{
  "annotation_id": "d783a2ad-13c6-42c9-8c9a-c3c72e1be9dc",
  "date_created": "2026-03-02T18:00:22.103000Z",
  "date_modified": "2026-03-02T18:00:22.103000Z",
  "file_hash": "502845c86a0d01434a7edf83d05effd308cf377274e480a5812e6b339c30bbba",
  "private": false,
  "record": {
    "abstract": "A recent development on the working of effective field theories in nuclei and\nin dense hadronic matter is discussed. We consider two extreme regimes: One,\ndilute regime for which fluctuations are made on top of the matter-free vacuum;\ntwo, dense systems for which fluctuations are treated on top of the \"vacuum\"\ndefined at a given density, with masses and coupling constants varying as\nfunction of matter density (\"Brown-Rho scaling\"). Based on an intricate -- as\nyet mostly conjectural -- connection between the in-medium structure of chiral\nLagrangian field theory which is a beautiful effective theory of QCD and that\nof Landau Fermi liquid theory which is an equally beautiful and highly\nsuccessful effective theory of many-body systems, it is suggested that a chiral\nLagrangian with Brown-Rho scaling in the mean field is equivalent to\nFermi-liquid fixed point theory. I make this connection using electroweak and\nstrong responses of nuclear matter up to nuclear matter density and then\nextrapolating to higher densities encountered in heavy-ion collisions and\ncompact stars.",
    "arxiv_id": "nucl-th/9806029",
    "authors": [
      "Mannque Rho"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "journal_ref": "Acta Phys.Polon. B29 (1998) 2297-2308",
    "title": "Effective Field Theories For Nuclei And Dense Matter",
    "url": "https://arxiv.org/abs/nucl-th/9806029"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "60df012a-3193-42ee-be43-f9626992f39b",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}