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Related papers: Family Unification on an Orbifold

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A realistic SU(3)_C x SU(3)_W unified theory is constructed with a TeV sized extra dimension compactified on the orbifold S_1/Z_2, leaving only the standard model gauge group SU(3)_C x SU(2)_L x U(1)_Y unbroken in the low energy 4D theory.…

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

In this work, we present a trinification-based grand unified theory incorporating a global $\mathrm{SU}(3)$ family symmetry that after a spontaneous breaking leads to a left-right symmetric model. Already at the classical level, this model…

High Energy Physics - Phenomenology · Physics 2016-10-06 José Eliel Camargo-Molina , António P. Morais , Roman Pasechnik , Jonas Wessén

Supersymmetric gauge models with local horizontal symmetries are known to generate large flavor changing neutral current effects induced by supersymmetry breaking D-terms. We show how the presence of a U(1) gauge symmetry solves this…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. S. Babu , R. N. Mohapatra

The unification of gauge and top Yukawa couplings is an attractive feature of gauge-Higgs unification models in extra-dimensions. This feature is usually considered difficult to obtain based on simple group theory analyses. We reconsider a…

High Energy Physics - Phenomenology · Physics 2018-01-17 Ammar Abdalgabar , Mohammed Omer Khojali , Alan S. Cornell , Giacomo Cacciapaglia , Aldo Deandrea

We do not know why there are three fermion families in the Standard Model (SM), nor can we explain the observed pattern of fermion masses and mixing angles. Standard grand unified theories based on the SU(5) and SO(10) groups fail to shed…

High Energy Physics - Phenomenology · Physics 2020-12-16 Renato M. Fonseca

We consider Yukawa couplings generated by a configuration of intersecting seven-branes in F-theory. In configurations with a single interaction point and no fluxes turned on, the Yukawa matrices have rank one. This is no longer true when…

High Energy Physics - Theory · Physics 2010-07-15 Sergio Cecotti , Miranda C. N. Cheng , Jonathan J. Heckman , Cumrun Vafa

We consider the scenario where all the couplings in the theory are strong at the cut-off scale, in the context of higher dimensional grand unified field theories where the unified gauge symmetry is broken by an orbifold compactification. In…

High Energy Physics - Phenomenology · Physics 2009-09-29 Yasunori Nomura

The purpose of this note is to extend the results obtained in [arXiv:1303.6970] in two ways. First, the six-dimensional F-theory compactifications with U(1) x U(1) gauge symmetry on elliptic Calabi-Yau threefolds, constructed as a…

High Energy Physics - Theory · Physics 2015-06-16 Mirjam Cvetic , Denis Klevers , Hernan Piragua

Unification based on the group SO(10)^3 \times S_3 is studied. Each family has its own SO(10) group, and the S_3 permutes the three families and SO(10) factors. This is the maximal local symmetry for the known fermions. Family unification…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. S. Babu , S. M. Barr , Ilia Gogoladze

In this paper we analyze Yukawa unification in a three family SO(10) SUSY GUT. We perform a global $\chi^2$ analysis and show that SUSY effects do not decouple even though the universal scalar mass parameter at the GUT scale, $m_{16}$, is…

High Energy Physics - Phenomenology · Physics 2016-03-29 Zijie Poh , Stuart Raby

We review the known ways of incorporating and breaking symmetries in a renormalizable way. We summarize the various grand unified theories based on $SU_5, SO_{10}$, and $E_6$ as family enlargement groups. An $SU_5$ model with an $SU_2$…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Ramond

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

If supersymmetry (SUSY) solves the hierarchy problem, then naturalness considerations coupled with recent LHC bounds require non-trivial superpartner flavor structures. Such "Natural SUSY" models exhibit a large mass hierarchy between…

High Energy Physics - Phenomenology · Physics 2015-06-04 Nathaniel Craig , Matthew McCullough , Jesse Thaler

The Standard Model flavor structure can be explained in theories where the fermions are localized on different points in a compact extra dimension. We show that models with two bulk scalars compactified on an orbifold can produce such…

High Energy Physics - Phenomenology · Physics 2014-11-17 Yuval Grossman , Gilad Perez

We construct new supersymmetric SU(5) Grand Unified Models based on Z4 x Z2 orientifolds with intersecting D6-branes. Unlike constructions based on Z2 x Z2 orientifolds, the orbifold images of the three-cycles wrapped by D6-branes…

High Energy Physics - Theory · Physics 2008-11-26 Mirjam Cvetic , Paul Langacker

We propose a theory of flavour based on abelian horizontal gauge symmetries and modular invariances. We construct explicit supergravity models where the scale of the horizontal $U(1)$ symmetry breaking is fixed by the Green-Schwarz…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Dudas , C. Grojean , S. Pokorski , C. A. Savoy

We present a systematic construction of F-theory compactifications with Abelian gauge symmetries in addition to a non-Abelian gauge group G. The formalism is generally applicable to models in global Tate form but we focus on the…

High Energy Physics - Theory · Physics 2013-08-02 Christoph Mayrhofer , Eran Palti , Timo Weigand

A holomorphic vector bundle on a Calabi-Yau threefold, X, with h^{1,1}(X)>1 can have regions of its Kahler cone where it is slope-stable, that is, where the four-dimensional theory is N=1 supersymmetric, bounded by "walls of stability". On…

High Energy Physics - Theory · Physics 2014-11-20 Lara B. Anderson , James Gray , Burt Ovrut

The requirement of Yukawa coupling unification highly constrains the SUSY parameter space. In several SUSY breaking scenarios it is hard to reconcile Yukawa coupling unification with experimental constraints from B(b->s gamma) and the muon…

High Energy Physics - Phenomenology · Physics 2009-11-10 Csaba Balazs , Radovan Dermisek

It is argued that a phenomenologically viable grand unification model from superstring is $SU(3)^3$, the simplest gauge group among the grand unifications of the electroweak hypercharge embedded in semi-simple groups. We construct a…

High Energy Physics - Theory · Physics 2009-11-10 Jihn E. Kim