{
  "id": "1903.02892",
  "version": "v1",
  "published": "2019-03-07T13:10:55.000Z",
  "updated": "2019-03-07T13:10:55.000Z",
  "title": "Bound states of relativistic nature",
  "authors": [
    "V. A. Karmanov",
    "J. Carbonell",
    "H. Sazdjian"
  ],
  "comment": "13 pages, 10 figures, to be published in Proceedings of the International Conference: Nuclear Theory in the Supercomputing Era-2018 (NTSE-2018), Daejeon, South Korea, October 29 - November 2, 2018; eds. A. M. Shirokov and A. I. Mazur. Pacific National University, Khabarovsk, Russia, 2019",
  "categories": [
    "hep-ph",
    "hep-th",
    "nucl-th"
  ],
  "abstract": "Bethe-Salpeter equation, for massless exchange and large fine structure constant $\\alpha>\\pi/4$, in addition to the Balmer series, provides another (abnormal) series of energy levels which are not given by the Schr\\\"odinger equation. So strong field can be created by a point-like charge $Z>107$. The nuclei with this charge, though available, they are far from to be point-like that weakens the field. Therefore, the abnormal states of this origin hardly exist. We analyze the more realistic case of exchange by a massive particle when the large value of coupling constant is typical for the strong interaction. It turns out that this interaction still generates a series of abnormal relativistic states. The properties of these solutions are studied. Their existence in nature seems possible.",
  "revisions": [
    {
      "version": "v1",
      "updated": "2019-03-07T13:10:55.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "bound states",
      "relativistic nature",
      "large fine structure constant",
      "abnormal relativistic states",
      "bethe-salpeter equation"
    ],
    "tags": [
      "conference paper"
    ],
    "note": {
      "typesetting": "TeX",
      "pages": 13,
      "language": "en",
      "license": "arXiv",
      "status": "editable"
    }
  }
}