Next-to-Leading BFKL

Abstract

The 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.

Comments: 5 pages, latex, Talk given at the International Conference "DIS98", April 4-8, Brussels, Belgium, 1998