{
  "annotation_id": "ac7a774d-ad35-40f6-85de-dbeffbabbd73",
  "date_created": "2026-03-02T18:00:15.538000Z",
  "date_modified": "2026-03-02T18:00:15.538000Z",
  "file_hash": "2759bb57204ae8cf281fa3df8d794d321985cc463088fa2bf5e7878948f50e68",
  "private": false,
  "record": {
    "abstract": "In shell model calculations for the yrast even spin states of 50Cr, the\nstatic quadrupole moments of the low spin states 2+_1 and 4+_1 are negative but\nthose of the high spin states 10+_1, 12+_1 and 14+_1 are positive. Even spin\nstates beyond the single j shell limit, J_max=14, again have negative moments.\nWhile the B(E2)\u0027s for the J -\u003e J-2 transitions are strongest along the yrast\npath for J \u003c= 8, it is found that the transition from the second J=10 state to\nthe first J=8 state (10+_2 -\u003e 8+_1) is much stronger than the 10+_1 -\u003e 8+_1\ntransition. We also note that while the 16+_1 -\u003e 14+_1 transition is weak, the\n16+_1 -\u003e 14+_2 is quite strong.",
    "arxiv_id": "nucl-th/9507012",
    "authors": [
      "L. Zamick",
      "M. Fayache",
      "D. C. Zheng"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.53.188",
    "title": "Change of shape in the yrast sequence in 50Cr",
    "url": "https://arxiv.org/abs/nucl-th/9507012"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "49571d89-6411-4a09-a0f0-5b289124163e",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}