Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/3677
Title: Large H i optical depth and redshifted 21-cm signal from cosmic dawn
Authors: Majumdar, Suman
Keywords: Cooling;Cosmology;Distribution functions;Higher order statistics;Linearization;Optical properties;(cosmology) dark age, reionization, first star;(galaxy) intergalactic medium;Cooling mechanism;Cosmics;Galaxies intergalactic medium;Linearized equations;Optical depth;Reionization;Spin temperature;Theory;Galaxies
Issue Date: 2022
Publisher: Oxford University Press
Citation: Datta, K. K., Ghara, R., Hoque, A., & Majumdar, S. (2022). Large H i optical depth and redshifted 21-cm signal from cosmic dawn. Monthly Notices of the Royal Astronomical Society, 509(1), 945-953. doi:10.1093/mnras/stab3035
Abstract: The atomic neutral hydrogen (H i) 21-cm optical depth (b) can be considerably large as the kinetic and spin temperature of the intergalactic medium is expected to be very low during cosmic dawn. It will be particularly higher at regions with H i overdensity. We revisit the validity of the widely used linearized equation for estimating the H i 21-cm differential brightness temperature (Tb) which assumes b1 and approximates [1 - exp (- b)] as b. We consider two scenarios, one without any additional cooling mechanism or radio background (referred as standard scenario) and the other (referred as excess-cooling scenario) assumes the EDGES like absorption profile and an excess cooling mechanism. We find that given a measured global absorption signal, consistent with the standard (excess-cooling) scenario, the linearized equation overestimates the spin temperature by ${5}, (10,)$. Further, using numerical ulations, we study impact that the large optical depth has on various signal statistics. We observe that the variance, skewness, and kurtosis, calculated at ulation resolution (${0.5} ,h^{-1} , { Mpc}$), are overpredicted up to ${30}$, $30$, and $15,$, respectively, for the standard and up to $90$, $50$, and $50,$, respectively, for the excess-cooling scenario. Moreover, we find that the probability distribution function of Tb is squeezed and becomes more Gaussian in shape if no approximation is made. The spherically averaged H i power spectrum is overpredicted by up to $25$ and $80,$ at all scales for the standard and excess-cooling scenarios, respectively. © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society.
URI: https://doi.org/10.1093/mnras/stab3035
https://dspace.iiti.ac.in/handle/123456789/3677
ISSN: 0035-8711
Type of Material: Journal Article
Appears in Collections:Department of Astronomy, Astrophysics and Space Engineering

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