We compute the three-point function of the stress-energy tensor in d-dimensional conformal field theory CFT from AdSd+1 gravity. For $d=4$ the coefficients of the three linearly independent conformally covariant forms entering the three-point function are exactly the same as given by the free-field computations in the N=4 SYM theory just as expected from the known renormalization theorems. For $d=3$ and $d=6$ our results give the value of the corresponding three-point function in the theories of strongly coupled N=8 superconformal scalar and (2,0) tensor multiplets, respectively.
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Arutyunov et al. (1999) studied this question.
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