{
  "annotation_id": "2c0aeb6f-2e55-41f2-95f6-f2095fc7c36d",
  "date_created": "2026-03-02T18:00:04.285000Z",
  "date_modified": "2026-03-02T18:00:04.285000Z",
  "file_hash": "40f65041940f5f8395ff098f964ceed5e218322cab0e8e72e22df22129766f79",
  "private": false,
  "record": {
    "abstract": "A system H with a Hagedorn-like mass spectrum imparts its unique temperature\nTH to any other system coupled to it. An H system radiates particles in\npreexisting physical and chemical equilibrium. These particles form a saturated\nvapor at temperature TH. This coexistence describes a first order phase\ntransition. An H system is nearly indifferent to fragmentation into smaller H\nsystems. A lower mass cut-off in the spectrum does not significantly alter the\ngeneral picture",
    "arxiv_id": "nucl-th/0504010",
    "authors": [
      "L. G. Moretto",
      "K. A. Bugaev",
      "J. B. Elliott",
      "L. Phair"
    ],
    "categories": [
      "nucl-th",
      "cond-mat.stat-mech",
      "hep-ph",
      "nucl-ex"
    ],
    "doi": "10.1209/epl/i2006-10280-8",
    "journal_ref": "Europhys.Lett. 76 (2006) 402-408",
    "title": "The Hagedorn thermostat",
    "url": "https://arxiv.org/abs/nucl-th/0504010"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "c1eca58f-5328-4629-b1ab-300db812f82d",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}