Multi- nuclei and kaon condensation
arXiv:0801.3335 · doi:10.1103/PhysRevC.77.045206
Abstract
We extend previous relativistic mean-field (RMF) calculations of multi- nuclei, using vector boson fields with SU(3) PPV coupling constants and scalar boson fields constrained phenomenologically. For a given core nucleus, the resulting separation energy , as well as the associated nuclear and -meson densities, saturate with the number of mesons for . Saturation appears robust against a wide range of variations, including the RMF nuclear model used and the type of boson fields mediating the strong interactions. Because generally does not exceed 200 MeV, it is argued that multi- nuclei do not compete with multihyperonic nuclei in providing the ground state of strange hadronic configurations and that kaon condensation is unlikely to occur in strong-interaction self-bound strange hadronic matter. Last, we explore possibly self-bound strange systems made of neutrons and mesons, or protons and mesons, and study their properties.
21 pages, 8 figures, revised text and references
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- Calculations of nuclear quasi-bound states based on chiral meson-baryon amplitudes
- Antikaon interactions with nucleons and nuclei
- Kaonic atoms and in-medium amplitudes
- Application of a coupled-channel Complex Scaling Method with Feshbach projection to the system
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- Comprehensive application of a coupled-channel complex scaling method to the KbarN-piY system
- Multi-antikaonic nuclei in the relativistic mean-field theory
- Constraints on the threshold K- nuclear potential from FINUDA (stopped K-, pi-) hypernuclear spectra
- High-density kaonic-proton matter (KPM) composed of Lambda* equiv K-p multiplets and its astrophysical connections
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- Overview of Strangeness Nuclear Physics
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- Antikaon-nucleus dynamics: from quasibound states to kaon condensation
- Old and New in Strangeness Nuclear Physics