{
  "annotation_id": "d0b31780-fe71-437a-a72b-f672cf70d0b3",
  "date_created": "2026-03-02T18:01:14.522000Z",
  "date_modified": "2026-03-02T18:01:14.522000Z",
  "file_hash": "dcef9c246de98358cedb71c4c2500752464d78b6bd530997e998793527b521da",
  "private": false,
  "record": {
    "abstract": "In this paper the scaling law for the relaxation times in thermal phenomena\nis investigated. It is shown that dependent on the value of the parameter\nK=E/m(c\\alpha)^2,where E is the energy which is delivered to the system, m is\nthe parton mass and \\alpha=1/137 for electromagnetic interaction and\n\\alpha=0.16 for strong interaction respectively, heat transport is diffusive,\nfor K\u003c1, or contains the wave component for K\u003e1. For the system with N partons\nthe relaxation time is scaled as \\tau^N\\to N (\\hbar/(mc\\alpha)^2).\n  Key words: Thermal phenomena, scaling",
    "arxiv_id": "physics/0610267",
    "authors": [
      "M. Kozlowski",
      "J. Marciak-Kozlowska"
    ],
    "categories": [
      "physics.gen-ph"
    ],
    "title": "Scaling law in thermal phenomena",
    "url": "https://arxiv.org/abs/physics/0610267"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "15c03202-1a8a-4312-a187-6694efcfb49c",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}