Cosmological perturbations and gravitational waves in the general Einstein-vector theory

TL;DR

This paper explores the stability and gravitational wave characteristics of a comprehensive Einstein-vector theory in cosmology, revealing unique superluminal vector GWs and constraints on degrees of freedom, with implications for observational tests.

Contribution

It provides a systematic stability analysis and characterizes gravitational wave modes in the Einstein-vector theory, highlighting novel superluminal vector GWs and their observational signatures.

Findings

Tensor perturbations are stable with standard propagation.

Vector GWs can propagate superluminally, offering a distinctive observational signature.

Scalar sector stability depends on background vector field and wavenumber.

Abstract

We investigate the stability and gravitational waves (GWs) in the four-dimensional general Einstein-vector theory in a cosmological background. The theory accommodates up to six propagating degrees of freedom, comprising two tensor, two vector, and two scalar modes, in addition to matter perturbations. In certain regions of the parameter space, the number of scalar degrees of freedom is reduced to one or even zero. To investigate the stability, we systematically analyze ghost, Laplacian, and tachyonic instabilities at the linear perturbative level. The stability conditions are easily satisfied for tensor perturbations, but impose nontrivial constraints on the parameter space for vector perturbations. Furthermore, in the presence of a nonvanishing background vector field, the scalar sector becomes unstable at small wavenumbers $|\vec{k}|$. In the small-scale limit ($|\vec{k}|\rightarrow\infty$), we further investigate the GW properties of the general Einstein-vector theory within the stable parameter space, including the number of independent modes, their propagation speeds, and observational constraints from GW experiments. We find that there are at most two tensor modes, two vector modes, and one scalar mode. Notably, vector GWs propagate superluminally, yet they are forbidden if tensor GWs travel exactly at light speed. This distinctive feature provides a key observational signature for testing the theory.