{
  "annotation_id": "822ccdb6-c123-46a0-93d2-0f9a4597e186",
  "date_created": "2026-03-02T18:00:32.366000Z",
  "date_modified": "2026-03-02T18:00:32.366000Z",
  "file_hash": "37b7743e1a648db0f42c73b1dd13c1685db3d28755a8ff71de4c557a7e0b74a5",
  "private": false,
  "record": {
    "abstract": "The SNS linac accelerates an average beam current of 2 mA to an energy of 968\nMeV. The linac is pulsed at 60 Hz with an H- beam pulse of 1 ms. The first 185\nMev of the linac uses normal conducting cavities, and the remaining length of\nthe linac uses superconducting cavities. The linac operates at 402.5 MHz up to\n87 MeV and then changes to 805 MHz for the remainder. This paper gives an\noverview of the Linac RF system. The overview includes a description and\nconfiguration of the high power RF components, the HV converter/modulator, and\nthe RF controls. Issues and tradeoffs in the RF system will be discussed,\nespecially with regards to the use of pulsed superconducting cavities.",
    "arxiv_id": "physics/0008070",
    "authors": [
      "Michael Lynch",
      "William Reass",
      "Daniel Rees",
      "Amy Regan",
      "Paul Tallerico"
    ],
    "categories": [
      "physics.acc-ph"
    ],
    "journal_ref": "eConf C000821 (2000) THE01",
    "title": "The Spallation Neutron Source (SNS) Linac RF System",
    "url": "https://arxiv.org/abs/physics/0008070"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "728f5b83-9171-4832-9d25-6a74f278cfc9",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}