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Next-to-Leading BFKL

V. S. Fadin
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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.

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V. S. Fadin. 1998-07-29. Next-to-Leading BFKL. https://arxiv.org/abs/hep-ph/9807527

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