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 . 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 , where the gluons dominate, and increased support at large . 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 behavior as predicted by perturbative QCD.
- Received 9 February 2019
DOI:https://doi.org/10.1103/PhysRevLett.124.042002
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