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Three‐Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Polarization Analysis

  • Authors: L. Page, G. Hinshaw, E. Komatsu, M. R. Nolta, D. N. Spergel, C. L. Bennett, C. Barnes, R. Bean, O. Doré, J. Dunkley, M. Halpern, R. S. Hill, N. Jarosik, A. Kogut, M. Limon, S. S. Meyer, N. Odegard, H. V. Peiris, G. S. Tucker, L. Verde, J. L. Weiland, E. Wollack, and E. L. Wright

Page et al. 2007 The Astrophysical Journal Supplement Series 170 335.

  • Provider: AAS Journals

Caption: Fig. 1.

Model of the ionization history of the universe. The line marked with an "x" is the ionization fraction, ﹩x=n_{e}/ n﹩, where ﹩n_{e}﹩ is the number of electrons and ﹩n=11.2\omega _{b}( 1+z) ^{3}\ \mathrm{m}\,^{-3}﹩ is the number of protons with ﹩\omega _{b}﹩ the baryon density. From quasar absorption systems we know the universe has been fully ionized since at least ﹩z\approx 6﹩. Between ﹩6\lesssim z\lesssim 30﹩ the first generation of stars ionized the universe. We show a possible model inspired by Holder et al. (2003). The history for this period is uncertain although the reionization produces a characteristic signature in the CMB polarization. For ﹩30< z< 2000﹩, we show decoupling as described in Peebles (1993). The line marked τ is the net optical depth, ﹩\tau ( z) ﹩. The dashed curves are the integrands in the numerator (bottom) and denominator (top) of eq. (1) (divided by 200) for the ﹩100< z< 2000﹩ region. By eye, one can see that the ratio of the integrals at the maximum, and thus the fractional polarization, is ﹩\approx 5﹩%. The vertical line marks the redshift of decoupling, ﹩z_{\mathrm{dec}\,}=1088﹩, at the maximum of the visibility function (not shown).

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