{
  "annotation_id": "93f722da-2ba6-4af8-9888-d8d03d81817c",
  "date_created": "2026-03-02T18:00:08.537000Z",
  "date_modified": "2026-03-02T18:00:08.537000Z",
  "file_hash": "959bf4074f8a08f0009720e92939127840d6943c7f7d62a1bffe577245ec13c9",
  "private": false,
  "record": {
    "abstract": "In ultrarelativistic heavy ion collisions the produced high temperature, high\nenergy density state will cross different phases of the strongly interacting\nmatter. The original idea of quark-gluon plasma formation has been evolved and\nthe weakly interacting gaseous state of massless partons has been replaced by\nthe picture of strongly interacting massive constituent quarks. Experimental\nresults at SPS and RHIC supports this idea. We discuss the phases at LHC\nenergies.",
    "arxiv_id": "nucl-th/0601023",
    "authors": [
      "P. Levai"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1063/1.2140660",
    "journal_ref": "AIP Conf. Proc. 802:242-245,2005",
    "title": "The phases of strongly interacting matter in heavy ion collisions",
    "url": "https://arxiv.org/abs/nucl-th/0601023"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "83b15728-7aa6-4adc-bd32-44e0f9e6654e",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}