{
  "annotation_id": "7d67eced-c585-4e2f-9aea-068d2a2aaaf6",
  "date_created": "2026-03-02T18:01:49.385000Z",
  "date_modified": "2026-03-02T18:01:49.385000Z",
  "file_hash": "02f7402d917f90f4edcd6d050e1f1d9e106488eebdb79dbe1c27b831c8b7a3f9",
  "private": false,
  "record": {
    "abstract": "The Schwinger oscillator operator representation of SU(3), studied in a\nprevious paper from the representation theory point of view, is analysed to\ndiscuss the intimate relationships between standard oscillator coherent state\nsystems and systems of SU(3) coherent states. Both SU(3) standard coherent\nstates, based on choice of highest weight vector as fiducial vector, and\ncertain other specific systems of generalised coherent states, are found to be\nrelevant. A complete analysis is presented, covering all the oscillator\ncoherent states without exception, and amounting to SU(3) harmonic analysis of\nthese states.",
    "arxiv_id": "quant-ph/0204120",
    "authors": [
      "S. Chaturvedi",
      "N. Mukunda"
    ],
    "categories": [
      "quant-ph",
      "hep-th"
    ],
    "doi": "10.1063/1.1508811",
    "journal_ref": "J.Math.Phys. 43 (2002) 5278-5309",
    "title": "The Schwinger SU(3) Construction - II: Relations between Heisenberg-Weyl   and SU(3) Coherent States",
    "url": "https://arxiv.org/abs/quant-ph/0204120"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "54adf7b9-d6ce-4453-9224-c742e2436246",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}