{
  "annotation_id": "0571ce84-92a6-4871-bd32-09d6309c97cc",
  "date_created": "2026-03-02T18:00:14.643000Z",
  "date_modified": "2026-03-02T18:00:14.643000Z",
  "file_hash": "0dfad33e072bbe063b9a9ed426a8d557ffa6359ffa96f6f08e2c795b89a44a73",
  "private": false,
  "record": {
    "abstract": "In relativistic Hamiltonians the two-nucleon interaction is expressed as a\nsum of $\\tilde{v}_{ij}$, the interaction in the ${\\bf P}_{ij}=0$ rest frame,\nand the ``boost interaction\u0027\u0027 $\\delta v({\\bf P}_{ij})$ which depends upon the\ntotal momentum ${\\bf P}_{ij}$ and vanishes in the rest frame. The $\\delta v$\ncan be regarded as a sum of four terms: $\\delta v_{RE}$, $\\delta v_{LC}$,\n$\\delta v_{TP}$ and $\\delta v_{QM}$; the first three originate from the\nrelativistic energy-momentum relation, Lorentz contraction and Thomas\nprecession, while the last is purely quantum. The contributions of $\\delta\nv_{RE}$ and $\\delta v_{LC}$ have been previously calculated with the\nvariational Monte Carlo method for $^3$H and $^4$He. In this brief note we\nreport the results of similar calculations for the contributions of $\\delta\nv_{TP}$ and $\\delta v_{QM}$. These are found to be rather small.",
    "arxiv_id": "nucl-th/9410013",
    "authors": [
      "J. L. Forest",
      "V. R. Pandharipande",
      "J. Carlson",
      "R. Schiavilla"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.52.576",
    "title": "Variational Monte Carlo Calculations of $^3$H and $^4$He with a   relativistic Hamiltonian - II",
    "url": "https://arxiv.org/abs/nucl-th/9410013"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "66b258e2-3f11-43bc-8808-de2c3c2c7a0e",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}