{
  "annotation_id": "c155e374-1d03-4233-9465-196e862bfe9e",
  "date_created": "2026-03-02T18:00:08.068000Z",
  "date_modified": "2026-03-02T18:00:08.068000Z",
  "file_hash": "9e808ee7251016560e67948fe180c304fba19dc94578cdea7ee3a46a0de82c14",
  "private": false,
  "record": {
    "abstract": "In this paper, we report a systematic study of the heaviest nuclei within the\nrelativistic mean field (RMF) model. By comparing our results with those of the\nHartree-Fock-Bogoliubov method (HFB) and the finite range droplet model (FRDM),\nthe stability and the shape of the heaviest nuclei are discussed. The\ntheoretical predictions as well as the existing experimental data indicate that\nthe experimentally synthesized superheavy nuclei are in between the fission\nstability line, the line connecting the nucleus with maximum binding energy per\nnucleon in each isotopic chain, and the $\\beta$-stability line, the line\nconnecting the nucleus with maximum binding energy per nucleon in each isobaric\nchain. It is shown that both the fission stability line and the\n$\\beta$-stability line tend to be more proton rich in the superheavy region.\nMeanwhile, all the three theoretical models predict most synthesized superheavy\nnuclei to be deformed.",
    "arxiv_id": "nucl-th/0602030",
    "authors": [
      "L. S. Geng",
      "H. Toki",
      "E. G. Zhao"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1088/0954-3899/32/4/013",
    "journal_ref": "J.Phys. G32 (2006) 573-582",
    "title": "The stability and the shape of the heaviest nuclei",
    "url": "https://arxiv.org/abs/nucl-th/0602030"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "4f4fc989-acd6-4a01-b782-b6ddedc825b4",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}