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We study the effective field theory (EFT) of large-scale structure for cosmic density and momentum fields. We show that the finite part of the two-loop calculation and its counterterms introduces an apparent scale dependence for the leading-order parameter cₒ^2 of the EFT starting at k=0. 1 hMpc^-1. These terms limit the range over which one can trust the one-loop EFT calculation at the 1% level to k<0. 1 hMpc^-1 at redshift z=0. We construct a well-motivated one-parameter ansatz to fix the relative size of the one- and two-loop counterterms using their high-k sensitivity. Although this one-parameter model is a very restrictive choice for the counterterms, it explains the apparent scale dependence of cₒ^2 seen in simulations. It is also able to capture the scale dependence of the density power spectrum up to k0. 3 hMpc^-1 at the 1% level at redshift z=0. Considering a simple scheme for the resummation of large-scale motions, we find that the two-loop calculation reduces the need for this IR resummation at k<0. 2 hMpc^-1. Finally, we extend our calculation to momentum statistics and show that the same one-parameter model can also describe density-momentum and momentum-momentum statistics.
Baldauf et al. (Wed,) studied this question.
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