2010
DOI: 10.1088/0264-9381/27/6/065015
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Boundary terms unbound! Holographic renormalization of asymptotically linear dilaton gravity

Abstract: A variational principle is constructed for gravity coupled to an asymptotically linear dilaton and a p-form field strength. This requires the introduction of appropriate surface terms -also known as 'boundary counterterms' -in the action. The variation of the action with respect to the boundary metric yields a boundary stress tensor, which is used to construct conserved charges that generate the asymptotic symmetries of the theory. In most cases a minimal set of assumptions leads to a unique set of counterterm… Show more

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Cited by 19 publications
(30 citation statements)
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References 49 publications
(190 reference statements)
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“…This result matches with (138) in [56], where the mass was obtained from an approach of Brown and York [27] as well as of Hawking and Horowitz [57]. See also (6.17) of [58], where another approach was used.…”
Section: Linear Dilaton Backgroundsupporting
confidence: 84%
“…This result matches with (138) in [56], where the mass was obtained from an approach of Brown and York [27] as well as of Hawking and Horowitz [57]. See also (6.17) of [58], where another approach was used.…”
Section: Linear Dilaton Backgroundsupporting
confidence: 84%
“…Previously, three counter terms (different from ours) with undetermined coefficients were considered in the context of linear dilaton gravity [37]. For a certain value of dilaton coupling, one of the coefficient remains unfixed for a well defined variational problem.…”
Section: On-shell Actionmentioning
confidence: 95%
“…The letter are deformations of the Maldacena-dilaton (ALD) backgrounds. Recall that the linear dilaton behavior φ ∼ z refers actually to a different coordinate system (in string frame) than the conventional one (in Einstein frame), used in [30] to establish the holographic renormalization of ALD backgrounds.…”
Section: Summary and Discussionmentioning
confidence: 99%
“…For comparison of the two systems, see for example [31]. In the coordinate system of [30], that is relevant for us, the asymptotic behavior of the dilaton is φ ∼ c 1 ln z + c 2 + ... , where c 1,2 = const. Now, for the walking solutions of [18] the dilaton is constant, while it is zero here.…”
Section: Summary and Discussionmentioning
confidence: 99%