{
  "annotation_id": "73c5178b-b114-448c-9f7d-7416a4b1394f",
  "date_created": "2026-03-02T18:01:07.935000Z",
  "date_modified": "2026-03-02T18:01:07.935000Z",
  "file_hash": "32c196733c6e27c73ed2678bb0146b31ef8ad0739f575df30d88f2adf8b64133",
  "private": false,
  "record": {
    "abstract": "The ILC baseline consists of two interaction regions, one with a 20mrad\ncrossing angle and the other with a 2mrad crossing angle. It is known that the\noutgoing beam losses in the final doublet and subsequent extraction line are\nlarger in the 2mrad than in the 20mrad layout. In this work, we exploit NbTi\nand Nb$_3$Sn superconducting magnet technologies to redesign and optimise the\nfinal doublet, with the aim of providing satisfactory outgoing disrupted beam\npower losses in this region. We present three new final doublet layouts,\nspecifically optimised for the 500 GeV and the 1 TeV machines.",
    "arxiv_id": "physics/0606022",
    "authors": [
      "R. Appleby",
      "P. Bambade"
    ],
    "categories": [
      "physics.acc-ph"
    ],
    "doi": "10.1088/1748-0221/1/10/P10005",
    "journal_ref": "JINST1:P10005,2006",
    "title": "Improved final doublet designs for the ILC baseline small crossing angle   scheme",
    "url": "https://arxiv.org/abs/physics/0606022"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ed3ee669-f01a-4a6a-a8ab-b65c50633621",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}