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Related papers: Yukawa Interaction from a SUSY Composite Model

200 papers

We present a supersymmetric SU(5) x U(1)_H model, free from gauge anomalies, where the Abelian factor U(1)_H, introduced to account for the hierarchy of fermion masses and mixings, is broken by the same adjoint representations of SU(5) that…

High Energy Physics - Phenomenology · Physics 2010-11-19 Diego Aristizabal , Enrico Nardi

We construct realistic theories in which the Higgs fields arise from extra dimensional components of higher dimensional gauge fields. In particular, we present a minimal 5D SU(3)_C x SU(3)_W model and a unified 5D SU(6) model. In both cases…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gustavo Burdman , Yasunori Nomura

We analyze the quantum transport equations for supersymmetric electroweak baryogenesis including previously neglected bottom and tau Yukawa interactions and show that they imply the presence of a previously unrecognized dependence of the…

High Energy Physics - Phenomenology · Physics 2009-02-27 Daniel J. H. Chung , Bjorn Garbrecht , Michael J. Ramsey-Musolf , Sean Tulin

We show how the SUSY flavour and CP problems can be solved using gauged SU(3) family symmetry previously introduced to describe quark and lepton masses and mixings, in particular neutrino tri-bimaximal mixing via constrained sequential…

High Energy Physics - Phenomenology · Physics 2009-01-06 Stefan Antusch , Stephen F. King , Michal Malinsky

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

We study the origin of fermion mass hierarchy and flavor mixing in the standard model, paying attention to flavor symmetries and fermion kinetic terms. There is a possibility that the hierarchical flavor structure of quarks and charged…

High Energy Physics - Phenomenology · Physics 2019-12-06 Yoshiharu Kawamura

A SU(3) \times SU(2) \times U(1) supersymmetric theory is constructed with a TeV sized extra dimension compactified on the orbifold S^1/(Z_2 \times Z_2'). The compactification breaks supersymmetry leaving a set of zero modes which…

High Energy Physics - Phenomenology · Physics 2009-09-29 Riccardo Barbieri , Lawrence J. Hall , Yasunori Nomura

Fermion masses and mixing angles are studied in an SUSY $SO(10)\times \Delta (48)\times U(1)$ model with small $\tan\beta$. Thirteen parameters involving masses and mixing angles in the quark and charged lepton sector are successfully…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. C. Chou , Y. L Wu

We discuss some recent developments in SUSY Grand Unified Theories based on the gauge group SO(10). Considering renormalisable Yukawa couplings, we present ways to accommodate quark and lepton masses and and mixings.

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Grimus , H. Kuhbock

We study a number of models, based on a non-Abelian discrete group, that successfully reproduce the simple and predictive Yukawa textures usually associated with U(2) theories of flavor. These models allow for solutions to the solar and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alfredo Aranda , Christopher D. Carone , Richard F. Lebed

We revisit a recent solution to the flavor hierarchy problem based on the paradigm that Yukawa couplings are, rather than fundamental constants, effective low energy couplings radiatively generated by interactions in a hidden sector of the…

High Energy Physics - Phenomenology · Physics 2018-03-29 Emidio Gabrielli , Luca Marzola , Martti Raidal

We construct an orbifold model in which all the standard model particles are unified in a gauge multiplet in higher dimensional supersymmetric gauge theory. We find that a flavor symmetry has to remain in four dimensions due to the discrete…

High Energy Physics - Phenomenology · Physics 2009-03-12 Yukihiro Mimura

We investigate the confining phase vacua of supersymmetric $Sp(2\NC)$ gauge theories that contain matter in both fundamental and antisymmetric representations. The moduli spaces of such models with $\NF=3$ quark flavors and $\NA=1$…

High Energy Physics - Theory · Physics 2009-10-30 Peter Cho , Per Kraus

The localized fermions on the intersection curve $\Sigma$ of D7-branes, are connected to a N=2 supersymmetric quantum mechanics algebra. Due to this algebra the fields obey a global U(1) symmetry. This symmetry restricts the proton decay…

High Energy Physics - Theory · Physics 2015-05-28 V. K. Oikonomou

The consequences of assuming the third-generation Yukawa couplings are all large and comparable are studied in the context of the minimal supersymmetric extension of the standard model. General aspects of the RG evolution of the parameters,…

High Energy Physics - Phenomenology · Physics 2011-01-27 R. Rattazzi , U. Sarid

Gauge-Yukawa Unification (GYU) yields a functional relation among the gauge and Yukawa couplings, and it may follow from the usual Grand Unification if it is supplemented with some additional principles. Postulating the principles of…

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

We argue that the discovery of neutrino mass effects at Super-Kamiokande implies a clear logical chain leading from the Standard Model, through the MSSM and the recently developed Minimal Left Right Supersymmetric models with a…

High Energy Physics - Phenomenology · Physics 2009-10-31 Charanjit S. Aulakh

We define a new class of $Z'$ models with neutral flavor-changing interactions at tree level in the down-quark sector. They are related in an exact way to elements of the quark mixing matrix due to an underlying flavored $U(1)'$ gauge…

High Energy Physics - Phenomenology · Physics 2015-07-17 Alejandro Celis , Javier Fuentes-Martin , Martin Jung , Hugo Serodio

We interpret anomalies, deviations, from the standard model as being in fact due to effects not given by perturbation, because the top Yukawa coupling is after all so large that not by perturbation effects become important. Most of the…

High Energy Physics - Phenomenology · Physics 2019-05-02 Colin D. Froggatt , Holger Bech Nielsen

We consider the most general renormalizable chiral Yukawa model with $SU(3)_{\rm color}$ replaced by $SU(N_c)$, $SU(2)_{\rm L}$ replaced by $SU(N_w )$ and $U(1)_{Y}$ replaced by $U(1)^{N_w -1}$ in the limit $N_c \rightarrow\infty$, $N_w…

High Energy Physics - Lattice · Physics 2009-10-22 George Bathas , Herbert Neuberger