Renormalization group in Lifshitz-type theories

TL;DR

This paper investigates the renormalization group flow of Lorentz-violating couplings in Lifshitz-type scalar theories, showing that Lorentz symmetry is generally not emergent at low energies without fine-tuning.

Contribution

It provides a detailed analysis of how Lorentz-violating parameters evolve under RG flow in Lifshitz theories, highlighting the difficulty of recovering Lorentz symmetry naturally.

Findings

Lorentz-violating couplings run logarithmically with energy scale.

Lorentz symmetry is not naturally recovered at low energies without fine-tuning.

The results apply broadly to Lifshitz-type theories, including quantum gravity models.

Abstract

We study the one-loop renormalization and evolution of the couplings in scalar field theories of the Lifshitz type, i.e. with different scaling in space and time. These theories are unitary and renormalizable, thanks to higher spatial derivative terms that modify the particle propagator at high energies, but at the expense of explicitly breaking Lorentz symmetry. We study if and under what conditions the Lorentz symmetry can be considered as emergent at low energies by studying the RG evolution of the ``speed of light'' coupling $c^2_\phi$ and, for more than one field, of $\delta c^2\equiv c^2_{\phi_1}-c^2_{\phi_2}$ in simple models. We find that in the UV both $c^2_\phi$ and $\delta c^2$ generally flow logarithmically with the energy scale. A logarithmic running of $c^2$ persists also at low-energies, if $\delta c^2 \neq 0$ in the UV. As a result, Lorentz symmetry is not recovered at low energies with the accuracy needed to withstand basic experimental constraints, unless all the Lorentz breaking terms, including $\delta c^2$, are unnaturally fine-tuned to extremely small values in the UV. We expect that the considerations of this paper will apply to any generic theory of Lifshitz type, including a recently proposed quantum theory of gravity by Horava.