{
  "annotation_id": "f7f40199-f200-4ea8-805f-1e5f5510d081",
  "date_created": "2026-03-02T18:00:56.863000Z",
  "date_modified": "2026-03-02T18:00:56.863000Z",
  "file_hash": "5b2cd552d6eebfb3528d09670df6473e04203d411bd974e980dd05da0b4c7d4a",
  "private": false,
  "record": {
    "abstract": "The bunch-by-bunch BPM signal array has to be reshaped into a turn-by-turn\n(TBT) matrix in order to make the TBT beam position information of a single\nbunch available for further data analysis, such as via the Fourier transform to\nobtain the synchrotron tune and betatron tune, etc. Since the RF frequency\nsweeps more than 10 MHz in the first 8 ms of a Booster cycle, the revolution\ntime decreases more than 20%. The number of data points for each Booster turn\n(BT) should be varied in the same pace with the revolution time since the\nsampling rate of a digital oscilloscope is usually fixed. And this can be done\nby pre-determining the relationship between the RF frequency and the time in a\ncycle via the curve fit.",
    "arxiv_id": "physics/0501026",
    "authors": [
      "Xi Yang",
      "Charles M. Ankenbrandt",
      "James Lackey",
      "Vic Scarpine"
    ],
    "categories": [
      "physics.acc-ph"
    ],
    "title": "Reshape of the Bunch-by-bunch BPM Signal to a Turn-by-turn Matrix during   the Fast RF Frequency-sweeping Time in Booster",
    "url": "https://arxiv.org/abs/physics/0501026"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "a9ca12c6-8e26-4af8-9ee2-47d24caf537c",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}