Direct Wavelet Expansion of the Primordial Power Spectrum

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© 2003. The American Astronomical Society. All rights reserved. Printed in U.S.A.
, , Citation Pia Mukherjee and Yun Wang 2003 ApJ 598 779 DOI 10.1086/379107

0004-637X/598/2/779

Abstract

In order to constrain and possibly detect unusual physics during inflation, we allow the power spectrum of primordial matter density fluctuations, Pin(k), to be an arbitrary function in the estimation of cosmological parameters from data. The multiresolution and good localization properties of orthogonal wavelets make them suitable for detecting features in Pin(k). We expand Pin(k) directly in wavelet basis functions. The likelihood of the data is thus a function of the wavelet coefficients of Pin(k), as well as the Hubble constant H0, baryon density Ωb h2, cold dark matter density Ωc h2, and the reionization optical depth τri in a flat ΛCDM cosmology. We derive constraints on these parameters from cosmic microwave background anisotropy data (WMAP, CBI, and ACBAR) and large-scale structure data (2dFGRS and PSCZ) using the Markov chain Monte Carlo (MCMC) technique. The direct wavelet expansion method is different from and complementary to the wavelet band power method of Mukherjee & Wang, and results from the two methods are consistent. In addition, as we demonstrate, the direct wavelet expansion method has the advantage that once the wavelet coefficients have been constrained, the reconstruction of Pin(k) can be effectively denoised, i.e., Pin(k) can be reconstructed using only the coefficients that, say, deviate from zero at greater than 1 σ. In doing so, we retain the essential properties of Pin(k). The reconstruction also suffers much less from the correlated errors of binning methods. The shape of the primordial power spectrum, as reconstructed in detail here, reveals an interesting new feature at 0.001 ≲ k/Mpc-1 ≲ 0.005. It will be interesting to see whether this feature is confirmed by future data. The reconstructed and denoised Pin(k) is favored over the scale-invariant and power-law forms at ≳1 σ.

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10.1086/379107