{
  "annotation_id": "a31acaef-10a3-41a0-8ec5-ed78c2f100f8",
  "date_created": "2026-03-02T18:00:08.656000Z",
  "date_modified": "2026-03-02T18:00:08.656000Z",
  "file_hash": "4055349d5c0f127b17bf71906c9c8dfebe28545fad69c61de3daf6d15567066a",
  "private": false,
  "record": {
    "abstract": "We report on the first genuinely three-body ${\\bar K}NN - \\pi \\Sigma N$\ncoupled-channel Faddeev calculation in search for quasi-bound states in the\n$K^- p p$ system. The main absorptivity in the $K^- p$ subsystem is accounted\nfor by fitting to $K^- p$ data near threshold. Our calculation yields one such\nquasi-bound state, with $I=1/2$, $J^{\\pi}=0^-$, bound in the range $B \\sim\n55-70$ MeV, with a width of $\\Gamma \\sim 95-110$ MeV. These results differ\nsubstantially from previous estimates, and are at odds with the $K^- p p \\to\n\\Lambda p$ signal observed by the FINUDA collaboration.",
    "arxiv_id": "nucl-th/0610022",
    "authors": [
      "N. V. Shevchenko",
      "A. Gal",
      "J. Mares"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevLett.98.082301",
    "journal_ref": "Phys.Rev.Lett.98:082301,2007",
    "title": "Faddeev calculation of a $K^- p p$ quasi-bound state",
    "url": "https://arxiv.org/abs/nucl-th/0610022"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "3438b968-fed0-4980-ba71-9995eab7bb5b",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}