Abstract

In-medium valence-quark distributions of $\pi^+$ and $K^+$ mesons in symmetric nuclear matter are studied by combining the Nambu--Jona-Lasinio model and the quark-meson coupling model. The in-medium properties of the current quarks, which are used as inputs for studying the in-medium pion and kaon properties in the Nambu--Jona-Lasinio model, are calculated within the quark-meson coupling model. The light-quark condensates, light-quark dynamical masses, pion and kaon decay constants, and pion- and kaon-quark coupling constants are found to decrease as nuclear density increases. The obtained valence quark distributions in vacuum for both the $\pi^+$ and $K^+$ could reasonably describe the available experimental data over a wide range of Bjorken-$x$. The in-medium valence $u$-quark distribution in the $\pi^+$ at $Q^2=16~\mbox{GeV}^2$ is found to be almost unchanged compared to the in-vacuum case. However, the in-medium to in-vacuum ratios of both the valence $u$-quark and valence $s$-quark distributions of the $K^+$ meson at $Q^2=16~\mbox{GeV}^2$ increase with nuclear matter density, but show different $x$-dependence. Namely, the ratio for the valence $u$-quark distribution increases with $x$, while that for the valence $s$ quark decreases with $x$. These features are enhanced at higher density regions.

Highlights

  • Pions and kaons, which emerge as a consequence of dynamical chiral symmetry breaking [1], play very important and special roles in understanding the nonperturbative features of low-energy quantum chromodynamics (QCD) [2]

  • In the present work we study the valence-quark distributions of both the πþ and Kþ mesons in symmetric nuclear matter based on the NJL model with an improved treatment for the nuclear medium effects

  • As quark properties are modified in nuclear medium, it is quite natural to expect that the quark distributions or parton distribution functions (PDFs) of mesons are modified in medium

Read more

Summary

INTRODUCTION

Pions and kaons, which emerge as a consequence of dynamical chiral symmetry breaking [1], play very important and special roles in understanding the nonperturbative features of low-energy quantum chromodynamics (QCD) [2]. The nonperturbative aspects of QCD can be accessed through the elastic electromagnetic form factors, and quark distribution functions of these mesons [3,4,5] as well as hadron distribution functions in the low-Q2 region, where the latter quantities are used as inputs for Q2-evolution to high-Q2 region that the perturbative QCD phenomena are experimentally accessible They can provide us with important information on the internal structure of pions and kaons as well as the quark and gluon dynamics. The NJL model was applied for studying the kaon electromagnetic form factor and valence-quark distributions in vacuum [5], as well as the in-medium electroweak properties of pions [41].

PION AND KAON FREE-SPACE PROPERTIES IN THE NJL MODEL
IN-MEDIUM QUARK PROPERTIES IN THE QMC MODEL
IN-MEDIUM PION AND KAON PROPERTIES
IN-MEDIUM VALENCE-QUARK DISTRIBUTIONS OF PIONS AND KAONS
Findings
SUMMARY
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call