Perturbative SO(10) GUT and the Minimal Higgs Sector
| dc.creator | Wiesenfeldt, Soren | |
| dc.creator | Willenbrock, Scott | |
| dc.date | 2007-07-23 | |
| dc.date | 2008-02-16 | |
| dc.date.accessioned | 2026-07-07T11:18:01Z | |
| dc.date.available | 2026-07-07T11:18:01Z | |
| dc.description | The breaking of SO(10) to SU(3)_C x U(1)_EM can be accomplished by just four Higgs fields: the symmetric rank-two tensor, S(54); a pair of spinors, C(16) and Cbar(16bar); and a vector, T(10). This setup is also able to generate realistic fermion masses. The heavy color triplets in the vector and spinor fields mediate proton decay via dimension-five operators. The experimental bounds on proton decay constrain the structure and size of the Yukawa operators. | |
| dc.description | v2: discussion about gauge coupling unification extended; figure added; to appear in Phys. Lett. B | |
| dc.identifier | https://arxiv.org/abs/0707.3300 | |
| dc.identifier | http://arxiv.org/abs/0707.3300 | |
| dc.identifier | Phys.Lett.B661:268-272,2008 | |
| dc.identifier | doi:10.1016/j.physletb.2008.02.022 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/193203 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Perturbative SO(10) GUT and the Minimal Higgs Sector | |
| dc.type | text |