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http://hdl.handle.net/2289/2223
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DC Field | Value | Language |
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dc.contributor.author | Sethi, S.K. | - |
dc.date.accessioned | 2007-04-03T09:51:19Z | - |
dc.date.available | 2007-04-03T09:51:19Z | - |
dc.date.issued | 2005-11 | - |
dc.identifier.citation | Monthly Notices of the Royal Astronomical Society, 2005, Vol.363, Issue 3, p818-830. | en |
dc.identifier.issn | 0035-8711 | - |
dc.identifier.uri | http://hdl.handle.net/2289/2223 | - |
dc.description | Restricted Access. An open access version is available at arXiv.org.(one of the alternative locations) | en |
dc.description.abstract | We investigate the all-sky signal in redshifted atomic hydrogen (HI) line from the re-ionization epoch. We model the phase of re-ionization as multiple point sources that carve out spherical Stromgren spheres. We study ionization histories compatible with Wilkinson Microwave Anisotropy Probe (WMAP) observation. The Lyman α and soft X-ray emission from these sources are taken into account for studying the HI signal. HI can be observed in both emission and absorption depending on the ratio of Lyman α to ionizing flux and the spectrum of the radiation in soft X-ray. We also compute the signal from pre-reionization epoch and show that within the uncertainty in cosmological parameters, it is fairly robust. The main features of HI signal can be summarized as follows. (i) The pre-ionized HI can be seen in absorption for ν~= 10-40 MHz; the maximum signal strength is ~=70-100 mK. (ii) A sharp absorption feature of width <~5 MHz might be observed in the frequency range ~=50-100 MHz, depending on the re-ionization history. The strength of the signal is proportional to the ratio of the Lyman α and the hydrogen-ionizing flux and the spectral index of the radiation field in soft X-ray. (iii) At larger frequencies, HI is seen in emission with peak frequency between 60 and 100MHz, depending on the ionization history of the Universe; the peak strength of this signal is ~=50 mK. From Fisher matrix analysis, we compute the precision with which the parameters of the model can be estimated from a future experiment as follows: (i) the pre-reionization signal can constrain a region in the Ωbh2-Ωmh2 plane (ii) HI observed in emission can be used to give precise, <~1 per cent, measurement of the evolution of the ionization fraction in the Universe and (iii) the transition region from absorption to emission can be used as a probe of the spectrum of ionizing sources; in particular, the HI signal in this regime can give a reasonably precise measurement of the fraction of the Universe heated by soft X-ray photons. | en |
dc.format.extent | 8338 bytes | - |
dc.format.mimetype | application/pdf | - |
dc.language.iso | en | en |
dc.publisher | Blackwell Publishing for the Royal Astronomical Society | en |
dc.relation.uri | http://arxiv.org/abs/astro-ph/0508172 | en |
dc.relation.uri | http://adsabs.harvard.edu/cgi-bin/bib_query?bibcode=2005MNRAS.363..818S | en |
dc.relation.uri | http://dx.doi.org/10.1111/j.1365-2966.2005.09485.x | en |
dc.rights | (2005) Blackwell Publishing for the Royal Astronomical Society | en |
dc.subject | cosmic microwave background | en |
dc.subject | cosmology: theory | en |
dc.subject | early Universe | en |
dc.title | HI signal from re-ionization epoch | en |
dc.type | Article | en |
Appears in Collections: | Research Papers (A&A) |
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2005 MNRAS_V363_p818.pdf Restricted Access | Restricted Access | 426 kB | Adobe PDF | View/Open Request a copy |
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