{
  "annotation_id": "48f9ac97-77da-4aca-8519-25408f31a9c5",
  "date_created": "2026-03-02T18:00:46.658000Z",
  "date_modified": "2026-03-02T18:00:46.658000Z",
  "file_hash": "c5d4be1d803ad9bf036e028ddccdf271f88add297e2ee20fae0a3bba576e0c1a",
  "private": false,
  "record": {
    "abstract": "It is commonly believed that ($\\alpha$-d) and (${^3}He$ - ${^3}H$) represent\nequivalent states of ${^6}Li$. It is shown here that this is not correct. These\ntwo are actually orthogonal to each other. It is shown here that these two with\nvery different shapes and forms actually co-exist for the ground state of\n${^6}Li$. This shape co-existence is the same as similar phenomenon in heavy\nnuclei. The puzzling anomaly of extremely small branching ratio for beta\ndelayed deuteron emission in ${^6}He$ is explained here. In addition the\nanomalously large branching ratio for beta delayed triton emission in ${^8}He$\nis explained. The cluster structure of the ground state and of the low-lying\nstates of ${^6}He$, ${^6}Li$ and ${^6}Be$ is clarified.",
    "arxiv_id": "physics/0306186",
    "authors": [
      "Afsar Abbas"
    ],
    "categories": [
      "physics.gen-ph"
    ],
    "doi": "10.1142/S0217732304014926",
    "journal_ref": "Mod Phys Letts, A 19, (No.31) (2004), 2365-2370",
    "title": "Structure of A=6 Nuclei: ${^6}He$, ${^6}Li$ and ${^6}Be$",
    "url": "https://arxiv.org/abs/physics/0306186"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "c7873ccf-9e7e-4ad2-b66c-6efcd18b47cb",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}