Imprints of Chameleon f(R) Gravity on Galaxy Rotation Curves

TL;DR

This study investigates how chameleon $f(R)$ gravity influences galaxy rotation curves and radial acceleration relations, using simulations to identify observable features that can constrain modified gravity models.

Contribution

It provides the first detailed analysis of galaxy rotation curves in chameleon $f(R)$ gravity, linking simulation predictions to potential observational constraints.

Findings

Screened and unscreened regions have distinct rotation curve features.

Rotation curves for certain $f_{R0}$ values mimic $ ext{Lambda}$CDM, while others violate Solar System constraints.

Observable upturns in rotation curves can constrain $f(R)$ gravity models.

Abstract

Current constraints on gravity are relatively weak on galactic and intergalactic scales. Screened modified gravity models can exhibit complex behaviour there without violating stringent tests of gravity within our Solar System. They might hence provide viable extensions of the theory of gravity. Here, we use galaxy kinematics to constrain screened modified gravity models. We focus on chameleon $f(R)$ gravity and predict its impact on galaxy rotation curves and radial acceleration relations. This is achieved by post-processing state-of-the-art galaxy formation simulations from the \textsc{auriga project}, using the \textsc{mg-gadget} code. For a given galaxy, the surface dividing screened and un-screened regions adopts an oblate shape, reflecting the disc morphology of the galaxy's mass distribution. At the `screening radius'---the radius at which screening is triggered in the disc plane---characteristic `upturns' are present in both rotation curves and radial acceleration relations. The locations of these features depend on various factors, such as the galaxy mass, the concentration of the density profile and the value of the background field amplitude $f_{R0}$. Self-screening of stars and environmental screening also play a role. For Milky Way-size galaxies, we find that a model with $|f_{R0}|=10^{-7}$ results in rotation curves that are indistinguishable from $\Lambda$CDM, while for $|f_{R0}| \geq 2 \times 10^{-6}$ the simulated galaxies are entirely unscreened, violating Solar System constraints. For intermediate values, distinct upturns are present. With a careful statistical analysis of existing samples of observed rotation curves, including lower mass objects, constraints on $f(R)$ gravity with a sensitivity down to $|f_{R0}|\sim10^{-7}$ should be possible.