{ "id": "1312.0051", "version": "v1", "published": "2013-11-30T02:45:37.000Z", "updated": "2013-11-30T02:45:37.000Z", "title": "The Muon Anomalous Magnetic Moment in the Reduced Minimal 3-3-1 Model", "authors": [ "Chris Kelso", "P. R. D. Pinheiro", "Farinaldo S. Queiroz", "William Shepherd" ], "comment": "19 pages, 4 figures", "journal": "Eur.Phys.J. C74 (2014) 2808", "doi": "10.1140/epjc/s10052-014-2808-4", "categories": [ "hep-ph" ], "abstract": "We study the muon anomalous magnetic moment $(g-2)_{\\mu}$ in the context of the reduced minimal 3-3-1 model recently proposed in the literature. In particular, its spectrum contains a doubly charged scalar ($H^{\\pm \\pm}$) and gauge boson ($U^{\\pm \\pm}$), new singly charged vectors ($V^{\\pm}$) and a $Z^{\\prime}$ boson, each of which might give a sizeable contribution to the $(g-2)_{\\mu}$. We compute the 1-loop contributions from all these new particles to the $(g-2)_{\\mu}$. We conclude that the doubly charged vector boson provides the dominant contribution, and by comparing our results with the experimental constraints we derive an expected value for the scale of $SU(3)_L\\otimes U(1)_N$ symmetry breaking $v_{\\chi} \\sim 2$ TeV. We also note that, if the discrepancy in the anomalous moment is resolved in the future without this model then the constraints will tighten to requiring $v_\\chi > 2.7$ TeV with current precision, and will entirely rule out the model if the expected precision is achieved by the future experiment at Fermilab.", "revisions": [ { "version": "v1", "updated": "2013-11-30T02:45:37.000Z" } ], "analyses": { "keywords": [ "muon anomalous magnetic moment", "reduced minimal", "spectrum contains", "doubly charged vector boson", "gauge boson" ], "tags": [ "journal article" ], "publication": { "journal": "European Physical Journal C", "year": 2014, "month": "Mar", "volume": 74, "pages": 2808 }, "note": { "typesetting": "TeX", "pages": 19, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1266979, "adsabs": "2014EPJC...74.2808K" } } }