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First‐Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Determination of Cosmological Parameters

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

Spergel et al. 2003 The Astrophysical Journal Supplement Series 148 175.

  • Provider: AAS Journals

Caption: Fig. 6.

Left: Comparison of the best‐fit ΛCDM model of § 3 based on WMAP data only to the 2dFGRS power spectrum (Percival et al. 2001). The bias parameter for the best‐fit power‐law ΛCDM model is 1.0, corresponding to a best‐fit value of ﹩\beta =0.45﹩. Right: Comparison of the best‐fit power‐law ΛCDM model of § 3 to the power spectrum at ﹩z=3﹩ inferred from the Lyα forest data. The data points have been scaled downward by 20%, which is consistent with the 1 σ calibration uncertainty (Croft et al. 2002).

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