{
  "annotation_id": "0470abd1-fc5a-43a1-8138-e65755c7e5ef",
  "date_created": "2026-03-02T18:00:39.704000Z",
  "date_modified": "2026-03-02T18:00:39.704000Z",
  "file_hash": "08f43b80e6f063fc7f3441e829be9a15f73f90d695541e4596ac48ca04d0bd50",
  "private": false,
  "record": {
    "abstract": "In this paper we overview some results on the hydrogen atom in external\nstatic uniform magnetic fields. We focus on the case of very strong magnetic\nfield, B\u003e\u003eB_0=2.3x10^9 Gauss, use various approximate models and, particularly,\nin the adiabatic approximation have calculated exactly the integral defining\nthe effective potential. This potential appears to be finite at z=0. Our\nconsideration of the problem of highly magnetized atoms and molecules is\nmotivated by the recently developed MagneGas technology by Santilli\n(http://www.magnegas.com). The ground state electron charge distribution of the\nhydrogen atom in an intense magnetic field is of a toroidal form, in agreement\nwith that studied by Santilli. This physical picture is at the foundation of\nthe new chemical species of magnecules proposed by Santilli.",
    "arxiv_id": "physics/0202049",
    "authors": [
      "A. K. Aringazin"
    ],
    "categories": [
      "physics.chem-ph",
      "physics.atm-clus"
    ],
    "journal_ref": "Hadronic J. 24 (2001) 395-434",
    "title": "Toroidal configuration of the orbit of the electron of the hydrogen atom   under strong external magnetic fields",
    "url": "https://arxiv.org/abs/physics/0202049"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "9f7184d8-6135-4f0e-b25a-30a693760d94",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}