Abstract
The properties of the kaon, , and antikaon, $\kbar$, in nuclear medium are studied in the quark-meson coupling (QMC) model. Employing a constituent quark-antiquark (MIT bag model) picture, their excitation energies in a nuclear medium at zero momentum are calculated within mean field approximation. The scalar, and the vector mesons are assumed to couple directly to the nonstrange quarks and antiquarks in the and $\kbar$ mesons. It is demonstrated that the meson induces different mean field potentials for each member of the isodoublets, and $\kbar$, when they are embedded in asymmetric nuclear matter. Furthermore, it is also shown that this meson potential is repulsive for the meson in matter with a neutron excess, and renders condensation less likely to occur.
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