Searching for the Proton's Missing Spin: Small-$x$ Helicity Evolution Equations and Their Analytic Solutions

TL;DR

This paper derives and solves analytically the small-$x$ helicity evolution equations for the proton spin problem, enabling precise predictions of quark and gluon spin contributions at high energies.

Contribution

It provides the first analytic solutions to small-$x$ helicity evolution equations in large-$N_c$ and large-$N_c ext{ exttwosuperior}$ limits, including a correction for quark-to-gluon transitions.

Findings

Predicted small-$x$ helicity distributions as power laws and explicit expressions.

Derived all-order polarized DGLAP anomalous dimensions in the considered limits.

Confirmed agreement with existing three-loop finite-order calculations.

Abstract

The proton spin puzzle denotes the challenge of describing the proton's spin in terms of the angular momenta of the quarks and gluons which comprise it. These quarks and gluons carry a fraction $x$ of the proton's momentum. Contributions from small-$x$ quarks and gluons, which only possess a little of the proton's momentum, are difficult to measure, since this requires very high energy experiments. Furthermore, early theoretical work in the 1990s predicted substantial contributions to the proton spin from these small-$x$ particles. We need theoretical control over this corner of phase space in order to resolve the spin puzzle. In this dissertation, we build upon an existing framework for studying spin at small-$x$. Previously, several sets of small-$x$ evolution equations were derived in this formalism -- one in the large-$N_c$ limit and one in the large-$N_c\&N_f$ limit. Here $N_c$ and $N_f$ are the numbers of quark colors and flavors. These equations were numerically solved but no analytic solutions had been found. In this dissertation we detail the construction of such analytic solutions, first in the large-$N_c$ limit and then in the large-$N_c\&N_f$ limit, after deriving an important correction to the existing large-$N_c\&N_f$ equations due to the contributions of quark-to-gluon transition operators. From the solutions constructed here, we can predict the behavior of the quark and gluon helicity distributions at asymptotically small-$x$ (and large-$N_c$ or large-$N_c\&N_f$), both as a general power law and further as explicit analytic expressions in the asymptotic limit. Our solutions also allow us to predict all four polarized DGLAP anomalous dimensions in the same limits, yielding expressions exact to all orders in the strong coupling. The expansions of our predictions agree completely with the full extent of existing finite-order calculations, to three loops.