Constraints on μμ-distortion fluctuations and primordial non-Gaussianity from Planck data

preprint2015arXivOpen access

Abstract

We use the Planck HFI channel maps to make an all sky map of μμ-distortion fluctuations. Our μμ-type distortion map is dominated by the yy-type distortion contamination from the hot gas in the low redshift Universe and we can thus only place upper limits on the μμ-type distortion fluctuations. For the amplitude of μμ-type distortions on 10′10' scales we get the limit on root mean square (rms) value μrms10′<6.4×10−6μ_{rms}^{10'}< 6.4\times 10^{-6}, a limit 14 times stronger than the COBE-FIRAS (95%95\% confidence) limit on the mean of <μ><90×10−6< μ> <90\times 10^{-6}. Using our maps we also place strong upper limits on the auto angular power spectrum of μμ, CℓμμC_{\ell}^{μμ} and the cross angular power spectrum of μμ with the CMB temperature anisotropies, CℓμTC_{\ell}^{μT}. The strongest observational limits are on the largest scales, ℓ(ℓ+1)/(2π)Cℓμμ∣ℓ=2−26<(2.3±1.0)×10−12\ell(\ell+1)/(2π)C_{\ell}^{μμ}|_{\ell=2-26}<(2.3\pm 1.0)\times 10^{-12} and ℓ(ℓ+1)/(2π)CℓμT∣ℓ=2−26<(2.6±2.6)×10−12 K\ell(\ell+1)/(2π)C_{\ell}^{μT}|_{\ell=2-26}<(2.6\pm 2.6)\times 10^{-12}~{K}. Our observational limits can be used to constrain new physics which can create spatially varying energy release in the early Universe between redshifts 5×104≲z≲2×1065\times 10^4\lesssim z\lesssim 2\times 10^6. We specifically apply our observational results to constrain the primordial non-Gaussianity of the local type, when the source of μμ-distortion is Silk damping, for very squeezed configurations with the wavenumber for the short wavelength mode 46≲kS≲104 Mpc−146 \lesssim k_{S} \lesssim 10^4 ~{Mpc^{-1}} and for the long wavelength mode kL≈10−3 Mpc−1k_{L}\approx 10^{-3} ~{Mpc^{-1}}. Our limits on the primordial non-Gaussianity parameters are fNL<105,τNL<1.4×1011f_{NL}<10^5, τ_{NL}<1.4\times 10^{11} for kS/kL≈5×104−107k_{S}/k_{L}\approx 5\times 10^4- 10^7. We give a new derivation of the evolution of the μμ-distortion fluctuations. We also introduce mixing of Bose-Einstein spectra and yBEy^{BE}-type distortions.

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