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We propose a top and bottom seesaw model with partial composite top and bottom quarks. Such composite quarks and topcolor gauge bosons are bound states from supersymmetric strong dynamics by Seiberg duality. Supersymmetry breaking also…

High Energy Physics - Phenomenology · Physics 2015-06-11 Csaba Balazs , Tianjun Li , Fei Wang , Jin Min Yang

The combination of flavor symmetries with grand unification is considered: GUT $ \times$ flavor . To accommodate three generations the flavor group SO(3) is used. All fermions transform as 3-vectors under this group. The Yukawa couplings…

High Energy Physics - Phenomenology · Physics 2011-01-07 Berthold Stech

A mechanism is suggested by which the dynamics of confinement could be responsible for the fermion mass matrix. In this approach the large top quark Yukawa coupling is generated naturally during confinement, while those of the other quarks…

High Energy Physics - Phenomenology · Physics 2009-10-28 M. J. Strassler

In this letter we study the low-energy phenomenology and cosmological implications of supersymmetric grand unified theory with asymmetric flavor structure, which is suggested by the recent observation of fermion masses and mixing angles.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kenzo Inoue , Kentaro Kojima , Koichi Yoshioka

The calculation of Yukawa couplings in F-theory GUTs is developed. The method is applied to the top and bottom Yukawa couplings in an SU(5) model of fermion masses based on family symmetries coming from the SU(5)_\perp factor in the…

High Energy Physics - Theory · Physics 2011-03-03 G. K. Leontaris , G. G. Ross

We propose a composite grand unified theory to study the anomalies in the semileptonic $B$ decays. We show a simple group containing the custodial and Standard Model gauge symmetries, that can deliver a set of composite pseudo…

High Energy Physics - Phenomenology · Physics 2019-05-01 Leandro Da Rold , Federico Lamagna

The effective bottom Yukawa couplings are analyzed for the minimal supersymmetric extension of the Standard Model at two-loop accuracy within SUSY-QCD. They include the resummation of the dominant corrections for large values of tg(beta).…

High Energy Physics - Phenomenology · Physics 2011-06-24 David Noth , Michael Spira

We consider the NMSSM extended to include one vector-like family of quarks and leptons. If (some of) these vector-like matter particles, as the Higgs doublets, have Yukawa couplings to the singlet S that exceed unity at about the same scale…

High Energy Physics - Phenomenology · Physics 2016-07-20 Riccardo Barbieri , Dario Buttazzo , Lawrence J. Hall , David Marzocca

In cases of both abelian and nonabelian gauge groups, we study the Higgs mechanism in the topologically massive gauge theories in an arbitrary space-time dimension. We show that when the conventional Higgs potential coexists with a…

High Energy Physics - Theory · Physics 2011-07-19 Ichiro Oda

A unified mass matrix model of quarks and leptons with a seesaw-type form $M_f=m M_F^{-1} m$ is proposed on the basis of a non-standard Higgs scenario. The matrix $m$ is provided by U(3)-family nonet bosons $\phi$, and the matrix $M_F$ is a…

High Energy Physics - Phenomenology · Physics 2008-02-03 Yoshio Koide , Hideo Fusaoka

Recently one of the authors proposed a dual theory of a Supersymmetric Standard Model (SSM), in which it is naturally understood that at least one quark (the top quark) should be heavy, i.e., almost the same order as the weak scale, and the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Nobuhiro Maekawa , Joe Sato

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 2007-05-23 Satoru Kaneko , Hideyuki Sawanaka , Takaya Shingai , Morimitsu Tanimoto , Koichi Yoshioka

It is shown that the mechanism to soften contributions of top squarks to the Higgs mass, discussed in "Supersoft Top Squarks", Phys. Rev. Lett. 125, no.15, 151801 (2020), is very similar, with identical result in the leading order, to the…

High Energy Physics - Phenomenology · Physics 2021-12-14 Radovan Dermisek

We study the flavor structure of 5D warped models that provide a dual description of a composite pseudo-Goldstone Higgs. We first carefully re-examine the flavor constraints on the mass scale of new physics in the standard…

High Energy Physics - Phenomenology · Physics 2009-01-06 Csaba Csaki , Adam Falkowski , Andreas Weiler

We analyze a composite Higgs model based on the confining $SU(3)$ gauge theory with $N_f = 8$ Dirac fermions in the fundamental representation. This gauge theory has been studied on the lattice and shown to be well described by a dilaton…

High Energy Physics - Phenomenology · Physics 2021-05-19 Thomas Appelquist , James Ingoldby , Maurizio Piai

In the light of recent discovery of a very heavy top quark, we reexamine the top quark condensate model proposed by Miransky, Tanabashi and Yamawaki (MTY) and by Nambu. We first review the original MTY formulation based on the ladder…

High Energy Physics - Phenomenology · Physics 2009-10-28 Koichi Yamawaki

I discuss LHC signatures of the charged Higgs boson of the MSSM, focussing mainly on the case of the charged Higgs boson being heavier than top quark.

High Energy Physics - Phenomenology · Physics 2007-05-23 D. P. Roy

The main production mechanism for supersymmetric Higgs particles at hadron colliders crucially depends on the size of their Yukawa couplings to bottom quarks. For sufficiently large tan(beta) the total cross section for some of the neutral…

High Energy Physics - Phenomenology · Physics 2007-10-15 Alexander Mück

The gauge-Higgs unification theory identifies the zero mode of the extra dimensional component of the gauge field as the usual Higgs doublet. Since this degree of freedom is the Wilson line phase, the Higgs does not have the mass term nor…

High Energy Physics - Phenomenology · Physics 2009-11-10 Naoyuki Haba , Kazunori Takenaga , Toshifumi Yamashita

Finite Unified Theories (FUTs) are N=1 supersymmetric Grand Unified Theories (GUTs) which can be made finite to all-loop orders, leading to a drastic reduction in the number of free parameters. By confronting the predictions of SU(5) FUTs…

High Energy Physics - Phenomenology · Physics 2008-10-07 S. Heinemeyer , M. Mondragon , G. Zoupanos