Chameleon Screening in Cosmic Voids

TL;DR

This paper investigates how chameleon screening mechanisms influence cosmic voids using analytic and numerical methods, revealing the relationship between void properties and fifth force effects relevant for upcoming cosmological surveys.

Contribution

It introduces a combined analytic and finite element numerical approach to model chameleon screening in cosmic voids, providing new insights into the fifth force's dependence on void characteristics.

Findings

Fifth force ratios in voids range from 10^{-6} to 10^{-5} for realistic profiles.

Deeper voids with larger density gradients exhibit higher chameleon acceleration ratios.

Certain modified gravity models can produce significantly stronger fifth forces in voids.

Abstract

A key goal in cosmology in the upcoming decade will be to form a better understanding of the accelerated expansion of the Universe. Upcoming surveys, such as the Vera C. Rubin Observatory's 10-year Legacy Survey of Space and Time (LSST), Euclid and the Square Killometer Array (SKA) will deliver key datasets required to tackle this and other puzzles in contemporary cosmology. With this data, constraints of unprecedented power will be put on different models of dark energy and modified gravity. In this context it is crucial to understand how screening mechanisms, which hide the deviations of these theories from the predictions of general relativity in local experiments, affect structure formation. In this work we approach this problem by using a combination of analytic and numerical methods to describe chameleon screening in the context of cosmic voids. We apply a finite element method (FEM) code, SELCIE, to solve the chameleon equation of motion for a number of void profiles derived from observational data and simulations. The obtained results indicate a complex relationship between the properties of cosmic voids and the size of the chameleon acceleration of a test particle. We find that the fifth force on a test particle in a void is primarily related to the depth and the inner density gradient of the void. For realistic void profiles, the obtained chameleon-to-Newtonian acceleration ratios range between $a_{\phi}/a_{\rm Newt} \approx 10^{-6} - 10^{-5}$. However, it should be noted that in unusually deep voids with large inner density gradients, the acceleration ratios can be significantly higher. Similarly, other chameleon models, such as $f(R)$ Hu-Sawicki theory allow for significantly higher acceleration ratios. Given these results, we also discuss the optimal density profiles for detecting the fifth force in the upcoming observational surveys.