An SU(5)\(\otimes\)Z_{13} Grand Unification Model
We propose an SU(5) grand unified model with an invisible axion and the unification of the three coupling constants which is in agreement with the values, at \(M_Z\), of \(\alpha\), \(\alpha_s\), and \(\sin^2\theta_W\). A discrete, anomalous, \(Z_{13}\) symmetry implies that the Peccei-Quinn symmetr...
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description | We propose an SU(5) grand unified model with an invisible axion and the unification of the three coupling constants which is in agreement with the values, at \(M_Z\), of \(\alpha\), \(\alpha_s\), and \(\sin^2\theta_W\). A discrete, anomalous, \(Z_{13}\) symmetry implies that the Peccei-Quinn symmetry is an automatic symmetry of the classical Lagrangian protecting, at the same time, the invisible axion against possible semi-classical gravity effects. Although the unification scale is of the order of the Peccei-Quinn scale the proton is stabilized by the fact that in this model the standard model fields form the SU(5) multiplets completed by new exotic fields and, also, because it is protected by the \(Z_{13}\) symmetry. |
doi_str_mv | 10.48550/arxiv.0708.1009 |
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A discrete, anomalous, \(Z_{13}\) symmetry implies that the Peccei-Quinn symmetry is an automatic symmetry of the classical Lagrangian protecting, at the same time, the invisible axion against possible semi-classical gravity effects. Although the unification scale is of the order of the Peccei-Quinn scale the proton is stabilized by the fact that in this model the standard model fields form the SU(5) multiplets completed by new exotic fields and, also, because it is protected by the \(Z_{13}\) symmetry.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.0708.1009</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Symmetry</subject><ispartof>arXiv.org, 2007-12</ispartof><rights>Notwithstanding the ProQuest Terms and conditions, you may use this content in accordance with the associated terms available at http://arxiv.org/abs/0708.1009.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>780,784,27925</link.rule.ids></links><search><creatorcontrib>Dias, Alex G</creatorcontrib><creatorcontrib>Franco, Edison T</creatorcontrib><creatorcontrib>Pleitez, Vicente</creatorcontrib><title>An SU(5)\(\otimes\)Z_{13} Grand Unification Model</title><title>arXiv.org</title><description>We propose an SU(5) grand unified model with an invisible axion and the unification of the three coupling constants which is in agreement with the values, at \(M_Z\), of \(\alpha\), \(\alpha_s\), and \(\sin^2\theta_W\). 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A discrete, anomalous, \(Z_{13}\) symmetry implies that the Peccei-Quinn symmetry is an automatic symmetry of the classical Lagrangian protecting, at the same time, the invisible axion against possible semi-classical gravity effects. Although the unification scale is of the order of the Peccei-Quinn scale the proton is stabilized by the fact that in this model the standard model fields form the SU(5) multiplets completed by new exotic fields and, also, because it is protected by the \(Z_{13}\) symmetry.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.0708.1009</doi><oa>free_for_read</oa></addata></record> |
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title | An SU(5)\(\otimes\)Z_{13} Grand Unification Model |
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