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Analytic Solution for the Helicity Evolution Equations at Small x and Large N_c\&N_f

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arxiv 2508.00195 v1 pith:E5XPT4GX submitted 2025-07-31 hep-ph nucl-th

Analytic Solution for the Helicity Evolution Equations at Small x and Large N_c\&N_f

classification hep-ph nucl-th
keywords alphahelicitydeltaanalyticequationsevolutionexpressionsgamma
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We construct an exact analytic solution of the revised small-$x$ helicity evolution equations, where the contributions of the quark-to-gluon and gluon-to-quark transition operators were newly included. These evolution equations are written in the large-$N_c\&N_f$ limit and are double-logarithmic, resumming powers of $\alpha_s\ln^2(1/x)$. Here $N_c$ and $N_f$ are the numbers of quark colors and flavors, while $\alpha_s$ is the strong coupling constant and $x$ is the Bjorken-$x$ variable. Using our solution, we obtain analytic expressions for the flavor singlet quark and gluon helicity parton distribution functions (PDFs) and for the $g_1$ structure function as double-inverse Laplace transforms. We also extract analytic expressions for the four DGLAP polarized anomalous dimensions $\Delta \gamma_{qq}, \Delta \gamma_{qG}, \Delta \gamma_{Gq}$, and $\Delta \gamma_{GG}$: these expressions resum powers of $\alpha_s/\omega^2$ to all orders at large-$N_c\&N_f$ (with $\omega$ the Mellin moment variable). We extract the leading small-$x$ growth of the helicity distributions, \begin{align} \Delta\Sigma(x,Q^2) \sim \Delta G(x,Q^2)\sim g_1(x,Q^2) \sim \left(\frac{1}{x}\right)^{\alpha_h}, \end{align} where the intercept $\alpha_h$ satisfies an algebraic equation. We determine $\alpha_h$ numerically for various values of $N_c$ and $N_f$. We further obtain the explicit asymptotic expressions for the helicity distributions, which yield numerical values for the ratio of the gluon helicity PDF to the flavor singlet quark helicity PDF in the small-$x$ asymptotic limit (for different $N_f/N_c$). We find that all our predictions for polarized DGLAP anomalous dimensions are fully consistent with the existing finite-order calculations. Similar to the large-$N_c$ case, our intercept $\alpha_h$ exhibits a very slight disagreement with the predictions made within the infrared evolution equations framework.

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Cited by 4 Pith papers

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  1. Sub-eikonal stress and model dependence of the small-$x$ gluon D-term

    hep-ph 2026-07 unverdicted novelty 7.0

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  2. Sub-eikonal stress and model dependence of the small-$x$ gluon D-term

    hep-ph 2026-07 conditional novelty 6.0

    The small-x gluon D-term is a next-to-eikonal stress probe and is not fixed by the leading-eikonal dipole or saturation profile alone.

  3. On the Two $R$-Factors in the Small-$x$ Shockwave Formalism

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  4. Spin Structure of the Nucleon: Overview

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    A pedagogical review consolidates the proton spin decomposition into quark/gluon spin and orbital angular momentum, emphasizing gauge-invariant OAM definitions, small-x cancellations, and EIC observables.