{
  "annotation_id": "421c9851-2a3f-485b-91df-7ea4335ba8d2",
  "date_created": "2026-03-02T18:00:49.853000Z",
  "date_modified": "2026-03-02T18:00:49.853000Z",
  "file_hash": "2302dcb7acf98164d551ed0d68eec99a4b1dc19b36a9bce707b0abde287519ed",
  "private": false,
  "record": {
    "abstract": "In this paper it is shown how one can use Bessel beams to obtain a stationary\nlocalized wavefield with high transverse localization, and whose longitudinal\nintensity pattern can assume any desired shape within a chosen interval 0 \u003c z \u003c\nL of the propagation axis. This intensity envelope remains static, i.e., with\nvelocity v=0; and because of this we call \"Frozen Waves\" such news solutions to\nthe wave equations (and, in particular, to the Maxwell equations). These\nsolutions can be used in many different and interesting applications, as\noptical tweezers, atom guides, optical or acoustic bistouries, various\nimportant medical purposes, etc.",
    "arxiv_id": "physics/0407128",
    "authors": [
      "M. Zamboni-Rached"
    ],
    "categories": [
      "physics.class-ph",
      "physics.optics"
    ],
    "doi": "10.1364/OPEX.12.004001",
    "title": "Frozen Waves: Stationary optical wavefields with arbitrary longitudinal   shape, by superposing equal-frequency Bessel beams",
    "url": "https://arxiv.org/abs/physics/0407128"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "5cd8c8c2-e254-4ec2-bc31-b3af53dd1106",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}