Abstract

In this paper we study the gluon and valence quark distributions in the pion and kaon in nuclear medium for various nuclear densities as well as in vacuum within the Nambu--Jona-Lasinio (NJL) model with the help of the proper-time regularization scheme which simulates a confinement of QCD. The nuclear medium effect is also determined in the same model for the symmetric nuclear matter. We then analyze the gluon and valence quark distributions for the bound pion and kaon in symmetric nuclear matter as well as those in vacuum. We find that the valence quark and gluon distributions in vacuum have relatively good agreements with the experimental data, the lattice QCD simulations, and the JAM Monte-Carlo (MC) global fit QCD analysis. Evolving to the higher factorization scale $Q=4\text{ }\text{ }\mathrm{GeV}$, the in-medium gluon and valence-quark distributions of the pion for various nuclear densities are turned out to be almost unchanged in comparison to the vacuum cases. On the contrary, for the kaon, they increase significantly with respect to the densities. Finally, we find that the vacuum gluon distribution for the kaon is smaller than that for the pion, which is consistent with other theoretical predictions. This feature holds for the in-medium gluon distribution in the nuclear density up to the saturation density.

Highlights

  • Parton distribution functions (PDFs) play important roles in describing the nonperturbative aspects of quantum chromodynamics (QCD) for the internal structure of the hadron bound states [1]

  • We find that the valence quark and gluon distributions in vacuum have relatively good agreements with the experimental data, the lattice QCD simulations, and the Jefferson Lab Angular Momentum Collaboration (JAM) Monte-Carlo (MC) global fit QCD analysis

  • Our result shows a good agreement with the results from the lattice QCD simulation [16], and the JAM phenomenology global fit QCD analysis [5]

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Summary

INTRODUCTION

Parton distribution functions (PDFs) play important roles in describing the nonperturbative aspects of quantum chromodynamics (QCD) for the internal structure of the hadron bound states [1]. But for the nucleon case, a very recent study was made to investigate the gluon distributions of nucleon in vacuum compared with those in the nuclei using the NJL model [22] They found the significant effects of the medium modifications for the unpolarized and polarized gluon distributions of bound nucleon in nuclear matter. They reported that, in their work, the gluon distributions of the nucleon at scale Q2 were dynamically generated via next-to-leading order (NLO) DokshitzerGribov-Lipatov-Altarelli-Parisi (DGLAP) QCD evolution [23], meaning that it is no gluon dynamics at initial scale Inspired by these recent studies, for the first time we study in the present work the pion and kaon gluon distributions in nuclear medium in the framework of the NJL model with the help of the proper-time regularization (PTR) scheme, simulating a confinement of QCD.

NAMBU–JONA-LASINIO MODEL
Vacuum pion and kaon parton distributions
Nuclear matter NJL model
In-medium pion and kaon parton distributions
NUMERICAL RESULT
SUMMARY
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