{
  "annotation_id": "1e5ca04b-d8fb-4814-9d33-971738965681",
  "date_created": "2026-03-02T18:00:01.429000Z",
  "date_modified": "2026-03-02T18:00:01.429000Z",
  "file_hash": "a9d0f7b574085945763815c8c31266c346044895522faa8cb32dff351428451d",
  "private": false,
  "record": {
    "abstract": "The relativistic mean field (RMF) model is applied to a system of nucleons\nand a $\\bar K$ meson, interacting via scalar and vector boson fields. The model\nincorporates the standard RMF phenomenology for bound nucleons and, for the\n$\\bar K$ meson, it relates to low-energy ${\\bar K}N$ and $K^-$ atom\nphenomenology. Deeply bound $\\bar K$ nuclear states are generated dynamically\nacross the periodic table and are exhibited for $^{12}$C and $^{16}$O over a\nwide range of binding energies. Substantial polarization of the core nucleus is\nfound for these light nuclei. Absorption modes are also included dynamically,\nconsidering explicitly the reduced phase space for $\\bar K$ absorption from\ndeeply bound states. The behavior of the calculated width as function of the\n$\\bar K$ binding energy is studied in order to explore limits on the possible\nexistence of narrow $\\bar K$ nuclear states.",
    "arxiv_id": "nucl-th/0407063",
    "authors": [
      "J. Mares",
      "E. Friedman",
      "A. Gal"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/j.physletb.2004.11.086",
    "journal_ref": "Phys.Lett. B606 (2005) 295-302",
    "title": "Widths of $\\bar K$-nuclear deeply bound states in a dynamical model",
    "url": "https://arxiv.org/abs/nucl-th/0407063"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "6cb57bc4-8145-47c0-b910-004721927b71",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}