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Related papers: Quark and Lepton Masses in 5D SO(10)

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In this work we study an SO(10) GUT model with minimum Higgs representations belonging only to the 210 and 16 dimensional representations of SO(10). We add a singlet fermion S in addition to the usual 16 dimensional representation…

High Energy Physics - Phenomenology · Physics 2009-11-11 Kaushik Bhattacharya , C. R. Das , Bipin R. Desai , G. Rajasekaran , Utpal Sarkar

We construct realistic theories in which the Higgs fields arise from extra dimensional components of higher dimensional gauge fields. In particular, we present a minimal 5D SU(3)_C x SU(3)_W model and a unified 5D SU(6) model. In both cases…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gustavo Burdman , Yasunori Nomura

The alternative renormalizable minimal $SO(10)$ model is composed of the Yukawa couplings with $\textbf{10} \oplus \textbf{120}$ Higgs fields, whereas the right-handed (RH) neutrino Majorana masses are generated via the Witten mechanism.…

High Energy Physics - Phenomenology · Physics 2020-03-17 Takeshi Fukuyama , Nobuchika Okada , Hieu Minh Tran

We quantitatively analyze a quark-lepton flavour model derived from a six-dimensional supersymmetric theory with $SO(10)\times U(1)$ gauge symmetry, compactified on an orbifold with magnetic flux. Two bulk $\mathbf{16}$-plets charged under…

High Energy Physics - Phenomenology · Physics 2018-04-25 Wilfried Buchmuller , Ketan M. Patel

The supersymmetric (SUSY) minimal SO(10) model is a well-motivated grand unified theory, where the Standard Model (SM) fermions have Yukawa couplings with only one ${\bf 10}$-plet and one $\overline{\bf 126}$-plet Higgs fields and it is…

High Energy Physics - Phenomenology · Physics 2023-03-31 Takeshi Fukuyama , Nobuchika Okada , Hieu Minh Tran

A model based on SUSY SO(10) combined with U(2) family symmetry constructed recently by the authors is generalized to include phases in the mass matrices leading to CP violation. In contrast with the commonly used effective operator…

High Energy Physics - Phenomenology · Physics 2014-11-17 Mu-Chun Chen , K. T. Mahanthappa

We discuss a minimal Supersymmetric SO(10) model where B-L symmetry is broken by a {\bf 126} dimensional Higgs multiplet which also contributes to fermion masses in conjunction with a {\bf 10} dimensional superfield. This minimal Higgs…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. S. Goh , R. N. Mohapatra , Siew-Phang Ng

We study models of supersymmetric grand unification based on the SO(10) gauge group. We investigate scenarios of non-universal gaugino masses including models containing a mixture of two representations of hidden sector chiral superfields.…

High Energy Physics - Phenomenology · Physics 2014-12-30 D. J. Miller , A. P. Morais

Maximally supersymmetric SO(10) and SU(6) unified theories are constructed on the orbifold T^2/(Z_2 x Z'_2), with one length scale R_5 taken much larger than the other, R_6. The effective theory below 1/R_6 is found to be the highly…

High Energy Physics - Phenomenology · Physics 2009-09-29 Lawrence J. Hall , Yasunori Nomura

Has any progress been made on understanding and predicting the 13 parameters which describe the observed masses and mixing angles of the quarks and leptons? Arguments are given in favor of pursuing schemes in which grand unified and family…

High Energy Physics - Phenomenology · Physics 2009-10-22 Lawrence J. Hall

A model based on SUSY SO(10) combined with SU(2) family symmetry is constructed. In contrast with the commonly used effective operator approach, 126-dimensional Higgs fields are utilized to construct the Yukawa sector. R-parity symmetry is…

High Energy Physics - Phenomenology · Physics 2009-11-10 Mu-Chun Chen , K. T. Mahanthappa

We study the implications for bounds on the top quark pole mass m_t in models with low scale supersymmetry following the discovery of the Standard Model-like Higgs boson. In the minimal supersymmetric standard model, we find that m_t >= 164…

High Energy Physics - Phenomenology · Physics 2015-06-18 Ilia Gogoladze , Rizwan Khalid , Shabbar Raza , Qaisar Shafi

The form of the most general orbifold breaking of gauge, global and supersymmetries with a single extra dimension is given. In certain theories the Higgs boson mass is ultraviolet finite due to an unbroken local supersymmetry, which is…

High Energy Physics - Theory · Physics 2010-05-28 Riccardo Barbieri , Lawrence J. Hall , Yasunori Nomura

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

We consider a supersymmetric SO(10) model with a SU(3) symmetry of flavour in which fermion masses emerge via the see-saw mixing with superheavy fermions in 16+16bar representations. In this model the dangerous D=5 operators of proton decay…

High Energy Physics - Phenomenology · Physics 2009-11-11 Z. Berezhiani , F. Nesti

In a supersymmetric SU(5) grand unified model with a horizontal symmetry SU(1,1), we discuss spontaneous generation of generations to produce three chiral generations of quarks and leptons and one generation of higgses by using one…

High Energy Physics - Phenomenology · Physics 2014-05-07 Naoki Yamatsu

We investigate quartification models in five dimensions, with the fifth dimension forming an $S^1/Z_2\times Z_2'$ orbifold. The orbifold construction is combined with a boundary Higgs sector to break the quartified gauge group directly to a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alison Demaria , Kristian L. McDonald

A model is presented that fits the quark and lepton masses and mixings wherein five dimensionless parameters and a phase account for fifteen dimensionless observables. Among these are the Wolfenstein parameters $\rho$ and $\eta$, the…

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

We investigate a model on an extra dimension $S^1$ where plenty of effective boundary points described by point interactions (zero-thickness branes) are arranged. After suitably selecting the conditions on these points for each type of…

High Energy Physics - Phenomenology · Physics 2015-06-19 Yukihiro Fujimoto , Kenji Nishiwaki , Makoto Sakamoto , Ryo Takahashi

On the basis of the universal seesaw mass matrix model, which is a promising model of the unified description of the quark and lepton mass matrices, the behaviors of the gauge coupling constants and intermediate energy scales in the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yoshio Koide