{
  "annotation_id": "f3e53238-6505-4e47-9b5c-4d4c97daa6e1",
  "date_created": "2026-03-02T18:01:24.168000Z",
  "date_modified": "2026-03-02T18:01:24.168000Z",
  "file_hash": "46e13e3f431946f48d4f5bf66691eefcc0b02326a0c3c3718afead6aa48588d4",
  "private": false,
  "record": {
    "abstract": "The standard ohmic measurements by means of two extra leads contain an\nadditional thermal correction to resistance. The current results in\nheating(cooling) at first(second) sample contact due to Peltier effect. The\ncontacts temperatures are different. The measured voltage is the sum of the\nohmic voltage swing and Peltier effect induced thermopower which is linear on\ncurrent. As a result, the thermal correction to resistance measured exists at\n$I\\to 0$. The correction should be in comparison with ohmic resistance. Above\nsome critical frequency dependent on thermal inertial effects the thermal\ncorrection disappears.",
    "arxiv_id": "physics/9908060",
    "authors": [
      "M. V. Cheremisin"
    ],
    "categories": [
      "physics.class-ph",
      "cond-mat",
      "physics.gen-ph"
    ],
    "doi": "10.1134/1.1354694",
    "journal_ref": "Sov. Phys. JETP, 92, 357-360, 2001",
    "title": "Ohm\u0027s law revision",
    "url": "https://arxiv.org/abs/physics/9908060"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "13a1d8f5-b776-4dcf-8af4-b41e01a44175",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}