{
  "annotation_id": "9a151fd9-53a5-4014-b748-27b6b6dde7ba",
  "date_created": "2026-03-02T18:00:39.437000Z",
  "date_modified": "2026-03-02T18:00:39.437000Z",
  "file_hash": "ad677701db942976d0439173de8d95a2039ae6e60050d292ad1882a05762e050",
  "private": false,
  "record": {
    "abstract": "As known, any numerical simulation is composed of two parts: (1) the initial\npart of writing the relevant code and (2) the running of this code on the\ncomputer screen. The second part of running the program is extensively\ndiscussed theoretically and technically in the relevant literature. In this\nwork we pay special attention to the less discussed first part and show that it\nmay be discussed in a terminology and notation which describe physical\nphenomena. As examples we discuss the two cases of simulating (1) the harmonic\noscillator and (2) the electron-photon interaction which results in the known\nLamb shift.",
    "arxiv_id": "physics/0205010",
    "authors": [
      "D. Bar"
    ],
    "categories": [
      "physics.data-an"
    ],
    "title": "Computer simulations discussed in physical terms and terminology",
    "url": "https://arxiv.org/abs/physics/0205010"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "5bcf5c84-1664-4831-8e8d-9fbd95fc9ca3",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}