{
  "annotation_id": "e0913fda-3332-47d5-ab71-c99d2c2449cf",
  "date_created": "2026-03-02T18:00:00.605000Z",
  "date_modified": "2026-03-02T18:00:00.605000Z",
  "file_hash": "55f87943fa81564d318afa62262881e7c5aee8ea77bf656998642ef3149de334",
  "private": false,
  "record": {
    "abstract": "We discuss the relation between the effective vector meson mass and equation\nof state (EOS) for nuclear matter. In the mean field approximation, the EOS\nbecomes softer due to the reduction of the effective omega-meson mass, if we\nassume that the omega-meson mean field is proportional to the baryon density.\nWe examine the assumption by using the auxiliary field method at finite\ntemperature and /or density.",
    "arxiv_id": "nucl-th/0410025",
    "authors": [
      "Hiroaki Kouno"
    ],
    "categories": [
      "nucl-th"
    ],
    "journal_ref": "Soryushiron Kenkyu (Kyoto) 110 (2005), E84-E86",
    "title": "Auxiliary field method at finite temperature and/or finite density",
    "url": "https://arxiv.org/abs/nucl-th/0410025"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "c9f648c8-420b-4aa5-97b8-8f90306bf391",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}