Linearized f(R) Gravity: Gravitational Radiation & Solar System Tests

TL;DR

This paper analyzes the linearized form of f(R)-gravity, revealing modifications in gravitational radiation, deriving weak-field metrics, and comparing experimental bounds to constrain the theory's parameters.

Contribution

It provides a detailed analysis of linearized f(R)-gravity, deriving new metrics, examining gravitational wave signatures, and establishing bounds from solar system and laboratory tests.

Findings

Gravitational radiation admits an extra Ricci scalar mode.

Solar system tests constrain |a_2| to less than 1.2 x 10^18 m^2.

Laboratory experiments impose a stricter bound of |a_2| < 2 x 10^-9 m^2.

Abstract

We investigate the linearized form of metric f(R)-gravity, assuming that f(R) is analytic about R = 0 so it may be expanded as f(R) = R + a_2 R^2/2 + ... . Gravitational radiation is modified, admitting an extra mode of oscillation, that of the Ricci scalar. We derive an effective energy-momentum tensor for the radiation. We also present weak-field metrics for simple sources. These are distinct from the equivalent Kerr (or Schwarzschild) forms. We apply the metrics to tests that could constrain f(R). We show that light deflection experiments cannot distinguish f(R)-gravity from general relativity as both have an effective post-Newtonian parameter \gamma = 1. We find that planetary precession rates are enhanced relative to general relativity; from the orbit of Mercury we derive the bound |a_2| < 1.2 \times 10^18 m^2. Gravitational wave astronomy may be more useful: considering the phase of a gravitational waveform we estimate deviations from general relativity could be measurable for an extreme-mass-ratio inspiral about a 10^6 M_sol black hole if |a_2| > 10^17 m^2, assuming that the weak-field metric of the black hole coincides with that of a point mass. However Eot-Wash experiments provide the strictest bound |a_2| < 2 \times 10^-9 m^2. Although the astronomical bounds are weaker, they are still of interest in the case that the effective form of f(R) is modified in different regions, perhaps through the chameleon mechanism. Assuming the laboratory bound is universal, we conclude that the propagating Ricci scalar mode cannot be excited by astrophysical sources.