{ "id": "hep-ph/9910430", "version": "v2", "published": "1999-10-21T12:54:54.000Z", "updated": "1999-11-26T08:36:31.000Z", "title": "On the Dynamical Symmetry Breaking of the Electroweak Interactions by the Top Quark", "authors": [ "V. H. Nguyen", "X. Y. Pham" ], "comment": "Latex2e 9 pages, 2 postscript figures, 1 postscript logo", "journal": "Phys.Lett.B476:331-338,2000", "doi": "10.1016/S0370-2693(00)00142-8", "categories": [ "hep-ph" ], "abstract": "We discuss the electroweak gauge symmetry breaking triggered by a new strong attractive interaction to condensate fermion-antifermion, and topcolor is a prototype. To deal with the fermion pairing, a general method based on the Hubbard-Stratonovich transformation in the functional integral approach is used. We derive a formula which relates the $W^\\pm$, $Z^0$ weak boson masses to that of the condensated fermion, thus generalizing the Pagels-Stokar formula obtained in QCD. The custodial SU(2) electroweak symmetry turns out to be systematically violated, the deviation of $\\rho\\equiv M_W^2/(M_Z^2\\cos^2\\theta_W) $ from unity is related to the new physics scale $\\Lambda$. Some phenomenological consequences of the top-pair condensation models are discussed. Distinctive signatures of the $\\bar{t}t$ scalar bound state, a Higgs boson like denoted by $H_t$, are the dominant decay modes $H_t\\to \\Upsilon +\\gamma ,$ $H_t\\to \\Upsilon +Z^0$, and $H_t \\to B^* +\\bar{B}^*$.", "revisions": [ { "version": "v2", "updated": "1999-11-26T08:36:31.000Z" } ], "analyses": { "subjects": [ "11.15.Ex", "11.15.Tk", "12.60.Fr", "14.80.Cp" ], "keywords": [ "dynamical symmetry breaking", "electroweak interactions", "gauge symmetry breaking", "dominant decay modes", "electroweak gauge symmetry" ], "tags": [ "journal article" ], "note": { "typesetting": "LaTeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable", "inspire": 508957 } } }