Reionization and Cosmological Parameters
Eiichiro Komatsu (Univ. of Texas at Austin) CMBPol Workshop, June 24, 2008
Reionization and Cosmological Parameters Eiichiro Komatsu (Univ. of - - PowerPoint PPT Presentation
Reionization and Cosmological Parameters Eiichiro Komatsu (Univ. of Texas at Austin) CMBPol Workshop, June 24, 2008 5-Year E-Mode Polarization Power Spectrum at Low l E-Mode Angular Power Spectrum 5-sigma detection of the E- mode polarization
Eiichiro Komatsu (Univ. of Texas at Austin) CMBPol Workshop, June 24, 2008
Nolta et al. Black Symbols are upper limits 5-sigma detection of the E- mode polarization over l=2-6. (Errors include cosmic variance)
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E-Mode Angular Power Spectrum
Hinshaw et al. Errors include cosmic variance Black Symbols are upper limits
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E-Mode Angular Power Spectrum
the E-mode power spectrum:
(Page et al.; QV only)
measuring?
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Hinshaw et al.
reionization with τ=0.090
dominated at l<6
dominated at l<10, if noise is white
the noise further WMAP5 (KaQV) WMAP9 (KaQVW) Planck (81uK’)
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Dunkley et al.
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Instantaneous (τ=0.090) τ=0.107
WMAP
reionization (i.e., non-monotonic reionization)
τ=0.131 Instantaneous (τ=0.090)
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τ=0.114
WMAP
hidden in the WMAP data.
instantaneous reionization.
relaxed for double reionization models (i.e., non- monotonic reionization)
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Komatsu et al.
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zreion MUCH better than Planck.
WMAP5
(fsky=0.8; lmax=30)
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by-l) only up to l~10, assuming white noise.
further
limited (l-by-l) up to l~6
the limits on reionization histories? Yes, significantly!
find ALL of τ out there.
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measurement for the other cosmological parameters may be a lot less than those for WMAP.
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