Reionization and Cosmological Parameters Eiichiro Komatsu (Univ. of - - PowerPoint PPT Presentation

reionization and cosmological parameters
SMART_READER_LITE
LIVE PREVIEW

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


slide-1
SLIDE 1

Reionization and Cosmological Parameters

Eiichiro Komatsu (Univ. of Texas at Austin) CMBPol Workshop, June 24, 2008

slide-2
SLIDE 2

5-Year E-Mode Polarization Power Spectrum at Low l

Nolta et al. Black Symbols are upper limits 5-sigma detection of the E- mode polarization over l=2-6. (Errors include cosmic variance)

2

E-Mode Angular Power Spectrum

slide-3
SLIDE 3

The signal is on the sky, baby...

Hinshaw et al. Errors include cosmic variance Black Symbols are upper limits

(Ka-QV)/2

3

E-Mode Angular Power Spectrum

slide-4
SLIDE 4

Measuring The Optical Depth of the Universe

  • Optical Depth measured from

the E-mode power spectrum:

  • Tau(5yr)=0.087 +/- 0.017
  • Tau(3yr)=0.089 +/- 0.030

(Page et al.; QV only)

  • 3-sigma improved to 5-sigma!
  • What is WMAP actually

measuring?

4

Hinshaw et al.

slide-5
SLIDE 5

Signal vs Noise Cl (unbinned)

  • Signal: instantaneous

reionization with τ=0.090

  • WMAP9: CV

dominated at l<6

  • Planck: CV

dominated at l<10, if noise is white

  • 1/f noise increases

the noise further WMAP5 (KaQV) WMAP9 (KaQVW) Planck (81uK’)

5

slide-6
SLIDE 6

Two-step Reionization

  • WMAP5 cannot constrain the EE power spectrum at l>7.
  • One has a freedom to choose reionization histories at z>~20.
  • You can hide τ at z>~20!

Dunkley et al.

6

Instantaneous (τ=0.090) τ=0.107

WMAP

slide-7
SLIDE 7

Double Reionization

  • Even more τ can be hidden in the WMAP 5-year data for double

reionization (i.e., non-monotonic reionization)

τ=0.131 Instantaneous (τ=0.090)

7

τ=0.114

WMAP

slide-8
SLIDE 8

ns - τ correlation

  • ns is closer to unity, if more τ is

hidden in the WMAP data.

  • Note that this plot assumes the

instantaneous reionization.

  • The constraint would be

relaxed for double reionization models (i.e., non- monotonic reionization)

8

Komatsu et al.

8

slide-9
SLIDE 9

Planck vs C.V. Limited

  • The cosmic variance limited experiment constrains both xe and

zreion MUCH better than Planck.

WMAP5

Planck C.V. Planck C.V.

(fsky=0.8; lmax=30)

9

slide-10
SLIDE 10

Conclusion

  • Planck’s EE measurement is cosmic variance limited (l-

by-l) only up to l~10, assuming white noise.

  • Contribution of 1/f noise degrades the sensitivity

further

  • Note that WMAP9’s EE would be cosmic variance

limited (l-by-l) up to l~6

  • Will the cosmic variance limited experiment improve

the limits on reionization histories? Yes, significantly!

  • Implications for the cosmological parameters?
  • Accurate determination of ns is possible only if we can

find ALL of τ out there.

10

slide-11
SLIDE 11

What I learned yesterday from Elena Pierpaoli

  • ns and τ are totally de-correlated for Planck and CMBPol
  • These experiments won’t need τ for measuring ns.
  • So, implications of Planck’s and CMBPol’s reionization

measurement for the other cosmological parameters may be a lot less than those for WMAP.

  • In fact, there may be no implication at all.
  • Good news!

11