (Cross TGE), which cross-correlates two cross-polarizations (RR and LL) to estimate the multifrequency angular power spectrum Cι(Δν). We expect this to mitigate several effects like noise bias, calibration errors, etc., which affect the 'Total' TGE that combines the two polarizations. Here, we apply the Cross TGE on 24.4-MHz-bandwidth uGMRT (upgraded Giant Metrewave Radio Telescope) Band 3 data centred at 432.8 MHz aiming H I IM at z = 2.28. The measured Cι(Δν) is modelled to yield maximum likelihood estimates of the foregrounds and the spherical power spectrum P(k) in several k bins. Considering the mean squared brightness temperature fluctuations, we report a 2σ upper limit Δ2UL(k) ≤ (58.67)2 mK2 at k = 0.804 Mpc−1, which is a factor of 5.2 improvement on our previous estimate based on the Total TGE. Assuming that the H I traces the underlying matter distribution, we have modelled Cι(Δν) to simultaneously estimate the foregrounds and [ΩH IbH I], where ΩH I and bH I are the H I density and linear bias parameters, respectively. We obtain a best-fitting value of [ΩH IbH I]2 = 7.51 × 10−4 ± 1.47 × 10−3 that is consistent with noise. Although the 2σ upper limit [ΩH IbH I]UL ≤ 0.061 is ∼50 times larger than the expected value, this is a considerable improvement over earlier works at this redshift. en_US
dc.description.sponsorship Centre for Development of Advanced Computing GMRT Department of Science and Technology, Ministry of Science and Technology, India Science and Engineering Research Board National Centre for Radio Astrophysics of the Tata Institute of Fundamental Research - SERB/F/9805/2019-2020 en_US
dc.language.iso en en_US
dc.publisher Oxford University Press en_US
dc.relation.ispartofseries Monthly Notices of the Royal Astronomical Society;520
dc.subject diffuse radiation; en_US
dc.subject large-scale structure of Universe; en_US
dc.subject methods: data analysis; en_US
dc.subject methods: statistical; en_US
dc.subject techniques: interferometric en_US
dc.title Towards 21-cm intensity mapping at z = 2.28 with uGMRT using the tapered gridded estimator - II. Cross-polarization power spectrum en_US
dc.type Article en_US


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