Abstract

Determination of the intercept of the BFKL pomeron is one of the pressing issues in the high energy physics. Earlier we have shown that, at the dipole size r= rΔ=(0.1–0.2)fm, the dipole cross section σ( x, r) which is a solution of the generalized BFKL equation, exhibits a precocious asymptotic behavior σ(x, r)∝( 1 x ) Δ P . In this paper we discuss how measuring F L(x, Q 2) and ∂F T(x, Q 2) ∂ logQ 2 at Q 2=(10–40)GeV 2 and Q 2=(2–10)GeV 2, respectively, one can probe σ( x, rΔ) and directly determine the intercept Δ P of the BFKL pomeron in the HERA experiments.

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