{
  "annotation_id": "6c180ec0-c154-4fad-9bc0-088a69ec0b8c",
  "date_created": "2026-03-02T18:00:01.594000Z",
  "date_modified": "2026-03-02T18:00:01.594000Z",
  "file_hash": "0fe3197d03737ecf1ec7e902bea96becc383cf8d7c321b30ec4aa70ee10aaeb1",
  "private": false,
  "record": {
    "abstract": "A variational Monte Carlo method is used to generate sets of orthogonal trial\nfunctions, Psi_T(J^pi,T), for given quantum numbers in various light p-shell\nnuclei. These Psi_T are then used as input to Green\u0027s function Monte Carlo\ncalculations of first, second, and higher excited (J^pi,T) states. Realistic\ntwo- and three-nucleon interactions are used. We find that if the physical\nexcited state is reasonably narrow, the GFMC energy converges to a stable\nresult. With the combined Argonne v_18 two-nucleon and Illinois-2 three-nucleon\ninteractions, the results for many second and higher states in A = 6--8 nuclei\nare close to the experimental values.",
    "arxiv_id": "nucl-th/0409012",
    "authors": [
      "Steven C. Pieper",
      "R. B. Wiringa",
      "J. Carlson"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.70.054325",
    "journal_ref": "Phys.Rev.C70:054325,2004",
    "title": "Quantum Monte Carlo calculations of excited states in A = 6--8 nuclei",
    "url": "https://arxiv.org/abs/nucl-th/0409012"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "08e82fde-2afe-464b-8a39-ed5a4a8a5f43",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}