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

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.

Figures (18)

• Figure 1.1: Naive quark model of the proton $P$ with two quark $q$ spins aligned and one anti-aligned relative to the proton spin.
• Figure 1.2: A more complicated but realistic illustration of the proton's structure. In addition to the three valence quarks (the large spheres), we now have a sea of quarks and antiquarks (the smaller colorful spheres) along with many gluons (the corkscrew lines). The spins of the particles are not represented here, but each quark and gluon can contribute its spin --- and also its orbital angular momentum --- to the proton's spin.
• Figure 2.3: Diagrammatic representation of deep inelastic electron-proton scattering in the proton's rest frame. The proton (gray oval) is illustrated as a collection of quarks and gluons.
• Figure 2.4: Deep inelastic scattering in the framework of dipole picture. The interaction between the $q\overline{q}$ dipole and the proton (P) is denoted with a gray oval. The antiquark is located at transverse coordinate $\underline{x}_0$, while the quark is located at transverse coordinate $\underline{x}_1$, with the transverse separation labeled $\underline{x}_{10} = \underline{x}_1 - \underline{x}_0$.
• Figure 2.5: Dipole-nucleon scattering in the Glauber-Gribov-Mueller model. For more detailed versions of these figures, see Ch. 4 of Kovchegov:2012mbw.