{
  "id": "1810.04382",
  "version": "v1",
  "published": "2018-10-10T06:23:13.000Z",
  "updated": "2018-10-10T06:23:13.000Z",
  "title": "$Ωd$ bound state",
  "authors": [
    "H. Garcilazo",
    "A. Valcarce"
  ],
  "comment": "5 pages",
  "journal": "Phys.Rev. C98 (2018) no.2, 024002",
  "doi": "10.1103/PhysRevC.98.024002",
  "categories": [
    "nucl-th",
    "hep-ph"
  ],
  "abstract": "The lattice QCD analyses of the HAL QCD Collaboration predicts a strongly attractive potential in the $\\Omega N$ $^5S_2$ channel which supports a bound state. In this paper we show that this $\\Omega N$ channel together with the $NN$ $^3S_1$ channel give rise to a $\\Omega d$ bound state in the state with maximal spin $(I,J^P)=(0,5/2^+)$ with a binding energy of $\\sim$ 17 MeV.",
  "revisions": [
    {
      "version": "v1",
      "updated": "2018-10-10T06:23:13.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "bound state",
      "hal qcd collaboration predicts",
      "lattice qcd analyses",
      "maximal spin",
      "strongly attractive potential"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Phys. Rev. C"
    },
    "note": {
      "typesetting": "TeX",
      "pages": 5,
      "language": "en",
      "license": "arXiv",
      "status": "editable"
    }
  }
}