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We review the result for the BFKL Pomeron intercept at N=4 Supersymmetric Yang-Mills model in the form of the inverse coupling expansion $j_0=2-2\lambda^{-1/2}-\lambda^{-1} + 1/4 , \lambda^{-3/2} + 2(3\zeta_3+1) , \lambda^{-2} +(18\zeta_3+361/64) , \lambda^{-5/2} + (39\zeta_3+447/32) , \lambda^{-3} + O(\lambda^{-7/2})$ which has been calculated in [1]-[5] with the use of the AdS/CFT correspondence.

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