Spherically symmetric solutions in Covariant Horava-Lifshitz Gravity

TL;DR

This paper explores spherically symmetric vacuum solutions in Covariant Horava-Lifshitz Gravity, classifying solutions based on the radial shift function and analyzing their observational consistency.

Contribution

It provides a comprehensive analysis of spherically symmetric solutions considering all higher order curvature terms compatible with power-counting, and compares two assumptions about the auxiliary field A.

Findings

Solutions split into two classes based on the radial shift function.

IR limit solutions align with observations under specific assumptions.

The auxiliary field A's role varies between solution classes.

Abstract

We study the most general case of spherically symmetric vacuum solutions in the framework of the Covariant Horava Lifshitz Gravity, for an action that includes all possible higher order terms in curvature which are compatible with power-counting normalizability requirement. We find that solutions can be separated into two main classes: (i) solutions with nonzero radial shift function, and (ii) solutions with zero radial shift function. In the case (ii), spherically symmetric solutions are consistent with observations if we adopt the view of Horava and Melby-Tomson, according to which the auxiliary field A can be considered as a part of an effective general relativistic metric, which is valid only in the IR limit. On the other hand, in the case (i), consistency with observations implies that the field A should be independent of the spacetime geometry, as the Newtonian potential arises from the nonzero radial shift function. Also, our aim in this paper is to discuss and compare these two alternative but different assumptions for the auxiliary field A.