Quark and Gluon Helicity Evolution at Small $x$: Revised and Updated

TL;DR

This paper refines the small-$x$ helicity evolution equations by including an operator previously omitted, leading to a more complete understanding of quark and gluon helicity distributions at small Bjorken-$x$ in QCD.

Contribution

It introduces a new operator into the small-$x$ helicity evolution equations, generalizing previous models and providing a more comprehensive framework for understanding helicity distributions.

Findings

Derived closed DLA evolution equations in large-$N_c$ and large-$N_c ext{&}N_f$ limits.

Numerically solved equations show asymptotic behavior of helicity distributions as $x$ approaches zero.

Results agree with earlier theoretical predictions by Bartels, Ermolaev, and Ryskin.

Abstract

We revisit the problem of small Bjorken-$x$ evolution of the gluon and flavor-singlet quark helicity distributions in the shock wave ($s$-channel) formalism. Earlier works on the subject in the same framework resulted in an evolution equation for the gluon field-strength $F^{12}$ and quark "axial current" ${\bar\psi}\gamma^+\gamma^5\psi$ operators (sandwiched between the appropriate light-cone Wilson lines) in the double-logarithmic approximation (DLA: summing powers of $\alpha_s\,\ln^2(1/x)$ with $\alpha_s$ the strong coupling constant). In this work, we observe that an important mixing of the above operators with another gluon operator, $\overleftarrow{D}^i\,{D}^i$, also sandwiched between the light-cone Wilson lines (with the repeated index $i=1,2$ 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, $D^i-\overleftarrow{D}^i$, which is related to the Jaffe-Manohar polarized gluon distribution. In this work we include this operator into small-$x$ helicity evolution, and construct a novel evolution mixing all three operators ($D^i-\overleftarrow{D}^i$, $F^{12}$, and ${\bar\psi}\gamma^+\gamma^5\psi$), generalizing the previous results. We also construct closed DLA evolution equations in the large-$N_c$ and large-$N_c\& N_f$ limits, with $N_c$ and $N_f$ the numbers of quark colors and flavors, respectively. Solving the large-$N_c$ equations numerically we obtain the following small-$x$ asymptotics of the quark and gluon helicity distributions $\Delta \Sigma$ and $\Delta G$, along with the $g_1$ structure function, \[\Delta\Sigma(x,Q^2)\sim\Delta G(x,Q^2)\sim g_1(x,Q^2)\sim\left(\frac{1}{x}\right)^{3.66\,\sqrt{\frac{\alpha_s\,N_c}{2\pi}}},\] in complete agreement with the earlier work by Bartels, Ermolaev and Ryskin.