Abstract
We present the first direct lattice-QCD calculation of the $\mathrm{Bjorken}\text{\ensuremath{-}}x$ dependence of the valence quark distribution of the pion. Using large-momentum effective theory (LaMET), we calculate the boosted pion state with long Wilson link operators. After implementing the one-loop matching and meson mass corrections, our result at ${m}_{\ensuremath{\pi}}\ensuremath{\approx}310\text{ }\text{ }\mathrm{MeV}$ is in agreement with those extracted from experimental data as well as from the Dyson-Schwinger equation in the $\mathrm{small}\text{\ensuremath{-}}x$ region, but there is a sizeable discrepancy in the $\mathrm{large}\text{\ensuremath{-}}x$ region. This discrepancy provides a nice opportunity to systematically study and disentangle the artifacts in the LaMET approach, which will eventually help to discern various existing analyses in the literature.
Highlights
The pion plays a fundamental role in QCD
In parallel with the progress using the large-momentum effective theory (LaMET) approach, other proposals to calculate the parton distribution function (PDF) in lattice QCD have been formulated [27,28,76,77,78,79,80,81,82], each of which is subject to its own systematics
Following our previous studies of nucleon PDFs [65], we perform nonperturbative renormalization in the RI/ MOM scheme, but we show the result from Wilson line renormalization in intermediate steps for comparison and to estimate the size of systematic uncertainties
Summary
The pion plays a fundamental role in QCD. As the lightest meson and the Goldstone boson associated with dynamical chiral symmetry breaking, it provides an important testing ground for our understanding of nonperturbative QCD. (3) Convert it to the PDF through a factorization formula accurate up to power corrections suppressed by the hadron momentum The existence of such a factorization is ensured by construction; for a proof, see Refs. In parallel with the progress using the LaMET approach, other proposals to calculate the PDFs in lattice QCD have been formulated [27,28,76,77,78,79,80,81,82], each of which is subject to its own systematics. We carry out the first direct lattice calculation for the valence quark distribution of the pion using the LaMET approach. Our results are comparable quantitatively with the results extracted from experimental data [7] as well as from the Dyson-Schwinger equation [14]
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