2003
DOI: 10.1088/1126-6708/2003/10/001
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Universal features of holographic anomalies

Abstract: We study the mechanism by which gravitational actions reproduce the trace anomalies of the holographically related conformal field theories. Two universal features emerge: a) the ratios of type B trace anomalies in any even dimension are independent of the gravitational action being uniquely determined by the underlying algebraic structure b) the normalization of the type A and the overall normalization of the type B anomalies are given by action dependent expressions with the dimension dependence completely f… Show more

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Cited by 34 publications
(36 citation statements)
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References 22 publications
(34 reference statements)
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“…The effective theory we develop may have broader applications for the study of holographic phenomenology [27,28], where our methods could be used to derive both the universal anomaly matching terms and the conformally invariant terms for light dilatons. Our methods might also relate to 6 WhenM I 1 is far away from this central value, it will lead to ghosts or negligible mixing [36].…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The effective theory we develop may have broader applications for the study of holographic phenomenology [27,28], where our methods could be used to derive both the universal anomaly matching terms and the conformally invariant terms for light dilatons. Our methods might also relate to 6 WhenM I 1 is far away from this central value, it will lead to ghosts or negligible mixing [36].…”
Section: Discussionmentioning
confidence: 99%
“…Thus our approach may be viewed as intermediate between a general conformal symmetry analysis [5][6][7][8][9] and the study of particular holographic examples (see [10] for a review and many older references e.g. [11], and also the recent work [12][13][14][15]) for the study of the low-energy τ action.…”
Section: Jhep02(2015)056mentioning
confidence: 99%
“…In general, any spacetime metric can be put in Gaussnormal coordinates ds 2 = N 2 (ρ)dρ 2 + h ij (x, ρ)dx i dx j . For AAdS spaces in EGB gravity (3), the FeffermanGraham expansion of the metric is also valid and defined by N = ℓ eff /2ρ, h ij = g ij (x, ρ)/ρ and the expansion g ij = g (0)ij +ρg (1)ij +ρ 2 g (2)ij +..., where g (0) represents the metric of the conformal boundary ρ = 0 [11,12]. The extrinsic curvature K ij = −∂ ρ h ij /2N takes the form…”
mentioning
confidence: 99%
“…In particular, in [22], general formulas for Asymptotically locally AdS spacetimes have been displayed. Dimensional regularization is also available with equivalent results [24,25,26]. A Hamilton-Jacobi method, exploiting the gravitational Hamiltonian constraint, is also available [27].…”
Section: Now the Approximation (4) Is Valid Provided The Action I[φ]mentioning
confidence: 99%