Quark and Gluon Helicity Evolution at Small : Revised and Updated
arXiv:2204.11898 · doi:10.1007/JHEP07(2022)095
Abstract
We revisit the problem of small Bjorken- evolution of the gluon and flavor-singlet quark helicity distributions in the shock wave (-channel) formalism. Earlier works on the subject in the same framework resulted in an evolution equation for the gluon field-strength and quark "axial current" operators (sandwiched between the appropriate light-cone Wilson lines) in the double-logarithmic approximation (DLA: summing powers of with the strong coupling constant). In this work, we observe that an important mixing of the above operators with another gluon operator, , also sandwiched between the light-cone Wilson lines (with the repeated index summed over), was missing in the previous works. This operator has the physical meaning of the sub-eikonal (covariant) phase: its contribution to helicity evolution is shown to be proportional to another sub-eikonal operator, , which is related to the Jaffe-Manohar polarized gluon distribution. In this work we include this operator into small- helicity evolution, and construct a novel evolution mixing all three operators (, , and ), generalizing the previous results. We also construct closed DLA evolution equations in the large- and large- limits, with and the numbers of quark colors and flavors, respectively. Solving the large- equations numerically we obtain the following small- asymptotics of the quark and gluon helicity distributions and , along with the structure function, \[ΔΣ(x,Q^2)\simΔG(x,Q^2)\sim g_1(x,Q^2)\sim\left(\frac{1}{x}\right)^{3.66\,\sqrt{\frac{α_s\,N_c}{2π}}},\] in complete agreement with the earlier work by Bartels, Ermolaev and Ryskin.
65 pages, 8 figures; v2, v3: typos corrected, comments added; v4: minor corrections in intermediate steps without changes to the final results
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