{
  "annotation_id": "3b3cadc0-0d00-4885-977c-5b6a74fe3670",
  "date_created": "2026-03-02T18:02:47.315000Z",
  "date_modified": "2026-03-02T18:02:47.315000Z",
  "file_hash": "ac5b1abf32db3b75f09f4fd83832225a0236cc0d1e02558ec4cf180f2a1bfc69",
  "private": false,
  "record": {
    "abstract": "The formalism of quantum mechanics is presented in a way that its\ninterpretation as a classical field theory is emphasized. Two coupled real\nfields are defined with given equations of motion. Densities and currents\nassociated to the fields are found with their corresponding conserved\nquantities. The behavior of these quantities under a galilean transformation\nsuggest the association of the fields with a quantum mechanical free particle.\nAn external potential is introduced in the Lagrange formalism. The description\nis equivalent to the conventional Schr\\\"odinger equation treatment of a\nparticle. We discuss the attempts to build an interpretation of quantum\nmechanics based on this scheme. The fields become the primary onthology of the\ntheory and the particles appear as emergent properties of the fields. These\ninterpretations face serious problems for systems with many degrees of freedom.",
    "arxiv_id": "quant-ph/9905032",
    "authors": [
      "A. C. de la Torre",
      "A. Daleo"
    ],
    "categories": [
      "quant-ph"
    ],
    "title": "Quantum Mechanics as a Classical Field Theory",
    "url": "https://arxiv.org/abs/quant-ph/9905032"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "776c53db-d93c-4038-8fb0-f7e628ec80b0",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}