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Related papers: Large Top Quark Yukawa Coupling and Horizontal Sym…

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In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the exception of neutrino masses. The hierarchies and apparent regularities among the quark and lepton masses are, however, otherwise a mystery.…

High Energy Physics - Phenomenology · Physics 2022-11-07 Sudip Jana , Sophie Klett , Manfred Lindner

Based on the hierarchy exhibited by quarks masses at low energies, we assume that Yukawa couplings of up and down quarks are related by $Y_u\propto Y_d^2$ at grand unification scales. This ansatz gives rise to a symmetrical CKM matrix at…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. González , S. R. Juárez W. , P. Kielanowski , G. López Castro

Measurement of the top-Yukawa coupling is important to understand the fermion mass generation mechanism and dynamics of electroweak symmetry breaking. We discuss the top quark anomalous couplings which can be described by higher dimensional…

High Energy Physics - Phenomenology · Physics 2009-02-16 Shinya Kanemura , Koichi Matsuda , Daisuke Nomura , Koji Tsumura

In a model with a gauge group $G_{SM}\otimes U(1)_X$, where $G_{SM} \equiv SU(3)_C \otimes SU(2)_L \otimes U(1)_Y$ is the standard model gauge group and $U(1)_X$ is a horizontal local gauge symmetry, we propose a radiative generation of the…

High Energy Physics - Phenomenology · Physics 2016-08-15 E. García , A. Hernández-Galeana , D. Jaramillo , W. A. Ponce , A. Zepeda

We consider the problem of the ordinary charged fermion mass patterns in the framework of a version of the 3-3-1 electroweak gauge model, which includes charged heavy leptons. The masses of the top and the bottom quarks are given at the…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. D. Tonasse

A non anomalous horizontal $U(1)_H$ gauge symmetry can be responsible for the fermion mass hierarchies of the minimal supersymmetric standard model. Imposing the consistency conditions for the absence of gauge anomalies yields the following…

High Energy Physics - Phenomenology · Physics 2009-10-31 Jesus M. Mira , Enrico Nardi , Diego A. Restrepo

We suggest a simple grand unified theory where the fifth dimensional coordinate is compactified on an $S_1/(Z_2 \times Z_2')$ orbifold. This model is based on the supersymmetric flipped $SU(5) \times U(1)$ grand unified theory, which can…

High Energy Physics - Phenomenology · Physics 2014-11-17 N. Haba , Y. Shimizu , Tomoharu Suzuki , Kazumasa Ukai

We study the predictions of the simplest SU(5) grand unified model within the framework of minimal supergravity, including constraints from the radiative breaking of electroweak symmetry. As a consequence of the unification of the $b$-quark…

High Energy Physics - Phenomenology · Physics 2011-07-19 H. Baer , M. Drees , C. Kao , M. Nojiri , X. Tata

In recent papers a microscopic model for the SM Higgs mechanism has been proposed, and an idea how to determine the 24 quark and lepton masses of all 3 generations has emerged in that framework. This idea is worked out in detail here by…

High Energy Physics - Phenomenology · Physics 2015-06-19 Bodo Lampe

In the scenarios with heavy top squarks, mass parameters of the Higgs field must be fine-tuned due to a large logarithmic correction to the soft scalar mass. We consider a new possibility that the top Yukawa coupling is small above TeV…

High Energy Physics - Phenomenology · Physics 2009-11-11 Tatsuo Kobayashi , Hiroaki Nakano , Haruhiko Terao

Radiatively generated fermion masses without tree level Yukawa couplings are re-analyzed within supersymmetric models. Special emphasis is given to the possible appearance of color and charge breaking vacua. Several scenarios in which the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Francesca Borzumati , Glennys Farrar , Nir Polonsky , Scott Thomas

A natural gradual extension of the idea of Grand Unification is to attempt to relate the gauge and Yukawa couplings; Gauge-Yukawa Unification (GYU). However, within the framework of renormalizable field theories, there exists no realistic…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jisuke Kubo , Myriam Mondragon , Marek Olechowski , George Zoupanos

In a supersymmetric model with hierarchical squark masses we analyze a pattern of flavour symmetry breaking centered on the special role of the top Yukawa coupling and, by extension, of the full Yukawa couplings for the up-type quarks. For…

High Energy Physics - Phenomenology · Physics 2011-02-15 Riccardo Barbieri , Enrico Bertuzzo , Marco Farina , Paolo Lodone , Dmitry Zhuridov

The generation of the fermion mass hierarchy in the standard model of particle physics is a long-standing puzzle. The recent discoveries from neutrino physics suggests that the mixing in the lepton sector is large compared to the quark…

High Energy Physics - Phenomenology · Physics 2008-11-26 David McKeen , Jonathan L. Rosner , Arun M. Thalapillil

We construct a model in which the hierarchies of the quark and lepton masses and mixing are explained by the $\Gamma_6^\prime$ modular flavor symmetry. The hierarchies are realized by the Froggatt-Nielsen-like mechanism due to the residual…

High Energy Physics - Phenomenology · Physics 2023-07-06 Yoshihiko Abe , Tetsutaro Higaki , Junichiro Kawamura , Tatsuo Kobayashi

In this talk, I present a new framework to understand the long-standing fermion mass hierarchy puzzle. We extend the Standard Model gauge symmetry by an extra local U(1)_S symmetry, broken spontaneously at the electroweak scale. All the SM…

High Energy Physics - Phenomenology · Physics 2015-05-14 S. Nandi

M-theory compactified on a $G_2$ manifold with resolved $E_8$ singularities realizes 4d $\mathcal{N} = 1$ supersymmetric gauge theories coupled to gravity with three families of Standard Model fermions. Beginning with one $E_8$ singularity,…

High Energy Physics - Theory · Physics 2021-07-28 Eric Gonzalez , Gordon Kane , Khoa Dang Nguyen , Malcolm J. Perry

We explore a mechanism for generating the Yukawa hierarchies by displacing the left- and right-handed components of the Standard Model fermions in a higher-dimensional space. We find a unique configuration of displacements which fits all…

High Energy Physics - Phenomenology · Physics 2009-10-31 Eugene A. Mirabelli , Martin Schmaltz

In the Standard Model, there is the single Higgs field, $\phi$, which gives rise to constituent quark and lepton masses. The Yukawa coupling is a highly complex set of $3 \times 3$ matrices, resulting in many textures of quark and lepton…

High Energy Physics - Phenomenology · Physics 2015-06-22 Ngee-Pong Chang

We discuss a supersymmetric unified model based on a product gauge group SU(5)\times SU(5)\times SU(5), where the gauge symmetry breaking is achieved without the adjoint or higher-dimensional Higgs field, and the doublet-triplet splitting…

High Energy Physics - Phenomenology · Physics 2007-05-23 Takehiko Asaka , Y. Takanishi