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Related papers: Flavour Models with Three Higgs Generations

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We update phenomenological constraints on a Two Higgs Doublet Model with lepton flavour non-conserving Yukawa couplings. We review that $\tan \beta$ is ambiguous in such "Type III" models, and define it from the $\tau$ Yukawa coupling. The…

High Energy Physics - Phenomenology · Physics 2010-06-15 Sacha Davidson , Gerald Grenier

ATLAS and CMS have observed a flavor violating decay of the Higgs to muon and tau. The fact that flavour violating couplings of the Higgs boson are exactly zero in the Standard Model suggests the mixing of the Higgs with another scalar with…

High Energy Physics - Phenomenology · Physics 2017-09-13 Venus Keus

We consider the standard model (SM) extended by the flavor symmetry D5 and search for a minimal model leading to viable phenomenology. We find that it contains four Higgs fields apart from the three generations of fermions whose left- and…

High Energy Physics - Phenomenology · Physics 2009-11-11 C. Hagedorn , M. Lindner , F. Plentinger

The mass matrix forms of quarks and leptons are discussed in theory with permutation flavor symmetry. The structure of scalar potential is analyzed in case that electroweak doublet Higgs fields have non-trivial flavor symmetry charges. We…

High Energy Physics - Phenomenology · Physics 2008-11-26 Satoru Kaneko , Hideyuki Sawanaka , Takaya Shingai , Morimitsu Tanimoto , Koichi Yoshioka

We study flavour-changing neutral current decays of the top quark in the democratic Three Higgs Doublet Model featuring a $Z_3$-symmetric scalar potential and Natural Flavour Conservation. In this framework, while such processes are absent…

High Energy Physics - Phenomenology · Physics 2026-01-26 Baradhwaj Coleppa , Benjamin Fuks , Akshat Khanna

We have presented a $S_4$ flavor model to unify quarks and leptons in the framework of the SU(5) GUT. Three generations of $\bar5$-plets in SU(5) are assigned $3_1$ of $S_4$ while the first and the second generations of 10-plets in SU(5)…

High Energy Physics - Phenomenology · Physics 2010-04-15 Hajime Ishimori , Yusuke Shimizu , Morimitsu Tanimoto

We discuss the neutrino masses and mixings as the realization of an $S_{3}$ flavour permutational symmetry in two models, namely the Standard Model and an extension of the Standard Model with three Higgs doublets. In the $S_3$ Standard…

High Energy Physics - Phenomenology · Physics 2013-03-26 F. Gonzalez Canales , A. Mondragon , M. Mondragon

The doublet-triplet splitting problem can be simply solved in product-group GUT models, using a global symmetry that distinguishes the doublets from the triplets. Apart from giving the required mass hierarchy, this ``triplet symmetry'' can…

High Energy Physics - Phenomenology · Physics 2009-11-11 Yehonathan Segev , Yael Shadmi

After we study the 6-dimensional ${\cal N} = (1, 1)$ supersymmetry breaking and $R$ symmetry breaking on $M^4\times T^2/Z_n$, we construct two ${\cal N} = (1, 1)$ supersymmetric $E_6$ models on $M^4\times T^2/Z_3$ where $E_6$ is broken down…

High Energy Physics - Phenomenology · Physics 2014-11-17 Tianjun Li

We demonstrate that an $SU(2)_L\times U(1)_Y$ model with extended Higgs sector gives rise to bi-maximal neutrino mixing through the incorporation of SO(3) flavour symmetry and discrete symmetry. The neutrino and the charged lepton masses…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ambar Ghosal

It is shown that it is possible to create successful models of flavor for both quarks and leptons using the discrete non-abelian group $T^{\prime}$ by itself. Two simple realizations are presented that can be used as the starting point for…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alfredo Aranda

Grand unified theories with fermions transforming as irreducible representations of a discrete nonabelian flavor symmetry can lead to realistic fermion masses, without requiring very small fundamental parameters. We construct a specific…

High Energy Physics - Phenomenology · Physics 2013-11-13 David B. Kaplan , Martin Schmaltz

In modular-invariant models of flavour, hierarchical fermion mass matrices may arise solely due to the proximity of the modulus $\tau$ to a point of residual symmetry. This mechanism does not require flavon fields, and modular weights are…

High Energy Physics - Phenomenology · Physics 2024-06-11 P. P. Novichkov , J. T. Penedo , S. T. Petcov

We extend our previous algebraic construction of three fermion generations in the complex Clifford algebra $\mathbb{C}\ell(10)$ by incorporating the Higgs sector. Using the $S_3$ family symmetry that permutes three algebraically…

General Physics · Physics 2026-04-29 Niels Gresnigt

In the framework of the modular symmetry approach to lepton flavour, we consider a class of theories where matter superfields transform in representations of the finite modular group $\Gamma_5 \simeq A_5$. We explicitly construct a basis…

High Energy Physics - Phenomenology · Physics 2019-05-02 P. P. Novichkov , J. T. Penedo , S. T. Petcov , A. V. Titov

We present a supersymmetric Pati-Salam model with small representations as a potential candidate for physics beyond the Standard Model. The model features a Higgs sector with bifundamental fields $H_R+\bar H_R=(4,1,2)+(\bar 4,1,2)$,…

High Energy Physics - Phenomenology · Physics 2025-02-24 George K. Leontaris , Ruiwen Ouyang , Ye-ling Zhou

We discuss our recently proposed S3(down)xS3(up) flavour-permutation-symmetric mixing observables, giving expressions for them in terms of (moduli-squared) of the mixing matrix elements. We outline their successful use in providing…

High Energy Physics - Phenomenology · Physics 2008-05-23 P. F. Harrison , D. R. J. Roythorne , W. G. Scott

We show how gauged flavour breaking and N = 1 supersymmetry breaking can be dynamically aligned to produce natural models. Supersymmetry is broken in a metastable vacuum, while a weakly gauged flavour symmetry is identified with an SU(3)_F…

High Energy Physics - Phenomenology · Physics 2015-06-19 Steven Abel , Moritz McGarrie

Using an SU(3)-flavour symmetry breaking expansion between the strange and light quark masses, we determine how this constrains the extrapolation of baryon octet matrix elements and form factors. In particular we can construct certain…

High Energy Physics - Lattice · Physics 2021-12-09 J. M. Bickerton , A. N. Cooke , R. Horsley , Y. Nakamura , H. Perlt , D. Pleiter , P. E. L. Rakow , G. Schierholz , H. Stüben , R. D. Young , J. M. Zanotti

We propose a twin Pati-Salam (PS) theory of flavour broken to the $G_{4321}$ gauge group at high energies, then to the Standard Model at low energies, yielding a TeV scale vector leptoquark $U^{\mu}_1(3,1,2/3)$ which has been suggested to…

High Energy Physics - Phenomenology · Physics 2021-11-24 Stephen F. King
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