Aberrating the CMB sky: fast and accurate computation of the aberration kernel

TL;DR

This paper introduces a fast, accurate method for computing the aberration kernel in the CMB sky, enabling precise analysis of motion-induced anisotropies and potential velocity measurements without relying solely on the dipole.

Contribution

It derives simple recursion relations for the aberration kernel, improving computational accuracy and efficiency for high multipoles, applicable at higher velocities beyond beta~10^{-3}.

Findings

Recursion relations enable precise aberration kernel computation.

First order beta terms suffice for statistical detection of aberration.

Method is robust across different velocities and multipole ranges.

Abstract

It is well known that our motion with respect to the cosmic microwave background (CMB) rest frame introduces a large dipolar CMB anisotropy, with an amplitude ~beta=v/c~10^{-3}. In addition it should lead to a small breaking of statistical isotropy which becomes most notable at higher multipoles. In principle this could be used to determine our velocity with respect to the CMB rest frame using high angular resolution data from Planck, without directly relying on the amplitude and direction of the CMB dipole, allowing us to constrain cosmological models in which the cosmic dipole arises partly from large-scale isocurvature perturbations instead of being fully motion-induced. Here we derive simple recursion relations that allow precise computation of the motion-induced coupling between different spherical harmonic coefficients. Although the lowest order approximations for the coupling kernel can be deficient by factors of 2-5 at multipoles l~1000-3000, using our results for the aberration kernel we explicitly confirm that for a statistical detection of the aberration effect only first order terms in beta matter. However, the expressions given here are not restricted to beta~10^{-3}, but can be used at much higher velocities. We demonstrate the robustness of these formulae, illustrating the dependence of the kernel on beta, as well as the spherical harmonic indices l and m.