Next-to-leading Bfkl ∗
نویسنده
چکیده
The representation of the total cross section at high energy √ 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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