Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/3677
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dc.contributor.authorMajumdar, Sumanen_US
dc.date.accessioned2022-03-17T01:00:00Z-
dc.date.accessioned2022-03-17T15:29:55Z-
dc.date.available2022-03-17T01:00:00Z-
dc.date.available2022-03-17T15:29:55Z-
dc.date.issued2022-
dc.identifier.citationDatta, 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/stab3035en_US
dc.identifier.issn0035-8711-
dc.identifier.otherEID(2-s2.0-85121252009)-
dc.identifier.urihttps://doi.org/10.1093/mnras/stab3035-
dc.identifier.urihttps://dspace.iiti.ac.in/handle/123456789/3677-
dc.description.abstractThe 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.en_US
dc.language.isoenen_US
dc.publisherOxford University Pressen_US
dc.sourceMonthly Notices of the Royal Astronomical Societyen_US
dc.subjectCoolingen_US
dc.subjectCosmologyen_US
dc.subjectDistribution functionsen_US
dc.subjectHigher order statisticsen_US
dc.subjectLinearizationen_US
dc.subjectOptical propertiesen_US
dc.subject(cosmology) dark age, reionization, first staren_US
dc.subject(galaxy) intergalactic mediumen_US
dc.subjectCooling mechanismen_US
dc.subjectCosmicsen_US
dc.subjectGalaxies intergalactic mediumen_US
dc.subjectLinearized equationsen_US
dc.subjectOptical depthen_US
dc.subjectReionizationen_US
dc.subjectSpin temperatureen_US
dc.subjectTheoryen_US
dc.subjectGalaxiesen_US
dc.titleLarge H i optical depth and redshifted 21-cm signal from cosmic dawnen_US
dc.typeJournal Articleen_US
dc.rights.licenseAll Open Access, Green-
Appears in Collections:Department of Astronomy, Astrophysics and Space Engineering

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