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We build on a recent paper by Grinstein, Redi and Villadoro, where a see-saw like mechanism for quark masses was derived in the context of spontaneously broken gauged flavour symmetries. The see-saw mechanism is induced by heavy Dirac…

High Energy Physics - Phenomenology · Physics 2011-04-20 Thorsten Feldmann

We construct a left-right symmetric (LRS) model in five dimensions which accounts naturally for the lepton flavor parameters. The fifth dimension is described by an orbifold, S_1/Z_2 times Z'_2, with a typical size of order TeV^{-1}. The…

High Energy Physics - Phenomenology · Physics 2009-11-07 Gilad Perez

We study quark and lepton flavor structures on magnetized $T^2/\mathbb{Z}_2$ twisted orbifold model. There are 6,460 number of flavor models but most of them cannot lead to realistic flavor observables because of the difficulties on…

High Energy Physics - Phenomenology · Physics 2024-03-27 Shota Kikuchi

In orbifold family unification on the basis of $SU(N)$ gauge theory on the six-dimensional space-time $M^4\times T^2/Z_m$ ($m=2, 3, 4, 6$), enormous numbers of models with three families of the standard model matter multiplets are derived…

High Energy Physics - Phenomenology · Physics 2018-09-12 Yuhei Goto , Yoshiharu Kawamura

We give an overview of recent progress in the study of fermion mass and flavor mixing phenomena. Mass matrix ansatze are considered within the SM and SUSY GUTs where some predictive frameworks based on SU(5) and SO(10) are reviewed. We…

High Energy Physics - Phenomenology · Physics 2009-11-11 N. Chamoun , S. Khalil

In non-supersymmetric grand unified models a ``radiative fermion mass hierarchy" can be achieved in which the spectrum of quark and lepton masses is determined entirely by physics at the unification scale, with many relations following from…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Barr

Instead of right-handed neutrino singlets, the standard model is extended to include lepton triplets $(\Sigma^+, \Sigma^0, \Sigma^-)$. Each quark and lepton family may now transform under an anomaly-free $U(1)_X$ gauge symmetry, known…

High Energy Physics - Phenomenology · Physics 2021-03-17 Ernest Ma

We built an extended 2HDM theory with a spontaneously broken $U(1) _{X}$ global symmetry, where the tree level Universal Seesaw Mechanism generates the mass hierarchy of the Standard Model charged fermions and the Zee-Babu mechanism…

High Energy Physics - Phenomenology · Physics 2024-10-25 A. E. Cárcamo Hernández , Diego Restrepo , Ivan Schmidt , Óscar Zapata

Pursuing a bottom-up approach to explore which flavor symmetry could serve as an explanation of the observed fermion masses and mixings, we discuss an extension of the standard model (SM) where the flavor structure for both quarks and…

High Energy Physics - Phenomenology · Physics 2011-05-05 C. Hagedorn , M. Lindner , R. N. Mohapatra

Numerical correlations between fermion masses and mixings could indicate the presence of a flavor symmetry at high energies. In general, the search for these correlations using low-energy data requires an estimate of leading-log radiative…

High Energy Physics - Phenomenology · Physics 2009-10-28 J. A. Aguilar-Saavedra , M. Masip

We present a extension of the 3-3-1 gauge model supplemented by an $A_4$ flavor symmetry and cyclic discrete symmetries, including $Z_2$, $Z_2'$, $Z_3$, $Z_4$, $Z_7$ and $Z_{10}$. The model successfully reproduces the observed SM fermion…

High Energy Physics - Phenomenology · Physics 2025-06-25 A. E. Cárcamo Hernández , D. T. Huong , H. N. Long , Daniel Salinas-Arizmendi

We present a method to identify symmetry groups of the Yukawa sector of the three-Higgs-doublet model and to determine the implication that the symmetry has on the lepton masses and mixing. The method can accommodate different hypotheses…

High Energy Physics - Phenomenology · Physics 2022-09-29 Bartosz Dziewit , Marek Zralek , Joris Vergeest , Piotr Chaber

We present a renormalizable fermion mass model based on the symmetry $Q_4$ that accommodates all fermion masses and mixing angles in both the quark and lepton sectors. It requires the presence of only four SU(2) doublet scalar fields…

High Energy Physics - Phenomenology · Physics 2011-08-12 Alfredo Aranda , Cesar Bonilla , Raymundo Ramos , Alma D. Rojas

The flavor structure of quarks and leptons is not yet fully understood, but it hints a more fundamental theory of non-universal generations. We therefore propose a simple extension of the Standard Model by flipping (i.e., enlarging) the…

High Energy Physics - Phenomenology · Physics 2024-07-09 Duong Van Loi , Phung Van Dong , N. T. Duy , Nguyen Huy Thao

The supersymmetric $SU(6)$ model accompanied by the flavour-blind discrete symmetry $Z_3$ can succesfully deal with such key problems of SUSY GUTs, as are the gauge hierarchy/doublet-triplet splitting, $\mu$-problem and flavour problem. The…

High Energy Physics - Phenomenology · Physics 2008-02-03 Zurab Berezhiani

The problem of quark-lepton families is discussed in the "bottom-up" phenomenological approach to the extensions of the Standard model. It provides the possibility of the {\it Horizontal unification} of the three known families on the basis…

High Energy Physics - Phenomenology · Physics 2013-07-02 Maxim Yu. Khlopov

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 investigate the implications of a seesaw type mass matrix, i.e., $M_f\simeq m_L M_F^{-1} m_R$, for quarks and leptons $f$ under the assumption that the matrices $m_L$ and $m_R$ are common to all flavors (up-/down- and quark-/lepton-…

High Energy Physics - Phenomenology · Physics 2010-11-01 Y. Koide , H. Fusaoka

We construct a flavor model in an anti-SU(5) GUT with a tetrahedral symmetry $A_4$. We choose a basis where $Q_{text{em}}=-\frac13$ quarks and charged leptons are already mass eigenstates. This choice is possible from the $A_4$ symmetry.…

High Energy Physics - Phenomenology · Physics 2020-03-25 Paul H. Frampton , Jihn E. Kim , Se-Jin Kim , Soonkeon Nam

Despite the remarkable success of the Standard Model, the hierarchy and patterns of fermion masses and mixings remain a profound mystery. To address this, we propose a model employing the rank mechanism, where the originally massless quarks…

High Energy Physics - Phenomenology · Physics 2025-02-06 Sudip Jana , Sophie Klett , Manfred Lindner , Rabindra N. Mohapatra