2026-07-072026-07-07http://salesiana.dossiersoluciones.com/handle/123456789/48074The representation of the total cross section at high energy $\sqrt s$ in the next-to-leading $\ln s$ approximation is given with definition of the impact factors and explicit expression for the BFKL kernel. The estimate of the Pomeron intercept and the next-to-leading contributions to anomalous dimensions near $j=1$ are presented.5 pages, latex, Talk given at the International Conference "DIS98", April 4-8, Brussels, Belgium, 1998High Energy Physics - PhenomenologyNext-to-Leading BFKLtext