{
  "annotation_id": "ae92b60d-8d30-485a-b8a6-9a6f8ec9110d",
  "date_created": "2026-03-02T18:01:42.011000Z",
  "date_modified": "2026-03-02T18:01:42.011000Z",
  "file_hash": "4804e95ee094ea3fa0df382c9ce8688de782cfebb109afe855303f1b1bfa1702",
  "private": false,
  "record": {
    "abstract": "We define coherent states for SU(3) using six bosonic creation and\nannihilation operators. These coherent states are explicitly characterized by\nsix complex numbers with constraints. For the completely symmetric\nrepresentations (n,0) and (0,m), only three of the bosonic operators are\nrequired. For mixed representations (n,m), all six operators are required. The\ncoherent states provide a resolution of identity, satisfy the continuity\nproperty, and possess a variety of group theoretic properties. We introduce an\nexplicit parameterization of the group SU(3) and the corresponding integration\nmeasure. Finally, we discuss the path integral formalism for a problem in which\nthe Hamiltonian is a function of SU(3) operators at each site.",
    "arxiv_id": "quant-ph/0012099",
    "authors": [
      "Manu Mathur",
      "Diptiman Sen"
    ],
    "categories": [
      "quant-ph",
      "cond-mat",
      "hep-th"
    ],
    "doi": "10.1063/1.1385563",
    "journal_ref": "J.Math.Phys. 42 (2001) 4181-4196",
    "title": "Coherent States For SU(3)",
    "url": "https://arxiv.org/abs/quant-ph/0012099"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "acef6521-bcc1-451c-9568-d1601f4f70f5",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}