{
  "annotation_id": "b0dc57fd-86c4-4a66-8540-8e7f9d848b0d",
  "date_created": "2026-03-02T18:00:04.210000Z",
  "date_modified": "2026-03-02T18:00:04.210000Z",
  "file_hash": "2d66e98d8052898be192780139691955f448cb0a22d9fd241005b9102f4e1df8",
  "private": false,
  "record": {
    "abstract": "The effects of the finite size of a liquid drop undergoing a phase transition\nare described in terms of the complement, the largest (but still mesoscopic)\ndrop representing the liquid in equilibrium with the vapor. Vapor cluster\nconcentrations, pressure and density from fixed mean density lattice gas\n(Ising) model calculations are explained in terms of the complement. Accounting\nfor this finite size effect is key to determining the infinite nuclear matter\nphase diagram from experimental data.",
    "arxiv_id": "nucl-th/0412070",
    "authors": [
      "L. G. Moretto",
      "K. A. Bugaev",
      "J. B. Elliott",
      "R. Ghetti",
      "J. Helgesson",
      "L. Phair"
    ],
    "categories": [
      "nucl-th",
      "cond-mat.stat-mech"
    ],
    "doi": "10.1103/PhysRevLett.94.202701",
    "journal_ref": "Phys.Rev.Lett. 94 (2005) 202701",
    "title": "The complement: a solution to liquid drop finite size effects in phase   transitions",
    "url": "https://arxiv.org/abs/nucl-th/0412070"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "93a99d4f-8a25-45cf-a2ca-68925893956a",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}