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The holographic Weyl anomaly
Author(s) -
Måns Henningson,
Kostas Skenderis
Publication year - 1998
Publication title -
journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1088/1126-6708/1998/07/023
Subject(s) - conformal anomaly , anomaly (physics) , gravitational anomaly , physics , mixed anomaly , supergravity , mathematical physics , gauge anomaly , central charge , general covariance , conformal field theory , gauge theory , gravitation , weyl transformation , symmetry (geometry) , conformal map , theoretical physics , supersymmetric gauge theory , quantum mechanics , mathematics , geometry , general relativity , supersymmetry , introduction to the mathematics of general relativity , numerical relativity
We calculate the Weyl anomaly for conformal field theories that can bedescribed via the adS/CFT correspondence. This entails regularizing thegravitational part of the corresponding supergravity action in a mannerconsistent with general covariance. Up to a constant, the anomaly only dependson the dimension d of the manifold on which the conformal field theory isdefined. We present concrete expressions for the anomaly in the physicallyrelevant cases d = 2, 4 and 6. In d = 2 we find for the central charge c = 3 l/2 G_N in agreement with considerations based on the asymptotic symmetry algebraof adS_3. In d = 4 the anomaly agrees precisely with that of the correspondingN = 4 superconformal SU(N) gauge theory. The result in d = 6 provides newinformation for the (0, 2) theory, since its Weyl anomaly has not been computedpreviously. The anomaly in this case grows as N^3, where N is the number ofcoincident M5 branes, and it vanishes for a Ricci-flat background.Comment: 12 pages, Latex, v2: minor improvement

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