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Related papers: $SO(10)$ models with $A_4$ modular symmetry

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The even weight modular forms of level $N$ can be arranged into the common irreducible representations of the inhomogeneous finite modular group $\Gamma_N$ and the homogeneous finite modular group $\Gamma'_N$ which is the double covering of…

High Energy Physics - Phenomenology · Physics 2021-09-30 Jun-Nan Lu , Xiang-Gan Liu , Gui-Jun Ding

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

We propose a natural $ S_4 \times SO(10) $ supersymmetric grand unified theory of flavour with an auxiliary $\mathbb{Z}_4^2 \times \mathbb{Z}_4^R$ symmetry, based on small Higgs representations (nothing larger than an adjoint) and hence a…

High Energy Physics - Phenomenology · Physics 2017-11-03 Fredrik Björkeroth , Francisco J. de Anda , Stephen F. King , Elena Perdomo

We propose a model with $A_4$ flavor symmetry for leptons and quarks in the framework of supersymmetric SU(5) grand unified theory (GUT). The running masses of quarks and charged leptons at GUT scale ($\sim 10^{16}$ GeV) are realized by the…

High Energy Physics - Phenomenology · Physics 2019-07-23 Yu Muramatsu , Hideaki Okane , Yusuke Shimizu , Kenta Takagi

The recent experimental results indicating the neutrino oscillations may strongly suggest that at least one more light neutrino species is required in order to reconcile the existing data. In the simple GUT frameworks, this fact seems…

High Energy Physics - Phenomenology · Physics 2009-10-31 Masako Bando , Koichi Yoshioka

Can the SO(10) model with one {\bf 10} and one {\bf 126} Higgs scalars give the observed masses and mixings of quarks and leptons without any other additional Higgs scalars? Recently, at least, for quarks and charged leptons, it has been…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. Matsuda , Y. Koide , T. Fukuyama , H. Nishiura

We consider a novel model for three standard families of left chiral states of quarks and leptons conjointly with a new family of dark matter fermionic particles and a sterile neutrino. It is suggested to use a SO(10) symmetry for…

High Energy Physics - Phenomenology · Physics 2016-10-13 V. V. Khruschov

The leptonic Higgs doublet model of neutrino masses is implemented with an A_4 discrete symmetry (the even permutation of 4 objects or equivalently the symmetry of the tetrahedron) which has 4 irreducible representations: 1, 1', 1'', and 3.…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ernest Ma , G. Rajasekaran

A predictive framework for fermion masses and mixing is given by the supersymmetric SO(10) model with one 10, one bar126, one 126 and one 210 Higgs representations, and type II seesaw dominating the neutrino mass matrix. We investigate the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Stefano Bertolini , Michele Frigerio , Michal Malinsky

We report the viability of the Type I seesaw mechanism in 3 generation renormalizable SO(10) GUTs based on the $\mathbf{{210-10-\oot-126-120}}$ Higgs system. The $\mathbf{120}$ -plet and $ \mathbf{10}$-plet Higgs fit charged fermion masses…

High Energy Physics - Phenomenology · Physics 2007-05-23 Charanjit S. Aulakh

A new SO(10) unified model is proposed based on a one step breaking of SO(10) to the Standard Model gauge group $SU(3)\times SU(2)\times U(1)_Y$ using a single 144 of Higgs. The symmetry breaking occurs when the SU(5) 24-plet component of…

High Energy Physics - Phenomenology · Physics 2009-11-11 K. S. Babu , Ilia Gogoladze , Pran Nath , Raza M. Syed

Based on a maximally symmetric minimal unification hypothesis and a quantum charge-dimension correspondence principle, it is demonstrated that each family of quarks and leptons belongs to the Majorana-Weyl spinor representation of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yue-Liang Wu

Neutrino masses have been extensively studied in the context of discrete symmetries. A family permutation symmetry easily explains all neutrino oscillations and their mixing angles. However it is not obvious the embedding of such symmetry…

High Energy Physics - Phenomenology · Physics 2016-09-06 Francesco Caravaglios , Stefano Morisi

An $SO(10)$ model where the $10_H$ and $120_H$ representations are used for generating fermion masses is quite predictive, though due to the absence of $SU(2)_{L,R}$ triplet/singlet fields it cannot give rise to neutrino masses through the…

High Energy Physics - Phenomenology · Physics 2015-05-20 Joydeep Chakrabortty , Srubabati Goswami , Amitava Raychaudhuri

We give a model for composite quarks and leptons based on the semisimple gauge group SU(4), with the preons in the 10 representation; this choice of gauge gluon and preon multiplets is motivated by the possibility of embedding them in an…

High Energy Physics - Theory · Physics 2016-09-06 Stephen L. Adler

Family Replicated Gauge Group models of the type SU(n)^N\times SU(m)^N, (SMG)^3 and (SMG\times U(1)_{B-L})^3 are reviewed, where SMG=SU(3)_{c}\times SU(2)_{L}\times U(1)_{Y} is the gauge symmetry group of the Standard Model, $B$ is the…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. D. Froggatt , L. V. Laperashvili , H. B. Nielsen , Y. Takanishi

We propose an inverse seesaw model with large $SU(2)_L$ multiplets applying modular $A_4$ symmetry where $SU(2)_L$ quartet and septet fermions are introduced as triplets under the symmetry. The neutral components of the quartet contribute…

High Energy Physics - Phenomenology · Physics 2020-07-31 Takaaki Nomura , Hiroshi Okada

Renormalizable SO(10) grand unified theories (GUTs), extended by $O(N_g)_F$ family gauge symmetry, generate minimal supersymmetric Standard Model flavour structure dynamically via vacuum expectation values of "Yukawon" Higgs multiplets. For…

High Energy Physics - Phenomenology · Physics 2015-06-17 Charanjit S. Aulakh , Charanjit K. Khosa

In a renormalizable $SO(10)$ theory, all fermion mass matrices are linear combinations of three fundamental types, $M^{10}, M^{\overline{126}}$, and $M^{120}$, whose superscripts indicate their $SO(10)$ transformation properties. We point…

High Energy Physics - Phenomenology · Physics 2015-06-19 C. S. Lam

$\mu$-$\tau$ symmetry imposed on the neutrino mass matrix in the flavour basis is known to be quite predictive. We integrate this very specific neutrino symmetry into a more general framework based on the supersymmetric SO(10) grand unified…

High Energy Physics - Phenomenology · Physics 2010-11-30 Anjan S. Joshipura , Bhavik P. Kodrani , Ketan M. Patel