Polarized Deep Inelastic Scattering as $x \to 1$ using Soft Collinear Effective Theory

TL;DR

This paper employs Soft Collinear Effective Theory to analyze polarized Deep Inelastic Scattering structure functions near the limit x→1, summing Sudakov logarithms and computing anomalous dimensions for improved understanding.

Contribution

It introduces a SCET-based factorization and resummation framework for polarized DIS at large x, including subleading operators and one-loop matching calculations.

Findings

Computed one-loop matching coefficients from QCD to SCET operators.

Derived the x→1 anomalous dimension of the parton distribution function.

Established the N→∞ behavior of QCD coefficient functions for structure functions.

Abstract

We use Soft Collinear Effective Theory (SCET) to factorize the polarized Deep Inelastic Scattering (DIS) structure functions $g_1(x)$ and $g_2(x)$, and to sum Sudakov double logarithms of $1-x$. The analysis is done both in terms of lightcone parton distributions and their moments. Computing $g_2$ requires subleading SCET operators which contain gluons. We calculate the one-loop matching coefficients from QCD onto these subleading SCET operators, and the one-loop matching from SCET onto the parton distribution function (PDF). The PDF in SCET is given by a bilocal operator, rather than the trilocal operator used in the QCD analysis of $g_2$ for generic $x$. We compute the one-loop anomalous dimension of the PDF operator for any $x$, and show that as $x \to 1$, it factors into a single-variable evolution. We comment on the QCD anomalous dimensions of twist-three operators, their equation-of-motion relation, and connection to the SCET analysis. We briefly discuss the definition of axial operators in the BMHV scheme. As a side result, we derive the $1/N$ dependence of the QCD coefficient functions for $F_1$, $F_L$ and $g_1$ in the $N \to \infty$ limit, where $N$ is the moment, which is expected to hold to all orders in $\alpha_s$.