{
  "annotation_id": "4ef290e7-fe8a-40f3-8bf9-5ca16b78b848",
  "date_created": "2026-03-02T18:00:53.458000Z",
  "date_modified": "2026-03-02T18:00:53.458000Z",
  "file_hash": "69a22768cef85d57b52f137fa2f748f3484dead6937050b64032f337abcccba4",
  "private": false,
  "record": {
    "abstract": "When an ArF excimer laser beam was focused in a high pressure argon gas from\n50 to 130 atm, the plasma development is observed by streak camera from side\nwindow of chamber. The high pressure ArF laser plasma develops symmetrically\nand the plasma produced by ArF excimer laser hardly develops as compared with\nthe plasma produced by XeCl. The photon energy of ArF laser light is higher\nthan the XeCl laser. The transmittance of ArF laser light was measured. Almost\nall the laser light is transmitted as the frequency of laser light is higher\nthan the plasma frequency, and the energy of laser light is hardly working for\nplasma development. The backward and forward plasma development produced by the\nArF laser was calculated by the breakdown wave and the radiation supported\nshock wave, which agreed with the experimental one. The backward development\nmechanism of high pressure ArF plasma is same as one of plasma produced by XeCl\nlaser. However, the forward development mechanism of ArF plasma differs from\none of plasma produced by XeCl laser.",
    "arxiv_id": "physics/0411068",
    "authors": [
      "Norio Tsuda",
      "Jun Yamada"
    ],
    "categories": [
      "physics.plasm-ph"
    ],
    "title": "Study on high pressure plasma produced by ArF laser",
    "url": "https://arxiv.org/abs/physics/0411068"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "1fa7116d-6ef4-427d-befc-b3dd9d5b4e24",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}