Abstract
The presence of exotic hadrons, such as hyperons and Δ isobars, in the dense nuclear matter in their cores has been shown to produce important changes in the properties of neutron stars. Within the quark-meson coupling model, we show that the many-body forces generated by the change in the internal quark structure of the baryons in the strong scalar mean fields generated in dense nuclear matter prohibit the appearance of Δ isobars.
Highlights
The study of nuclear matter in β-equilibrium at densities above that of normal nuclear matter presents a number of outstanding challenges for modern nuclear theory
We have shown that the repulsive many-body forces that arise naturally in the quark-meson coupling (QMC) model from the quark substructure of the baryons increases the chemical potential of the ∆− in such a way that it cannot appear in a neutron star
For symmetric nuclear matter containing nucleons the internal response to the scalar mean field reduces the effective coupling to that field as the density rises, providing a novel saturation mechanism
Summary
The study of nuclear matter in β-equilibrium at densities above that of normal nuclear matter presents a number of outstanding challenges for modern nuclear theory. It leads to the complete absence of Σ-hyperons in NS within the QMC model [7, 30] It is this OGE hyperfine interaction which splits the ∆ from the nucleon in free space in essentially all quark models and, as we have just explained, this mass difference will be enhanced in-medium. Already at twice nuclear matter density the mass splitting is enhanced by almost 100 MeV This already suggests that within the QMC model it is unlikely that the ∆ baryon will make an appearance. Our aim is to study the chemical potential of the ∆ in matter in β-equilibrium within the QMC model in order to understand whether it is likely to appear at any density relevant to the physics of neutron stars.
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