Distinguishing Quarks and Gluons in Pion and Kaon Parton Distribution Functions

Kyle D. Bednar, Ian C. Cloët, and Peter C. Tandy
Phys. Rev. Lett. 124, 042002 – Published 31 January 2020

Abstract

The leading-twist parton distribution functions of the pion and kaon are calculated for the first time using a rainbow-ladder truncation of QCD’s Dyson-Schwinger equations (DSEs) that self-consistently sums all planar diagrams. The nonperturbative gluon dressing of the quarks is thereby correctly accounted for, which in practice means solving the inhomogeneous Bethe-Salpeter equation (BSE) for the quark operator that defines the spin-independent quark distribution functions. An immediate consequence of using this dressed vertex is that gluons carry 35% of the pion’s and 30% of the kaon’s light-cone momentum, with the remaining momentum carried by the quarks. The scale associated with these DSE results is μ0=0.78GeV. The gluon effects generated by the inhomogeneous BSE are inherently nonperturbative and cannot be mimicked by the perturbative QCD evolution equations. A key consequence of this gluon dressing is that the valence quarks have reduced support at low-to-intermediate x, where the gluons dominate, and increased support at large x. As a result, our DSE calculation of the pion’s valence quark distribution is in excellent agreement with the Conway et al. pion-induced Drell-Yan data, but nevertheless exhibits the qπ(x)(1x)2 behavior as x1 predicted by perturbative QCD.

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  • Received 9 February 2019

DOI:https://doi.org/10.1103/PhysRevLett.124.042002

© 2020 American Physical Society

Physics Subject Headings (PhySH)

Particles & Fields

Authors & Affiliations

Kyle D. Bednar1,2, Ian C. Cloët2, and Peter C. Tandy1,3

  • 1Center for Nuclear Research, Department of Physics, Kent State University, Kent Ohio 44242, USA
  • 2Physics Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
  • 3CSSM, Department of Physics, University of Adelaide, Adelaide South Australia 5005, Australia

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Issue

Vol. 124, Iss. 4 — 31 January 2020

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