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Field Theory on Newton-Cartan Backgrounds and Symmetries of the Lifshitz Vacuum

Jelle Hartong, Elias Kiritsis, Niels A. Obers

TL;DR

The work advances a non-relativistic holographic program by coupling field theories to torsional Newton–Cartan boundaries and analyzing Lifshitz vacua, where the TNC vector $M_$ sources a particle-number current and can be promoted to a gauge field. It shows that bulk PBH diffeomorphisms induce a local Schrödinger algebra on $M$, enabling Schrödinger enhancements of Lifshitz symmetry in flat NC space-time and revealing how a nontrivial orbit of $M$ yields global Galilean and conformal-like symmetries. The authors develop Schrödinger-invariant probe actions on Lifshitz backgrounds, relate $M$-orbit structure to symmetry breaking/enhancement, and discuss the boundary field theory implications, including conserved particle-number currents and the role of the Stückelberg sector. These results provide a coherent holographic dictionary for Lifshitz spacetimes, clarify the boundary geometry as TNC with torsion, and open avenues for non-relativistic hydrodynamics and condensed-matter applications in non-AdS holography.

Abstract

Holography for Lifshitz space-times corresponds to dual field theories on a fixed torsional Newton-Cartan (TNC) background. We examine the coupling of non-relativistic field theories to TNC backgrounds and uncover a novel mechanism by which a global U(1) can become local. This involves the TNC vector $M_μ$ which sources a particle number current, and which for flat NC space-time satisfies $M_μ=\partial_μM$ with a Schroedinger symmetry realized on $M$. We discuss various toy model field theories on flat NC space-time for which the new mechanism leads to extra global space-time symmetries beyond the generic Lifshitz symmetry, allowing for an enhancement to Schroedinger symmetry. On the holographic side, the source $M$ also appears in the Lifshitz vacuum with exactly the same properties as for flat NC space-time. In particular, the bulk diffeomorphisms that preserve the boundary conditions realize a Schroedinger algebra on $M$, allowing for a conserved particle number current. Finally, we present a probe action for a complex scalar field on the Lifshitz vacuum, which exhibits Schroedinger invariance in the same manner as seen in the field theory models.

Field Theory on Newton-Cartan Backgrounds and Symmetries of the Lifshitz Vacuum

TL;DR

The work advances a non-relativistic holographic program by coupling field theories to torsional Newton–Cartan boundaries and analyzing Lifshitz vacua, where the TNC vector sources a particle-number current and can be promoted to a gauge field. It shows that bulk PBH diffeomorphisms induce a local Schrödinger algebra on , enabling Schrödinger enhancements of Lifshitz symmetry in flat NC space-time and revealing how a nontrivial orbit of yields global Galilean and conformal-like symmetries. The authors develop Schrödinger-invariant probe actions on Lifshitz backgrounds, relate -orbit structure to symmetry breaking/enhancement, and discuss the boundary field theory implications, including conserved particle-number currents and the role of the Stückelberg sector. These results provide a coherent holographic dictionary for Lifshitz spacetimes, clarify the boundary geometry as TNC with torsion, and open avenues for non-relativistic hydrodynamics and condensed-matter applications in non-AdS holography.

Abstract

Holography for Lifshitz space-times corresponds to dual field theories on a fixed torsional Newton-Cartan (TNC) background. We examine the coupling of non-relativistic field theories to TNC backgrounds and uncover a novel mechanism by which a global U(1) can become local. This involves the TNC vector which sources a particle number current, and which for flat NC space-time satisfies with a Schroedinger symmetry realized on . We discuss various toy model field theories on flat NC space-time for which the new mechanism leads to extra global space-time symmetries beyond the generic Lifshitz symmetry, allowing for an enhancement to Schroedinger symmetry. On the holographic side, the source also appears in the Lifshitz vacuum with exactly the same properties as for flat NC space-time. In particular, the bulk diffeomorphisms that preserve the boundary conditions realize a Schroedinger algebra on , allowing for a conserved particle number current. Finally, we present a probe action for a complex scalar field on the Lifshitz vacuum, which exhibits Schroedinger invariance in the same manner as seen in the field theory models.

Paper Structure

This paper contains 38 sections, 255 equations.