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Conformal Lifshitz Gravity from Holography

Tom Griffin, Petr Horava, Charles M. Melby-Thompson

TL;DR

This work shows that holographic renormalization in asymptotically Lifshitz spacetimes naturally yields gravity with anisotropic scaling, where near anisotropic infinity the counterterms reproduce a Lifshitz-conformal gravitational action with the correct dynamical exponent $z$. In the key case of $3+1$ bulk dimensions and $z=2$, a logarithmic counterterm emerges that matches the action of $z=2$ conformal gravity in $2+1$ dimensions and enforces detailed balance, a relation that persists when bulk scalars are included. The authors develop a Hamiltonian holographic renormalization framework, compute the divergences for bulk gravity with a massive vector (and with scalars), and show that detailed balance is a structural consequence of the holographic counterterm relations, with an analytic continuation linking the result to a de Sitter-like regime and a peculiar, spatially anisotropic ground-state wavefunction. Overall, the paper provides a string-theory-inspired holographic route to multicritical gravity and clarifies the role of anisotropic Weyl invariance and detailed balance in the Lifshitz holographic context, offering paths to generalize to higher $z$ and richer bulk embeddings.

Abstract

We show that holographic renormalization of relativistic gravity in asymptotically Lifshitz spacetimes naturally reproduces the structure of gravity with anisotropic scaling: The holographic counterterms induced near anisotropic infinity take the form of the action for gravity at a Lifshitz point, with the appropriate value of the dynamical critical exponent $z$. In the particular case of 3+1 bulk dimensions and $z=2$ asymptotic scaling near infinity, we find a logarithmic counterterm, related to anisotropic Weyl anomaly of the dual CFT, and show that this counterterm reproduces precisely the action of conformal gravity at a $z=2$ Lifshitz point in 2+1 dimensions, which enjoys anisotropic local Weyl invariance and satisfies the detailed balance condition. We explain how the detailed balance is a consequence of relations among holographic counterterms, and point out that a similar relation holds in the relativistic case of holography in $AdS_5$. Upon analytic continuation, analogous to the relativistic case studied recently by Maldacena, the action of conformal gravity at the $z=2$ Lifshitz point features in the ground-state wavefunction of a gravitational system with an interesting type of spatial anisotropy.

Conformal Lifshitz Gravity from Holography

TL;DR

This work shows that holographic renormalization in asymptotically Lifshitz spacetimes naturally yields gravity with anisotropic scaling, where near anisotropic infinity the counterterms reproduce a Lifshitz-conformal gravitational action with the correct dynamical exponent . In the key case of bulk dimensions and , a logarithmic counterterm emerges that matches the action of conformal gravity in dimensions and enforces detailed balance, a relation that persists when bulk scalars are included. The authors develop a Hamiltonian holographic renormalization framework, compute the divergences for bulk gravity with a massive vector (and with scalars), and show that detailed balance is a structural consequence of the holographic counterterm relations, with an analytic continuation linking the result to a de Sitter-like regime and a peculiar, spatially anisotropic ground-state wavefunction. Overall, the paper provides a string-theory-inspired holographic route to multicritical gravity and clarifies the role of anisotropic Weyl invariance and detailed balance in the Lifshitz holographic context, offering paths to generalize to higher and richer bulk embeddings.

Abstract

We show that holographic renormalization of relativistic gravity in asymptotically Lifshitz spacetimes naturally reproduces the structure of gravity with anisotropic scaling: The holographic counterterms induced near anisotropic infinity take the form of the action for gravity at a Lifshitz point, with the appropriate value of the dynamical critical exponent . In the particular case of 3+1 bulk dimensions and asymptotic scaling near infinity, we find a logarithmic counterterm, related to anisotropic Weyl anomaly of the dual CFT, and show that this counterterm reproduces precisely the action of conformal gravity at a Lifshitz point in 2+1 dimensions, which enjoys anisotropic local Weyl invariance and satisfies the detailed balance condition. We explain how the detailed balance is a consequence of relations among holographic counterterms, and point out that a similar relation holds in the relativistic case of holography in . Upon analytic continuation, analogous to the relativistic case studied recently by Maldacena, the action of conformal gravity at the Lifshitz point features in the ground-state wavefunction of a gravitational system with an interesting type of spatial anisotropy.

Paper Structure

This paper contains 29 sections, 149 equations.