{
  "annotation_id": "56aa40e9-1d13-4e3f-88fa-dc31b08eba2f",
  "date_created": "2026-03-02T18:01:56.060000Z",
  "date_modified": "2026-03-02T18:01:56.060000Z",
  "file_hash": "8e1fd9354a9c7c552fb33f5e8d6879e816390e2400b5dafa17360db285dd7566",
  "private": false,
  "record": {
    "abstract": "A general procedure for constructing coherent states, which are eigenstates\nof annihilation operators, related to quantum mechanical potential problems, is\npresented. These coherent states, by construction are not potential specific\nand rely on the properties of the orthogonal polynomials, for their derivation.\nThe information about a given quantum mechanical potential enters into these\nstates, through the orthogonal polynomials associated with it and also through\nits ground state wave function. The time evolution of some of these states\nexhibit fractional revivals, having relevance to the factorization problem.",
    "arxiv_id": "quant-ph/0302171",
    "authors": [
      "P. K. Panigrahi",
      "T. Shreecharan",
      "J. Banerji",
      "V. Sundaram"
    ],
    "categories": [
      "quant-ph"
    ],
    "title": "Coherent States: A General Approach",
    "url": "https://arxiv.org/abs/quant-ph/0302171"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "56129116-2de9-4957-b497-dafd273b1b6c",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}