Abstract
There have been rapid developments in the direct calculation in lattice QCD (LQCD) of the Bjorken-$x$ dependence of hadron structure through large-momentum effective theory (LaMET). LaMET overcomes the previous limitation of LQCD to moments (that is, integrals over Bjorken-$x$) of hadron structure, allowing LQCD to directly provide the kinematic regions where the experimental values are least known. LaMET requires large-momentum hadron states to minimize its systematics and allow us to reach small-$x$ reliably. This means that very fine lattice spacing to minimize lattice artifacts at order $(P_z a)^n$ will become crucial for next-generation LaMET-like structure calculations. Furthermore, such calculations require operators with long Wilson-link displacements (in finer lattice units), increasing the communication costs relative to that of the propagator inversion. In this work, we explore whether machine-learning (ML) algorithms can make correlator predictions to reduce the computational cost of these LQCD calculations. We consider two algorithms, gradient-boosting decision tree and linear models, applied to LaMET data, the matrix elements needed to determine the kaon and $\eta_s$ unpolarized parton distribution functions (PDFs), meson distribution amplitude (DA), and the nucleon gluon PDF. We find that both algorithms can reliably predict the target observables with different fit quality and systematic errors. The predictions from smaller displacement $z$ to larger ones work better than those for momentum $p$ due to the higher correlation among the data.
Highlights
In the early days, probing hadron structure with lattice QCD (LQCD) was limited to only the first few moments, due to complications arising from the breaking of rotational symmetry by the discretized Euclidean spacetime
This paper focuses on the discussion with quasiPDF, what we learn here applies to the pseudo-PDF1 [27,28,29,30] correlators since the building blocks of matrix elements are the same
As Nambu-Goldstone bosons associated with dynamical chiral SU(3) symmetry breaking, the pion and kaon serve as a fundamental test ground for our understanding of QCD theory at the hadronic scale
Summary
In the early days, probing hadron structure with lattice QCD (LQCD) was limited to only the first few moments, due to complications arising from the breaking of rotational symmetry by the discretized Euclidean spacetime. Lattice-QCD results using LaMET already include the isovector quark PDF of the nucleon [10,11,12,13,14], the pion generalized parton distribution [15], the meson distribution amplitudes (DAs) [16,17] and the nonperturbative renormalization in the regularization-independent momentum subtraction scheme [18,19]. Most work so far has been limited to a single ensemble; more detailed studies incorporating the systematic errors from lattice artifacts, such as finite-volume and lattice spacing, is necessary to reach precision LQCD PDFs. Larger boost momentum in the hadron is important to suppress finite-momentum corrections, as well as getting the antiquark distribution and small-x quark distribution corrections.
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