Current models of the observable consequences of cosmic reionization and their detectability
A number of large current experiments aim to detect the signatures of the Cosmic Reionization at redshifts z> 6. Their success depends crucially on understanding the character of the reionization process and its observable consequences and designing the best strategies to use. We use large-scale...
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ftciteseerx:oai:CiteSeerX.psu:10.1.1.338.1684 2023-05-15T18:22:48+02:00 Current models of the observable consequences of cosmic reionization and their detectability Ilian T. Iliev Garrelt Mellema Ue-li Pen J. Richard Bond Paul R. Shapiro The Pennsylvania State University CiteSeerX Archives 2008 application/pdf http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.338.1684 http://arxiv.org/pdf/astro-ph/0702099v2.pdf en eng http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.338.1684 http://arxiv.org/pdf/astro-ph/0702099v2.pdf Metadata may be used without restrictions as long as the oai identifier remains attached to it. http://arxiv.org/pdf/astro-ph/0702099v2.pdf Key words H II regions—high-redshift—galaxies formation—intergalactic medium— text 2008 ftciteseerx 2016-01-07T23:45:28Z A number of large current experiments aim to detect the signatures of the Cosmic Reionization at redshifts z> 6. Their success depends crucially on understanding the character of the reionization process and its observable consequences and designing the best strategies to use. We use large-scale simulations of cosmic reionization to evaluate the reionization signatures at redshifted 21-cm and small-scale CMB anisotropies in the best current model for the background universe, with fundamental cosmological parameters given by WMAP 3-year results (WMAP3). We find that the optimal frequency range for observing the “global step ” of the 21-cm emission is 120-150 MHz, while statistical studies should aim at 140-160 MHz, observable by GMRT. Some strongly-nongaussian brightness features should be detectable at frequencies up to ∼ 190 MHz. In terms of sensitivity-signal trade-off relatively low resolutions, corresponding to beams of at least a few arcminutes, are preferable. The CMB anisotropy signal from the kinetic Sunyaev-Zel’dovich effect from reionized patches peaks at tens of µK at arcminute scales and has an rms of ∼ 1µK, and should be observable by the Atacama Cosmology Telescope and the South Pole Telescope. We discuss the various observational issues and the uncertainties involved, mostly related to the poorly-known reionization parameters and, to a lesser extend, to the uncertainties in the background cosmology. Text South pole Unknown South Pole |
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Key words H II regions—high-redshift—galaxies formation—intergalactic medium— |
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Key words H II regions—high-redshift—galaxies formation—intergalactic medium— Ilian T. Iliev Garrelt Mellema Ue-li Pen J. Richard Bond Paul R. Shapiro Current models of the observable consequences of cosmic reionization and their detectability |
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Key words H II regions—high-redshift—galaxies formation—intergalactic medium— |
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A number of large current experiments aim to detect the signatures of the Cosmic Reionization at redshifts z> 6. Their success depends crucially on understanding the character of the reionization process and its observable consequences and designing the best strategies to use. We use large-scale simulations of cosmic reionization to evaluate the reionization signatures at redshifted 21-cm and small-scale CMB anisotropies in the best current model for the background universe, with fundamental cosmological parameters given by WMAP 3-year results (WMAP3). We find that the optimal frequency range for observing the “global step ” of the 21-cm emission is 120-150 MHz, while statistical studies should aim at 140-160 MHz, observable by GMRT. Some strongly-nongaussian brightness features should be detectable at frequencies up to ∼ 190 MHz. In terms of sensitivity-signal trade-off relatively low resolutions, corresponding to beams of at least a few arcminutes, are preferable. The CMB anisotropy signal from the kinetic Sunyaev-Zel’dovich effect from reionized patches peaks at tens of µK at arcminute scales and has an rms of ∼ 1µK, and should be observable by the Atacama Cosmology Telescope and the South Pole Telescope. We discuss the various observational issues and the uncertainties involved, mostly related to the poorly-known reionization parameters and, to a lesser extend, to the uncertainties in the background cosmology. |
author2 |
The Pennsylvania State University CiteSeerX Archives |
format |
Text |
author |
Ilian T. Iliev Garrelt Mellema Ue-li Pen J. Richard Bond Paul R. Shapiro |
author_facet |
Ilian T. Iliev Garrelt Mellema Ue-li Pen J. Richard Bond Paul R. Shapiro |
author_sort |
Ilian T. Iliev |
title |
Current models of the observable consequences of cosmic reionization and their detectability |
title_short |
Current models of the observable consequences of cosmic reionization and their detectability |
title_full |
Current models of the observable consequences of cosmic reionization and their detectability |
title_fullStr |
Current models of the observable consequences of cosmic reionization and their detectability |
title_full_unstemmed |
Current models of the observable consequences of cosmic reionization and their detectability |
title_sort |
current models of the observable consequences of cosmic reionization and their detectability |
publishDate |
2008 |
url |
http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.338.1684 http://arxiv.org/pdf/astro-ph/0702099v2.pdf |
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South Pole |
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South Pole |
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South pole |
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South pole |
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http://arxiv.org/pdf/astro-ph/0702099v2.pdf |
op_relation |
http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.338.1684 http://arxiv.org/pdf/astro-ph/0702099v2.pdf |
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Metadata may be used without restrictions as long as the oai identifier remains attached to it. |
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1766202223960784896 |