2015
DOI: 10.1007/jhep01(2015)052
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Lifshitz holography: the whole shebang

Abstract: Journal of High Energy Physics 2015.1 (2015): 052 reproduced by permission of Scuola Internazionale Superiore di Studi Avanzati (SISSA)We provide a general algorithm for constructing the holographic dictionary for any asymptotically locally Lifshitz background, with or without hyperscaling violation, and for any values of the dynamical exponents z and θ, as well as the vector hyperscaling violating exponent [1, 2], that are compatible with the null energy condition. The analysis is carried out for a very gener… Show more

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Cited by 65 publications
(169 citation statements)
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“…The fact that Sct, which in this case is an algebraic function of the canonical variables, vanishes on-shell indicates that constant dilaton solutions satisfy a second class constraint. As it was shown in a different context in [71], the boundary counterterms are ambiguous up to second class constraints, but this ambiguity is lifted to linear order in the second class constraints by requiring that the canonical variables themselves are appropriately renormalized. More generically, the renormalization of n-point functions determines the counterterms up to order n in the second class constraints.…”
Section: Jhep12(2016)008mentioning
confidence: 99%
“…The fact that Sct, which in this case is an algebraic function of the canonical variables, vanishes on-shell indicates that constant dilaton solutions satisfy a second class constraint. As it was shown in a different context in [71], the boundary counterterms are ambiguous up to second class constraints, but this ambiguity is lifted to linear order in the second class constraints by requiring that the canonical variables themselves are appropriately renormalized. More generically, the renormalization of n-point functions determines the counterterms up to order n in the second class constraints.…”
Section: Jhep12(2016)008mentioning
confidence: 99%
“…More generally, we expect that the pressure is related to the O(r d+z ) contributions to f (r), though we note that the holographic renormalization for T µν can require some care, especially in Lifshitz theories [48]. With this particular choice for f (r), we find that for a rather general family of x-independent matter backgrounds that support a Lifshitz geometry, the equations of motion for the metric perturbation h xy , defined in (4.37), are independent of the details of the bulk matter:…”
Section: Jhep07(2017)149mentioning
confidence: 96%
“…These covariant temporal and spatial projectors have been introduced in [52,53] in the context of Lifshitz holography. Their applications can be found in e.g.…”
Section: Anisotropic Disformal Transformation In Newton-cartan Geometrymentioning
confidence: 99%