Abstract
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.