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Related papers: Dynamical Flavor Hierarchy and Heavy Top

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The spontaneous breaking of the $SU(3)^5$ quark/lepton flavor symmetry by means of three multiplets of scalar `Yukawa fields' admits vacua with one O(1) and two vanishing vacuum expectation values (vevs) for each multiplet. If the number of…

High Energy Physics - Phenomenology · Physics 2011-09-08 Enrico Nardi

One main obstacle for any beyond the SM (BSM) scenario solving the hierarchy problem is its potentially large contributions to electric dipole moments. An elegant way to avoid this problem is to have the light SM fermions couple to the BSM…

High Energy Physics - Phenomenology · Physics 2016-08-24 Giuliano Panico , Alex Pomarol

A dynamical origin of the Yukawa couplings is a promising scenario to explain the flavour puzzle. The focus of this letter is set on the role of the neutrino Majorana character: when an $O(2)_{N_R}$ flavour symmetry acts on the right-handed…

High Energy Physics - Phenomenology · Physics 2015-06-16 R. Alonso , M. B. Gavela , D. Hernandez , L. Merlo , S. Rigolin

We reconsider the flavor problem in the models with two Higgs doublets. By studying two generation toy models, we look for flavor basis independent constraints on Yukawa couplings that will give us the mass hierarchy while keeping all…

High Energy Physics - Phenomenology · Physics 2011-03-17 Andrew E. Blechman , Alexey A. Petrov , Gagik Yeghiyan

We construct a supersymmetric theory of flavor based on the discrete gauge group (D_6)^2, where D_6 describes the symmetry of a regular hexagon under proper rotations in three dimensions. The representation structure of the group allows one…

High Energy Physics - Phenomenology · Physics 2014-11-17 Christopher D. Carone , Richard F. Lebed

We present a model where all fermions are contained in a single irreducible representation of an SU(19) gauge symmetry group. If there is only one scalar field, Yukawa interactions are controlled by a single number rather than by one or…

High Energy Physics - Phenomenology · Physics 2021-03-17 Andreas Ekstedt , Renato M. Fonseca , Michal Malinský

Motivated by the fermion mass hierarchy we study the phenomenology of two flavorful two-Higgs-doublet model (2HDM) scenarios. By virtue of the flavor or singular alignment ansatz it is possible to link the mass of a subset of fermions to…

High Energy Physics - Phenomenology · Physics 2021-08-25 J. L. Diaz-Cruz , U. J. Saldana-Salazar , K. M. Tame-Narvaez , V. T. Tenorth

We consider the maximal U(3) horizontal scheme as a handle on fermion masses and mixings. In particular, we attempt to explain the large top Yukawa coupling and the masses and mixing in the two heaviest generations. A simple model is…

High Energy Physics - Phenomenology · Physics 2016-08-25 Andrija Rasin

We study a hybrid model in which the Technicolor and fundamental heavy scalars live together. We concern extreme case, where electroweak symmetry breaking (EWSB) comes almost entirely from the strong dynamics of Technicolor, but the masses…

High Energy Physics - Phenomenology · Physics 2013-04-16 Vladimir Sauli

We classify models of the Dirac neutrino mass by concentrating on flavor structures of the mass matrix. The advantage of our classification is that we do not need to specify detail of models except for Yukawa interactions because flavor…

High Energy Physics - Phenomenology · Physics 2016-05-26 Shinya Kanemura , Kodai Sakurai , Hiroaki Sugiyama

In a generic supersymmetric extension of the Standard Model, whether unified or not, a simple and well motivated U(2) symmetry, acting on the lightest two generations, completely solves the flavour changing problem and necessarily leads to…

High Energy Physics - Phenomenology · Physics 2009-10-28 Riccardo Barbieri , George Dvali , Lawrence Hall

In the so-called yukawaon model, where effective Yukawa coupling constants Y_f^{eff} (f=e,\nu,u,d) are given by vacuum expectation values of gauge singlet scalars (yukawaons) Y_f with 3\times 3 flavor components, it is tried to give a…

High Energy Physics - Phenomenology · Physics 2010-01-14 Yoshio Koide

It has recently been shown that F-theory based constructions provide a potentially promising avenue for engineering GUT models which descend to the MSSM. In this note we show that in the presence of background fluxes, these models…

High Energy Physics - Theory · Physics 2014-11-18 Jonathan J. Heckman , Cumrun Vafa

The structure of the mass matrix, a challenging problem in the Standard Model, is closely related to flavor phenomenology and the understanding of the Yukawa interaction. We derive a factorized mass structure based on observed fermion mass…

High Energy Physics - Phenomenology · Physics 2025-07-08 Qingfeng Cao , Ying Zhang

The origin of mass must lie in physics beyond the Standard Model. Dynamical electroweak symmetry breaking models like technicolor can generate masses for the W and Z bosons. Providing the large top quark mass and large top-bottom mass…

High Energy Physics - Phenomenology · Physics 2007-05-23 Elizabeth H. Simmons

We propose a class of theories to generate quark and lepton mass matrices where the scale of new physics is at the TeV scale, without inducing the large flavor and CP violating processes that are often thought to relegate the origin of…

High Energy Physics - Phenomenology · Physics 2026-02-23 Nima Arkani-Hamed , Carolina Figueiredo , Lawrence J. Hall , Claudio Andrea Manzari

We present a class of supersymmetric models in which flavor symmetries are broken dynamically, by a set of composite flavon fields. The strong dynamics that is responsible for confinement in the flavor sector also drives flavor symmetry…

High Energy Physics - Phenomenology · Physics 2014-11-17 Christopher D. Carone , Lawrence J. Hall , Takeo Moroi

We consider a 4-Higgs-doublet model in which each Higgs doublet gives mass to one of the fermion sets $\{ m_t\}$, $\{ m_b,m_\tau,m_c \}$, $\{ m_\mu,m_s \}$, and $\{ m_d,m_u,m_e \}$. The sets have the feature that within each of them the…

High Energy Physics - Phenomenology · Physics 2019-07-24 Werner Rodejohann , Ulises Saldaña-Salazar

I define a set of conditions that the most general hierarchical Yukawa mass matrices have to satisfy so that the leading rotations in the diagonalization matrix are a pair of (2,3) and (1,2) rotations. In addition to Fritzsch structures,…

High Energy Physics - Phenomenology · Physics 2010-11-23 Andrija Rasin

Building an organized Yukawa structure of quarks and leptons is an essential mission to understand fermion mass hierarchy and flavor mixing in particle physics. Inspired by the similarity of CKM and PMNS mixings, a common mass pattern for…

High Energy Physics - Phenomenology · Physics 2023-11-16 Ying Zhang