Testing the assumptions of the Effective Field Theory of Large-Scale Structure

TL;DR

This paper compares the bottom-up and top-down approaches of the Effective Field Theory of Large-Scale Structure, finding strong agreement in corrections but challenging some assumptions about coefficient growth.

Contribution

It introduces a top-down method to estimate EFT coefficients from N-body simulations and compares it to the traditional bottom-up approach, revealing new insights into coefficient behavior.

Findings

Top-down EFT coefficients match bottom-up results closely.

Leading EFT coefficient decreases after orbit crossing, contrary to previous assumptions.

Results are robust across different wavelength separations.

Abstract

The Effective Field Theory of Large-Scale Structure (EFTofLSS) attempts to amend some of the shortcomings of the traditional perturbative methods used in cosmology. It models the evolution of long-wavelength perturbations above a cutoff scale without the need for a detailed description of the short-wavelength ones. Short-scale physics is encoded in the coefficients of a series of operators composed of the long-wavelength fields, and ordered in a systematic expansion. As applied in the literature, the EFTofLSS corrects a summary statistic (such as the power spectrum) calculated from standard perturbation theory by matching it to $N$-body simulations or observations. This `bottom-up' construction is remarkably successful in extending the range of validity of perturbation theory. In this work, we compare this framework to a `top-down' approach, which estimates the EFT coefficients from the stress tensor of an $N$-body simulation, and propagates the corrections to the summary statistic. We consider simple initial conditions, viz. two sinusoidal, plane-parallel density perturbations with substantially different frequencies and amplitudes. We find that the leading EFT correction to the power spectrum in the top-down model is in excellent agreement with that inferred from the bottom-up approach which, by construction, provides an exact match to the numerical data. This result is robust to changes in the wavelength separation between the two linear perturbations. However, in our setup, the leading EFT coefficient does not always grow linearly with the cosmic expansion factor as assumed in the literature based on perturbative considerations. Instead, it decreases after orbit crossing takes place.