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Related papers: String-Inspired Special Grand Unification

200 papers

The $SO(11)$ gauge-Higgs grand unification in the Randall-Sundrum warped space is presented. The 4D Higgs field is identified as the zero mode of the fifth dimensional component of the gauge potentials, or as the fluctuation mode of the…

High Energy Physics - Phenomenology · Physics 2016-06-24 Atsushi Furui , Yutaka Hosotani , Naoki Yamatsu

Renormalizable SO(10) grand unified theories (GUTs), extended by $O(N_g)_F$ family gauge symmetry, generate minimal supersymmetric Standard Model flavour structure dynamically via vacuum expectation values of "Yukawon" Higgs multiplets. For…

High Energy Physics - Phenomenology · Physics 2015-06-17 Charanjit S. Aulakh , Charanjit K. Khosa

We extend the unitary groups beyond the ${\rm SU}(5)$ and ${\rm SU}(6)$ to look for possible grand unified theories that give rise to three-generational Standard Model fermions without the simple repetition. By demanding asymptotic free…

High Energy Physics - Phenomenology · Physics 2022-02-03 Ning Chen

Requiring that supersymmetric SU(5) and SU(6) grand unifications in the heterotic string theory must have 3 chiral families, adjoint (or higher representation) Higgs fields in the grand unifiedgauge group, and a non-abelian hidden sector,…

High Energy Physics - Theory · Physics 2009-10-30 Zurab Kakushadze , S. -H. Henry Tye

After a brief review of the flavour problem we present a new predictive framework based on SUSY $SO(10)$ theory, where the first family plays a role of the mass unification point. The inter-family hierarchy is first generated in a sector of…

High Energy Physics - Phenomenology · Physics 2009-09-25 Zurab G. Berezhiani

We discuss the anomalous U(1) gauge symmetry as a mechanism of generating the grand-unification scale. We conclude that unification to a simple group cannot be realized unless some parameters are ``tuned'', and that models with product…

High Energy Physics - Phenomenology · Physics 2009-09-29 K. -I. Izawa , Kiichi Kurosawa , Yasunori Nomura , T. Yanagida

We construct non-minimal GUT local models in the F-theory configuration. The gauge group on the bulk G_S is one rank higher than the GUT gauge group. The line bundles on the curves are non-trivial to break G_S down to the GUT gauge groups.…

High Energy Physics - Theory · Physics 2011-01-21 Ching-Ming Chen , Yu-Chieh Chung

Use of the AdS/CFT correspondence to arrive at phenomenological gauge field theories is dicussed, focusing on the orbifolded case without supersymmetry. An abelian orbifold with the finite group $Z_{p}$ can give rise to a $G = SU(N)^p$…

High Energy Physics - Theory · Physics 2007-05-23 Paul H. Frampton

In the first part of the talk, I explain what empirical evidence points to the need for having an effective grand unification-like symmetry possessing the symmetry SU(4)-color in 4D. If one assumes the premises of a future predictive theory…

High Energy Physics - Phenomenology · Physics 2009-11-11 Jogesh C. Pati

We study supersymmetric unified models with three fermion generations based on the gauge group $SO(10)$ and require Gauge-Yukawa Unification, i.e., a renormalization group invariant functional relationship among the gauge and Yukawa…

High Energy Physics - Phenomenology · Physics 2011-01-27 Jisuke Kubo , Myriam Mondragon , Shigeyuki Shoda , George Zoupanos

Higher dimensional grand unified theories, with gauge symmetry breaking by orbifold compactification, possess SU(5) breaking at fixed points, and do not automatically lead to tree-level gauge coupling unification. A new framework is…

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

Grand Unified Theories predict relationships between the GUT-scale quark and lepton masses. Using new data in the context of the MSSM, we update the values and uncertainties of the masses and mixing angles for the three generations at the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Graham Ross , Mario Serna

We construct a minimal example of a supersymmetric grand unified model in a toroidal compactification of type I string theory with magnetized D9-branes. All geometric moduli are stabilized in terms of the background internal magnetic fluxes…

High Energy Physics - Theory · Physics 2008-11-26 Ignatios Antoniadis , Alok Kumar , Binata Panda

We suggest simple models which produce the suitable fermion mass hierarchies and flavor mixing angles based on the supersymmetric SO(10) grand unified theory in 6 dimensions compactified on a T^2/Z_2 orbifold. The gauge and Higgs fields…

High Energy Physics - Phenomenology · Physics 2009-11-07 N. Haba , T. Kondo , Y. Shimizu

In the context of the standard SUSY GUT scenario, we present a detailed analysis of the softly broken finite supersymmetric grand unified theory. The model, albeit non-minimal, remains very rigid due to the requirement of finiteness. It is…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. I. Kazakov , M. Yu. Kalmykov , I. N. Kondrashuk , A. V. Gladyshev

Grand Unified Theories (GUTs) are a very well motivated extensions of the Standard Model (SM), but the landscape of models and possibilities is overwhelming, and different patterns can lead to rather distinct phenomenologies. In this work…

High Energy Physics - Phenomenology · Physics 2017-09-08 Frank F. Deppisch , Tomas E. Gonzalo , Lukas Graf

In the standard model matter fields form complete representations of a grand unified group whereas Higgs fields belong to incomplete `split' multiplets. This remarkable fact is naturally explained by `local grand unification' in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Wilfried Buchmuller , Koichi Hamaguchi , Oleg Lebedev , Michael Ratz

We exploit the recently developed software package LieART to show that SU(N) grand unified theories with chiral fermions in mixed tensor irreducible representations can lead to standard model chiral fermions without additional light exotic…

High Energy Physics - Phenomenology · Physics 2015-08-19 Robert P. Feger , Thomas W. Kephart

The Weinberg angle is an important parameter in Grand Unified Theories (GUT) as its size is crucially influenced by the assumption of unification. In scenarios with different steps of symmetry breaking, in particular in models that involve…

High Energy Physics - Phenomenology · Physics 2020-06-10 Christoph Englert , David J. Miller , Dumitru Dan Smaranda

After a brief review of the motivations for grand unification, I discuss the main challenges facing realistic SUSY GUT model building. Achieving doublet-triplet splitting without fine--tuning is chief among them. Symmetry breaking should…

High Energy Physics - Phenomenology · Physics 2011-11-10 K. S. Babu