Abstract

We review the result for the BFKL Pomeron intercept at N=4 Supersymmetric Yang-Mills model in the form of the inverse coupling expansion j0=2−2λ−1/2−λ−1+1/4 λ−3/2+2(3ζ3+1) λ−2+(18ζ3+361/64) λ−5/2+(39ζ3+447/32) λ−3+O(λ−7/2)j_0=2-2λ^{-1/2}-λ^{-1} + 1/4 \, λ^{-3/2} + 2(3ζ_3+1) \, λ^{-2} +(18ζ_3+361/64) \, λ^{-5/2} + (39ζ_3+447/32) \, λ^{-3} + O(λ^{-7/2}) which has been calculated in [1]-[5] with the use of the AdS/CFT correspondence.

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