{
  "annotation_id": "079b76be-0e1c-4e31-bec9-a07f46c33cdf",
  "date_created": "2026-03-02T18:01:35.736000Z",
  "date_modified": "2026-03-02T18:01:35.736000Z",
  "file_hash": "6d9f9388722713f4e017150233b7540433809e2c9d647abaf87c29b34fb18dda",
  "private": false,
  "record": {
    "abstract": "The physical model (PhsMdl) of a Schrodinger nonrelativistic quantized\nelectron (ShEl) is built by means of a transition of the quadratic differential\nparticle equation of Hamilton-Jacoby into the quadratic differential wave\nequation of Schrodinger in this work, which interprets the physical reason of\nits quantum (wave and stochastic) behaviour by explanation of the physical\nreason, which forces the classical Lorentz electron (LrEl) to participate in\nFurthian quantized stochastic oscillation motion, which turn it into quantum\nShEl. It is performed that this transition is realized by my consideration the\nBohm\u0027s quantum potential as a kinetic energy of the forced Furthian quantized\nstochastic oscillation motion of the ShEl\u0027s well spread elementary electric\ncharge close to a smooth thin trajectory of a classical LrEl. There exist as an\nessential analogy between the Furthian quantum stochastic trembling oscillation\nmotion and the Brownian classical stochastic trembling motion so and between\nthe description of their behaviours.",
    "arxiv_id": "quant-ph/0001079",
    "authors": [
      "Josiph Mladenov Rangelov"
    ],
    "categories": [
      "quant-ph"
    ],
    "title": "The Physical Model of Schrodinger Electron. Schrodinger Convenient Way   for Description of its Quantum Behaviour",
    "url": "https://arxiv.org/abs/quant-ph/0001079"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "437dddd4-d397-405a-844e-8f4f21618ee7",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}