{
  "id": "nucl-th/0104049",
  "version": "v2",
  "published": "2001-04-13T14:57:37.000Z",
  "updated": "2001-08-23T13:51:17.000Z",
  "title": "Microscopic optical potentials for nucleon-nucleus scattering",
  "authors": [
    "S. Karataglidis",
    "M. B. Chadwick"
  ],
  "comment": "17 pages, 2 tables, 7 figures, replaced with version accepted for publication in Phys. Rev. C",
  "journal": "Phys.Rev. C64 (2001) 064601",
  "doi": "10.1103/PhysRevC.64.064601",
  "categories": [
    "nucl-th"
  ],
  "abstract": "Microscopic optical potentials for nucleon-nucleus (NA) scattering obtained from the full folding of the effective g matrices, solutions of the Bruckner-Bethe-Goldstone equation, with the densities of the target, are applied to the case of neutron-nucleus scattering. Given that the optical potentials are specified in all two-body angular momentum, spin and isospin channels available to the NA scattering, the only difference in this model description of proton and neutron scattering observables for a given nucleus is in the inclusion of the Coulomb interaction. A priori microscopic optical model predictions for neutron and proton elastic scattering are compared with results from a phenomenological optical model and with data. New measurements are recommended to reduce discrepancies in the existing database, and to differentiate between different theoretical predictions.",
  "revisions": [
    {
      "version": "v2",
      "updated": "2001-08-23T13:51:17.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "microscopic optical potentials",
      "nucleon-nucleus scattering",
      "priori microscopic optical model predictions",
      "two-body angular momentum",
      "bruckner-bethe-goldstone equation"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Phys. Rev. C"
    },
    "note": {
      "typesetting": "TeX",
      "pages": 17,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 555446
    }
  }
}