BFKL equation in the next-to-leading order: solution at large impact parameters
arXiv:1906.09603 · doi:10.1140/epjc/s10052-019-7363-6
Abstract
In this paper, we show (i) that the NLO corrections do not change the power-like decrease of the scattering amplitude at large impact parameter ($b^2 \,>\,r^2 \exp\left( 2\bar(α}_S η(1 + 4 \barα_S)\right)$, where denotes the size of scattering dipole and for DIS), and, therefore, they do not resolve the inconsistency with unitarity; and (ii) they lead to an oscillating behaviour of the scattering amplitude atlarge , in direct contradiction with the unitarity constraints. However, from the more practical point of view, the NLO estimates give a faster decrease of the scattering amplitude as a function of , and could be very useful for description of the experimental data. It turns out, that in a limited range of , the NLO corrections generates the fast decrease of the scattering amplitude with , which can be parameterized as with in accord with the numerical estimates in Ref.[1].
14 pp, 21 figures in pdf files
References in corpus (3)
Cited by in corpus (7)
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- Non-linear equation in the re-summed next-to-leading order of perturbative QCD: the leading twist approximation
- Impact-parameter-dependent solutions to the Balitsky-Kovchegov equation at next-to-leading order
- Contribution of the non-linear term in the Balitsky-Kovchegov equation to the nuclear structure functions