{
  "annotation_id": "ec150ea2-6c59-471e-8637-979f129538c7",
  "date_created": "2026-03-02T18:01:00.638000Z",
  "date_modified": "2026-03-02T18:01:00.638000Z",
  "file_hash": "ad9de5e70c51b818a625a55620cc43a8ad24236f1ccb224366d29a5ab22e95ea",
  "private": false,
  "record": {
    "abstract": "Under certain conditions, a transparent photonic band can be designed into a\none-dimensional metallodielectric nanofilm structure. Unlike conventional pass\nbands in photonic crystals, where the finite thickness of the structure affects\nthe transmission of electromagnetic fields having frequency within the pass\nband, the properties of the transparent band are almost unaffected by the\nfinite thickness of the structure. In other words, an incident field at a\nfrequency within the transparent band exhibits 100% transmission independent of\nthe number of periods of the structure. The transparent photonic band\ncorresponds to excitation of pure eigenstate modes across the entire Bloch band\nin structures possessing mirror symmetry. The conditions to create these modes\nand thereby to lead to a totally transparent band phenomenon are discussed.",
    "arxiv_id": "physics/0507155",
    "authors": [
      "Simin Feng",
      "J. Merle Elson",
      "Pamela L. Overfelt"
    ],
    "categories": [
      "physics.optics"
    ],
    "doi": "10.1103/PhysRevB.72.085117",
    "journal_ref": "Phys. Rev. B, v.72, p.085117 (2005)",
    "title": "Transparent photonic band in metallodielectric nanostructures",
    "url": "https://arxiv.org/abs/physics/0507155"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "93e8956b-dee4-48c3-a8bb-2ef8b6b21a27",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}