{
  "id": "1403.4262",
  "version": "v2",
  "published": "2014-03-17T20:07:40.000Z",
  "updated": "2014-09-01T10:16:59.000Z",
  "title": "Electroweak Symmetry Breaking via QCD",
  "authors": [
    "Jisuke Kubo",
    "Kher Sham Lim",
    "Manfred Lindner"
  ],
  "comment": "5 pages, 3 figures. Title changed, references added, matches version published in PRL",
  "journal": "Phys. Rev. Lett. 113, 091604 (2014)",
  "doi": "10.1103/PhysRevLett.113.091604",
  "categories": [
    "hep-ph",
    "hep-ex",
    "hep-lat"
  ],
  "abstract": "We propose a new mechanism to generate the electroweak scale within the framework of QCD, which is extended to include conformally invariant scalar degrees of freedom belonging to a larger irreducible representation of $SU(3)_c$. The electroweak symmetry breaking is triggered dynamically via the Higgs portal by the condensation of the colored scalar field around 1 TeV. The mass of the colored boson is restricted to be 350 GeV $\\lesssim m_S\\lesssim $ 3 TeV, with the upper bound obtained from perturbative renormalization group evolution. This implies that the colored boson can be produced at LHC. If the colored boson is electrically charged, the branching fraction of the Higgs decaying into two photons can slightly increase, and moreover, it can be produced at future linear colliders. Our idea of non-perturbative EW scale generation can serve as a new starting point for more realistic model building in solving the hierarchy problem.",
  "revisions": [
    {
      "version": "v1",
      "updated": "2014-03-17T20:07:40.000Z",
      "title": "Electroweak Symmetry Breaking by QCD",
      "abstract": "We propose a new mechanism to generate the electroweak scale within the framework of QCD, which is extended to include conformally invariant scalar degrees of freedom belonging to a larger irreducible representation of $SU(3)_c$. The electroweak symmetry breaking is triggered dynamically via the Higgs portal by the condensation of the colored scalar field around $1$ TeV. The mass of the colored boson is restricted to be $350$ GeV $\\lesssim m_S\\lesssim 3$ TeV, with the upper bound obtained from renormalization group evolution. This implies that the colored boson can be produced at LHC. If the colored boson is electrically charged, the branching fraction of the Higgs decaying into two photons can slightly increase, and moreover, it can be produced at future linear colliders.",
      "comment": "5 pages, 4 figures",
      "journal": null,
      "doi": null
    },
    {
      "version": "v2",
      "updated": "2014-09-01T10:16:59.000Z"
    }
  ],
  "analyses": {
    "subjects": [
      "11.30.Qc",
      "11.25.Hf",
      "12.38.-t",
      "12.60.Fr"
    ],
    "keywords": [
      "electroweak symmetry breaking",
      "colored boson",
      "renormalization group evolution",
      "conformally invariant scalar degrees",
      "larger irreducible representation"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "publisher": "APS",
      "journal": "Physical Review Letters",
      "year": 2014,
      "month": "Aug",
      "volume": 113,
      "number": 9,
      "pages": "091604"
    },
    "note": {
      "typesetting": "TeX",
      "pages": 5,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 1286312,
      "adsabs": "2014PhRvL.113i1604K"
    }
  }
}