Boundary terms and three-point functions: an AdS/CFT puzzle resolved

N= 8 superconformal field theories, such as the ABJM theory at Chern-Simons level k = 1 or 2, contain 35 scalar operators O I J with Δ = 1 in the 35 v representation of SO(8). The 3-point correlation function of these operators is non-vanishing, and indeed can be calculated non-perturbatively in the...

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Main Authors: Pilch, Krzysztof (Author), Warner, Nicholas P. (Author), Freedman, Daniel Z (Contributor), Pufu, Silviu (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Mathematics (Contributor), Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: Springer Nature, 2018-06-25T14:40:07Z.
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Online Access:Get fulltext
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100 1 0 |a Pilch, Krzysztof  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Mathematics  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Freedman, Daniel Z  |e contributor 
100 1 0 |a Pufu, Silviu  |e contributor 
700 1 0 |a Warner, Nicholas P.  |e author 
700 1 0 |a Freedman, Daniel Z  |e author 
700 1 0 |a Pufu, Silviu  |e author 
245 0 0 |a Boundary terms and three-point functions: an AdS/CFT puzzle resolved 
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856 |z Get fulltext  |u http://hdl.handle.net/1721.1/116553 
520 |a N= 8 superconformal field theories, such as the ABJM theory at Chern-Simons level k = 1 or 2, contain 35 scalar operators O I J with Δ = 1 in the 35 v representation of SO(8). The 3-point correlation function of these operators is non-vanishing, and indeed can be calculated non-perturbatively in the field theory. But its AdS 4 gravity dual, obtained from gauged N= 8 supergravity, has no cubic A 3 couplings in its Lagrangian, where A IJ is the bulk dual of O I J . So conventional Witten diagrams cannot furnish the field theory result. We show that the extension of bulk supersymmetry to the AdS 4 boundary requires the introduction of a finite A 3 counterterm that does provide a perfect match to the 3-point correlator. Boundary supersymmetry also requires infinite counterterms which agree with the method of holographic renormalization. The generating functional of correlation functions of the Δ = 1 operators is the Legendre transform of the on-shell action, and the supersymmetry properties of this functional play a significant role in our treatment. 
655 7 |a Article 
773 |t Journal of High Energy Physics