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Related papers: Family Replication in the Dual Standard Model

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We find the spectrum of magnetic monopoles produced in the symmetry breaking SU(5) to [SU(3)\times SU(2)\times U(1)']/Z_6 by constructing classical bound states of the fundamental monopoles. The spectrum of monopoles is found to correspond…

High Energy Physics - Theory · Physics 2009-10-30 Hong Liu , Tanmay Vachaspati

The present theory is based on the assumption that at the very small (Planck scale) distances our space-time is discrete, and this discreteness influences on the Planck scale physics. Considering our (3+1)-dimensional space-time as a…

High Energy Physics - Theory · Physics 2014-11-18 L. V. Laperashvili , H. B. Nielsen , D. A. Ryzhikh

The aim of the present talk is to show that monopoles cannot play any role in the Standard Model (SM) and in its usual extensions up to the Planck scale: $M_{Pl}=1.22\cdot 10^{19}$ GeV, because they have a huge charge and are completely…

High Energy Physics - Theory · Physics 2007-05-23 L. Laperashvili , H. B. Nielsen

Family Replicated Gauge Group models of the type SU(n)^N\times SU(m)^N, (SMG)^3 and (SMG\times U(1)_{B-L})^3 are reviewed, where SMG=SU(3)_{c}\times SU(2)_{L}\times U(1)_{Y} is the gauge symmetry group of the Standard Model, $B$ is the…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. D. Froggatt , L. V. Laperashvili , H. B. Nielsen , Y. Takanishi

The observed replication of fermions in three families is undoubtedly a reflection of a deeper symmetry underlying the standard model. In this paper we investigate one very elementary possibility, that physics above the grand unification…

High Energy Physics - Phenomenology · Physics 2009-10-22 Michael Joyce , Neil Turok

Models with fermions in bifundamental representations can lead naturally to family unification as opposed to family replication. Such models typically predict (exotic) color singlet states with fractional electric charge, and magnetic…

High Energy Physics - Phenomenology · Physics 2010-10-27 Thomas W. Kephart , Chin-Aik Lee , Qaisar Shafi

We investigate all spherically symmetric fundamental monopole solutions with fixed topological charge in the SU(5) --> SU(3)xSU(2)xU(1)/Z_3xZ_2 symmetry breaking. We find that there is three-fold replication of the monopoles. The three…

High Energy Physics - Theory · Physics 2010-11-19 Levon Pogosian , Daniele A. Steer , Tanmay Vachaspati

In this letter, we introduce a new approach to formulate the family structure of the standard model. Trying to mimic the highly contrained representation structure of the standard model while extending the symmetry, we propose a…

High Energy Physics - Phenomenology · Physics 2009-10-28 Otto C. W. Kong

Peering in from the outside, $\mathbb{A} := \mathbb{R}\otimes\mathbb{C}\otimes\mathbb{H}\otimes\mathbb{O}$ looks to be an ideal mathematical structure for particle physics. It is 32 $\mathbb{C}$-dimensional: exactly the size of one full…

High Energy Physics - Phenomenology · Physics 2022-09-28 N. Furey , M. J. Hughes

If a family symmetry exists for the quarks and leptons, the Higgs sector is expected to be enlarged to be able to support the transformation properties of this symmetry. There are however three possible generic ways (at tree level) of…

High Energy Physics - Phenomenology · Physics 2009-11-11 Ernest Ma

Considering our (3+1)-dimensional space-time as, in some way, discrete or l attice with a parameter $a=\lambda_P$, where $\lambda_P$ is the Planck length, we have investigated the additional contributions of lattice artifact monopoles to…

High Energy Physics - Theory · Physics 2014-11-18 L. V. Laperashvili , H. B. Nielsen , D. A. Ryzhikh

We reconsider a class of heterotic string theories studied in 1989, based on tensor products of N=2 minimal models with asymmetric simple current invariants. We extend this analysis from (2,2) and (1,2) spectra to (0,2) spectra with SO(10)…

High Energy Physics - Theory · Physics 2014-11-20 B. Gato-Rivera , A. N. Schellekens

We review the possibility that the Supersymmetric Standard Model arises from orbifold constructions of the E_8 x E_8 Heterotic Superstring, and the phenomenological properties that such a model should have. In particular, trying to solve…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Munoz

We discuss F-theory SU(5) GUTs in which some or all of the quark and lepton families are assigned to different curves and family symmetry enforces a leading order rank one structure of the Yukawa matrices. We consider two possibilities for…

High Energy Physics - Phenomenology · Physics 2014-11-21 S. F. King , G. K. Leontaris , G. G. Ross

In family unification models, all three families of quarks and leptons are grouped together into an irreducible representation of a simple gauge group, thus unifying the Standard Model gauge symmetries and a gauged family symmetry. Large…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , S. M. Barr , Bumseok Kyae

We examine the problem of constructing three generation free fermionic string models with grand unified gauge groups. We attempt the construction of $G\times G$ models, where $G$ is a grand unified group realized at level 1. This structure…

High Energy Physics - Theory · Physics 2009-10-28 D. Finnell

In this talk I outline work done in collaboration with R.J. Zhang and T. Kobayashi. We show how to construct the equivalent of three family orbifold GUTs in five dimensions from the heterotic string. I focus on one particular model with…

High Energy Physics - Theory · Physics 2016-09-06 Stuart Raby

We consider realistic F-theory GUT models based on discrete family symmetries $A_4$ and $S_3$, combined with $SU(5)$ GUT, comparing our results to existing field theory models based on these groups. We provide an explicit calculation to…

High Energy Physics - Phenomenology · Physics 2015-06-22 Athanasios Karozas , Stephen F. King , George K. Leontaris , Andrew K. Meadowcroft

In spite of its many successes, the Standard Model makes many empirical assumptions in the Higgs and fermion sectors for which a deeper theoretical basis is sought. Starting from the usual gauge symmetry $u(1) \times su(2) \times su(3)$…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. M. Chan , S. T. Tsou

The embedding in SU(4)xSU(3)xSU(3) of the well studied gauge groups SU(4)xSU(2)xSU(2) and SU(3)xSU(3)xSU(3) naturally leads to family unification as opposed to simple family replication. An inescapable consequence is the predicted existence…

High Energy Physics - Phenomenology · Physics 2011-05-12 Thomas W. Kephart , Qaisar Shafi
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