Abstract

We extract the pion valence quark distribution $q^\pi_{\rm v}(x)$ from lattice QCD (LQCD) calculated matrix elements of spacelike correlations of one vector and one axial vector current analyzed in terms of QCD collinear factorization, using a new short-distance matching coefficient calculated to one-loop accuracy. We derive the Ioffe time distribution of the two-current correlations in the physical limit by investigating the finite lattice spacing, volume, quark mass, and higher-twist dependencies in a simultaneous fit of matrix elements computed on four gauge ensembles. We find remarkable consistency between our extracted $q^\pi_{\rm v}(x)$ and that obtained from experimental data across the entire $x$-range. Further, we demonstrate that the one-loop matching coefficient relating the LQCD matrix computed in position space to the $q_{\rm v}^{\pi}(x)$ in momentum space has well-controlled behavior with Ioffe time. This justifies that LQCD calculated current-current correlations are good observables for extracting partonic structures by using QCD factorization, which complements to the global effort to extract partonic structure from experimental data.

Highlights

  • The pion, being both a Nambu-Goldstone boson and the lightest bound state in quantum chromodynamics (QCD), highlights the challenges in creating consistent theoretical and phenomenological frameworks to describe its partonic structure

  • We find that our calculated next-to-leading order (NLO) coefficient function, matching what is calculated in lattice QCD (LQCD) in position space to parton distribution functions (PDFs) in momentum space, is very stable without the large logarithms that are often seen in the perturbatively calculated hard coefficients in momentum space

  • It might be difficult to pin down the exact “power of (1 − x)” of the pion PDFs, the extraction of PDFs from future improved LQCD calculations of good hadron matrix elements, the lattice cross sections” (LCSs) that are calculable in LQCD and factorizable to PDFs, might help improve the accuracy of determining this “power,” since the matching coefficients for LCSs in position space are more perturbatively stable at larger x than the momentum-space matching coefficients for experimentally measured cross sections

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Summary

Introduction

The pion, being both a Nambu-Goldstone boson and the lightest bound state in quantum chromodynamics (QCD), highlights the challenges in creating consistent theoretical and phenomenological frameworks to describe its partonic structure. The shape of the pion valence parton distribution functions (PDFs) extracted from experimental data [1,2,3,4,5] in different analyses [6,7,8,9,10,11,12] are in sharp contrast among themselves and with perturbative QCD (pQCD)-based frameworks [13,14] at large longitudinal momentum fractions x.

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