  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.
