{
  "annotation_id": "4dee8783-430d-4d6f-be3c-dc6a4cd086f8",
  "date_created": "2026-03-02T17:59:57.647000Z",
  "date_modified": "2026-03-02T17:59:57.647000Z",
  "file_hash": "85019f9cbff77d3ea7b37b15925ab3e76a792bc5421761f5a11e3a75cc026403",
  "private": false,
  "record": {
    "abstract": "The spectrum and wave functions of $^{44}$Ti are studied in oblique-basis\ncalculations using spherical and SU(3) shell-model states. Although the results\nfor $^{44}$Ti are not as good as those previously reported for $^{24}$Mg, due\nprimarily to the strong spin-orbit interaction that generates significant\nsplitting of the single-particle energies that breaks the SU(3) symmetry, a\nmore careful quantitative analysis shows that the oblique-basis concept is\nstill effective. In particular, a model space that includes a few SU(3)\nirreducible representations, namely, the leading irrep (12,0) and next to the\nleading irrep (10,1) including its spin S=0 and 1 states, plus spherical\nshell-model configurations (SSMC) that have at least two valence nucleons\nconfined to the $f_{7/2}$ orbit -- the SM(2) states, provide results that are\ncompatible with SSMC with at least one valence nucleon confined to the\n$f_{7/2}$ orbit -- the SM(3) states.",
    "arxiv_id": "nucl-th/0304031",
    "authors": [
      "V. G. Gueorguiev",
      "J. P. Draayer",
      "W. E. Ormand",
      "C. W. Johnson"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1142/9789812703026_0028",
    "title": "Oblique-Basis Calculations for $^{44}$Ti",
    "url": "https://arxiv.org/abs/nucl-th/0304031"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "de7d4df7-a46b-43bf-84bf-3e9eac31b044",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}