Minimal twist for the Standard Model in noncommutative geometry: The field content
Noncommutative geometry provides both a unified description of the Standard Model of particle physics together with Einstein-Hilbert action (in Euclidean signature) and some tools to go beyond the Standard Model. In this paper, we extend to the full noncommutative geometry of the Standard Model the...
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| Vydáno v: | Physical review. D Ročník 104; číslo 2; s. 1 |
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| Hlavní autoři: | , , |
| Médium: | Journal Article |
| Jazyk: | angličtina |
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American Physical Society
15.07.2021
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| ISSN: | 2470-0010, 2470-0029 |
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| Abstract | Noncommutative geometry provides both a unified description of the Standard Model of particle physics together with Einstein-Hilbert action (in Euclidean signature) and some tools to go beyond the Standard Model. In this paper, we extend to the full noncommutative geometry of the Standard Model the twist (in the sense of Connes-Moscovici) initially worked out for the electroweak sector and the free Dirac operator only. Namely, we apply the twist also to the strong interaction sector and the finite part of the Dirac operator. To do so, we are forced to take into account a violation of the twisted first-order condition. As a result, we still obtain the extra scalar field required to stabilize the electroweak vacuum and fit the Higgs mass, but it now has two chiral components. We also get the additive field of 1-forms already pointed out in the electroweak model, but with a richer structure. Finally, we obtain a pair of Higgs doublets, which are expected to combine into a single Higgs doublet in the action formula, as will be investigated in the second part of this work. |
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| AbstractList | Noncommutative geometry provides both a unified description of the Standard Model of particle physics together with Einstein-Hilbert action (in Euclidean signature) and some tools to go beyond the Standard Model. In this paper, we extend to the full noncommutative geometry of the Standard Model the twist (in the sense of Connes-Moscovici) initially worked out for the electroweak sector and the free Dirac operator only. Namely, we apply the twist also to the strong interaction sector and the finite part of the Dirac operator. To do so, we are forced to take into account a violation of the twisted first-order condition. As a result, we still obtain the extra scalar field required to stabilize the electroweak vacuum and fit the Higgs mass, but it now has two chiral components. We also get the additive field of 1-forms already pointed out in the electroweak model, but with a richer structure. Finally, we obtain a pair of Higgs doublets, which are expected to combine into a single Higgs doublet in the action formula, as will be investigated in the second part of this work. |
| ArticleNumber | 025011 |
| Author | Filaci, Manuele Martinetti, Pierre Pesco, Simone |
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| Cites_doi | 10.1007/JHEP11(2013)132 10.1007/JHEP01(2014)042 10.1007/BF02506388 10.4171/JNCG/108 10.1016/j.geomphys.2013.06.006 10.1007/s11040-016-9228-7 10.1007/s11005-016-0880-4 10.1063/5.0029789 10.1007/JHEP03(2018)089 10.1007/s11040-016-9219-8 10.1007/JHEP09(2012)104 10.4310/ATMP.2007.v11.n6.a3 10.1007/s11005-018-1099-3 10.1007/s11005-018-1120-x 10.1007/978-94-017-9162-5 10.1088/1367-2630/ab9709 10.1007/978-3-030-29597-4 |
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| References | PhysRevD.104.025011Cc19R1 A. Connes (PhysRevD.104.025011Cc1R1) 1994 A. Connes (PhysRevD.104.025011Cc2R1) 2021 PhysRevD.104.025011Cc13R1 PhysRevD.104.025011Cc11R1 PhysRevD.104.025011Cc12R1 A. Connes (PhysRevD.104.025011Cc24R1) 2008 A. H. Chamseddine (PhysRevD.104.025011Cc14R1) 2019 PhysRevD.104.025011Cc17R1 PhysRevD.104.025011Cc26R1 A. Connes (PhysRevD.104.025011Cc15R1) 2008; 38 PhysRevD.104.025011Cc16R1 PhysRevD.104.025011Cc20R1 PhysRevD.104.025011Cc10R1 PhysRevD.104.025011Cc3R1 W. van Suijlekom (PhysRevD.104.025011Cc25R1) 2015 PhysRevD.104.025011Cc4R1 PhysRevD.104.025011Cc5R1 PhysRevD.104.025011Cc6R1 PhysRevD.104.025011Cc8R1 PhysRevD.104.025011Cc9R1 |
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| Title | Minimal twist for the Standard Model in noncommutative geometry: The field content |
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