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Motivated by the fact that, in some realistic models combining SO(10) GUTs and flavour symmetries, it is not possible to achieve the required baryon asymmetry through the CP asymmetry generated in the decay of right-handed neutrinos, we…

High Energy Physics - Phenomenology · Physics 2009-01-06 E. J. Chun , L. Velasco-Sevilla

We construct an explicit $SO(10) \times U(1)_F$ model of the Yukawa interactions by using as a guide previous phenomenological results obtained from a bottom-up approach to quark and lepton mass matrices. The global $U(1)_F$ family symmetry…

High Energy Physics - Phenomenology · Physics 2009-10-28 Carl H. Albright , Satyanarayan Nandi

A non-supersymmetric renormalizable $SO(10)$ model, with CP invariant Yukawa sector consisting of Lorentz scalars in $10$ and $\overline{126}$ dimensional representations, is proposed. The elemental Yukawa couplings are real due to CP…

High Energy Physics - Phenomenology · Physics 2023-05-01 Ketan M. Patel

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…

High Energy Physics - Phenomenology · Physics 2008-11-26 Soren Wiesenfeldt , Scott Willenbrock

A minimal SO(10) Higgs structure involving a single adjoint field along with spinors, vectors and singlets has been shown to break the SO(10) gauge symmetry to the standard model while stabilizing the F-flat directions and solving the…

High Energy Physics - Phenomenology · Physics 2011-05-12 Carl H. Albright , K. S. Babu , S. M. Barr

In this talk we discuss SO(10) Yukawa unification and its ramifications for phenomenology. The initial constraints come from fitting the top, bottom and tau masses, requiring large $\tan\beta \sim 50$ and particular values for soft SUSY…

High Energy Physics - Phenomenology · Physics 2015-06-17 Stuart Raby

We construct a realistic model based on SUSY SO(10) with U(2) flavor symmetry. In contrast to the commonly used effective operator approach, $126-$dimensional Higgses are used to construct the Yukawa sector. R-parity symmetry is thus…

High Energy Physics - Phenomenology · Physics 2011-07-19 Mu-Chun Chen , K. T. Mahanthappa

The clockwork mechanism, which can naturally explain the origin of small numbers, is implemented in $SO(10)$ grand unified theories to address the origin of hierarchies in fermion masses and mixings. We show that a minimal Yukawa sector…

High Energy Physics - Phenomenology · Physics 2021-01-13 K. S. Babu , Shaikh Saad

Grand Unified Theories (GUTs) based on groups like $SO(10)$ and $SU(5)$ unify Standard Model (SM) fermions into irreducible representations (irreps), and predict additional scalar fields beyond the SM Higgs. In $SO(10)$ GUTs, the scalar…

High Energy Physics - Phenomenology · Physics 2025-07-23 Saurabh K. Shukla

It is often argued that in the class of non-supersymmetric SO(10) grand unified theories there is barely any room for reconciling the lower bound on the position of the GUT scale emerging from the proton decay searches and the lower limit…

High Energy Physics - Phenomenology · Physics 2014-11-20 Michal Malinsky

It is well-known that the $SU(5)$ grand unified theory, with the standard model quarks and leptons unified in $\overline{5}$ and $10$ and the electroweak Higgs doublet residing in $5$ dimensional representations, leads to relation,…

High Energy Physics - Phenomenology · Physics 2024-01-12 Ketan M. Patel , Saurabh K. Shukla

We study Yukawa unification, including the effects of a physical neutrino mass consistent with the Superkamiokande observations, in a string/$D$-brane inspired Pati-Salam model which allows the most general non-universal scalar and gaugino…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. F. King , M. Oliveira

We recapitulate the latest results on the class of the simplest SO(10) grand unified models in which the GUT-scale symmetry breaking is triggered by an adjoint Higgs representation. We argue that the minimal survival approximation…

High Energy Physics - Phenomenology · Physics 2015-06-11 Stefano Bertolini , Luca Di Luzio , Michal Malinsky

Neutrino and charged fermion masses provide important constraints on grand unified theories. We illustrate this by focusing on a renormalizable, supersymmetric SO(10) theory proposed long ago, that recently attracted great interest in view…

High Energy Physics - Phenomenology · Physics 2009-11-18 Borut Bajc , Alejandra Melfo , Goran Senjanovic , Francesco Vissani

We discuss the possibility of unifying in a simple and economical manner the Yukawa couplings of third generation fermions in a non-supersymmetric SO(10) model with an intermediate symmetry breaking, focusing on two possible patterns with…

High Energy Physics - Phenomenology · Physics 2022-12-23 Abdelhak Djouadi , Ruiwen Ouyang , Martti Raidal

We study a prediction on neutrino observables in a non-supersymmetric renormalizable $SO(10)$ GUT model that contains a ${\bf 10}$ complex scalar field and a ${\bf 126}$ scalar field whose Yukawa couplings with ${\bf 16}$ matter fields…

High Energy Physics - Phenomenology · Physics 2023-04-19 Naoyuki Haba , Yasuhiro Shimizu , Toshifumi Yamada

Grand unification of gauge couplings and fermionic representations remains an appealing proposal to explain the seemingly coincidental structure of the Standard Model. However, to realise the Standard Model at low energies, the unified…

High Energy Physics - Phenomenology · Physics 2022-08-16 Aaron Held , Jan Kwapisz , Lohan Sartore

We consider fermion masses and mixings in a renormalizable SUSY SO(10) GUT with Yukawa couplings of scalar fields in the representation 10 + 120 + 126 bar. We investigate a scenario defined by the following assumptions: i) A single large…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Grimus , H. Kuhbock

We propose a simple supersymmetric SO(10) GUT model with only doublet Higgs scalars. The fermion mass problem is naturally solved by a new one-loop diagram. R-parity is conserved implying a stable LSP which can explain the dark matter of…

High Energy Physics - Phenomenology · Physics 2009-11-10 Utpal Sarkar

We construct the SU(5) and SO(10) models from F-theory. Turning on the U(1) fluxes, we can break the SU(5) gauge symmetry down to the Standard Model (SM) gauge symmetry, and break the SO(10) gauge symmetry down to the SU(3)_C X SU(2)_L X…

High Energy Physics - Theory · Physics 2010-04-29 Tianjun Li
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