{
  "annotation_id": "6ede0185-4fd4-4e45-a2ed-00ad7e3fbca6",
  "date_created": "2026-03-02T18:02:40.982000Z",
  "date_modified": "2026-03-02T18:02:40.982000Z",
  "file_hash": "23531f83a4249b1550d91b34f9e7b281d95647a0ce3e5d385ca4c179660576cb",
  "private": false,
  "record": {
    "abstract": "We continue our investigation concerning the question of whether atomic bound\nstates begin to stabilize in the ultra-intense field limit. The pulses\nconsidered are essentially arbitrary, but we distinguish between three\nsituations. First the total classical momentum transfer is non-vanishing,\nsecond not both the total classical momentum transfer and the total classical\ndisplacement are vanishing together with the requirement that the potential has\na finite number of bound states and third both the total classical momentum\ntransfer and the total classical displacement are vanishing. For the first two\ncases we rigorously prove, that the ionization probability tends to one when\nthe amplitude of the pulse tends to infinity and the pulse shape remains fixed.\nIn the third case the limit is strictly smaller than one. This case is also\nrelated to the high frequency limit considered by Gavrila et al.",
    "arxiv_id": "quant-ph/9707059",
    "authors": [
      "A. Fring",
      "V. Kostrykin",
      "R. Schrader"
    ],
    "categories": [
      "quant-ph",
      "physics.atom-ph"
    ],
    "doi": "10.1088/0305-4470/30/24/020",
    "journal_ref": "J.Phys.A30:8599-8610,1997",
    "title": "Ionization Probabilities through ultra-intense Fields in the extreme   Limit",
    "url": "https://arxiv.org/abs/quant-ph/9707059"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "64021670-ae25-4c26-9150-e88118ec1ead",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}