{
  "annotation_id": "66138519-b8e2-42bf-973d-487adcbbe148",
  "date_created": "2026-03-02T18:00:19.146000Z",
  "date_modified": "2026-03-02T18:00:19.146000Z",
  "file_hash": "647d9af40da77f3a44286f72a26938b2409bae48954eb010f813fc9dc97f7dfa",
  "private": false,
  "record": {
    "abstract": "A cranked mean-field model with two-body T=1 and T=0 pairing interactions is\npresented. Approximate projection onto good particle-number is enforced via an\nextended Lipkin-Nogami scheme. Our calculations suggest the simultaneous\npresence of both T=0 and T=1 pairing modes in N=Z nuclei. The transitions\nbetween different pairing phases are discussed as a function of neutron/proton\nexcess, T$_z$, and rotational frequency, $\\hbar\\omega$. The additional binding\nenergy due to the T=0 $np$-pairing correlations, is suggested as a possible\nmicroscopic explanation of the Wigner energy term in even-even nuclei.",
    "arxiv_id": "nucl-th/9608041",
    "authors": [
      "W. Satu\u0142a",
      "R. Wyss"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0370-2693(96)01603-6",
    "journal_ref": "Phys.Lett. B393 (1997) 1-6",
    "title": "Competition Between T=0 and T=1 Pairing in Proton-Rich Nuclei",
    "url": "https://arxiv.org/abs/nucl-th/9608041"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "4f7c6977-2448-4168-b364-e698e05acfdb",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}