{
  "annotation_id": "5a1acbb7-66c2-4069-8d77-d1b405ed44e4",
  "date_created": "2026-03-02T18:00:03.740000Z",
  "date_modified": "2026-03-02T18:00:03.740000Z",
  "file_hash": "96101776b6cfc5868610ba02115832bd97d2b0c82e469023faed357c74b0028e",
  "private": false,
  "record": {
    "abstract": "Strangeness canonical ensemble for Maxwell-Boltzmann statistics is\nreconsidered for excited nuclear systems with non-vanishing net strangeness. A\nnew recurrence relation method is applied to find the partition function. The\nmethod is first generalized to the case of quantum strangeness canonical\nensemble. Uncertainties in calculation of the K+/pi+ excitation function are\ndiscussed. A new scenario based on the strangeness distillation effect is put\nforward for a possible explanation of anomalous strangeness production observed\nat the bombarding energy near 30 AGeV. The peaked maximum in the K+/pi+ ratio\nis considered as a sign of the critical end-point reached in evolution of the\nsystem rather than a latent heat jump emerging from the onset of the first\norder deconfinement phase transition.",
    "arxiv_id": "nucl-th/0411125",
    "authors": [
      "V. D. Toneev",
      "A. S. Parvan"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1088/0954-3899/31/7/005",
    "journal_ref": "J.Phys. G31 (2005) 583-598",
    "title": "Canonical Strangeness and Distillation Effects in Hadron Production",
    "url": "https://arxiv.org/abs/nucl-th/0411125"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "bd8ddbfc-5f82-4a3d-b050-23a9e4eb0220",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}