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The discrete symmetry D_12 at the electroweak scale is used to fix the quark and lepton mixing angles. At the leading order, the Cabbibo angle theta_C is 15^o, and the PMNS matrix is of a bi-dodeca-mixing form giving the Solar-neutrino…

High Energy Physics - Phenomenology · Physics 2011-03-01 Jihn E. Kim , Min-Seok Seo

The standard electroweak model with Dirac neutrinos is extended by way of the principles of electroweak quark-lepton symmetry and weak topological-charge confinement to account for quark-lepton charge relations which, if not accidental, are…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernesto A. Matute

Unification ideas motivate the formulation of field equations on an extended spin space. Demanding that the Poincare symmetry be maintained, one derives scalar symmetries that are associated with flavor and gauge groups. Boson and fermion…

High Energy Physics - Theory · Physics 2009-11-07 J. Besprosvany

We show that all mixing angles are determined, within experimental uncertainty, by a product of SU(2) horizontal symmetries intimately linked to the algebra of weak neutral currents. This concerns: on one hand, the three quark mixing…

High Energy Physics - Phenomenology · Physics 2007-06-13 Quentin Duret , Bruno Machet

We discuss electroweak constraints on TeV scale extensions of the standard model. To obtain model-independent results, effective theory approach is adopted. Constraints are given on arbitrary linear combinations of a set of dimension-6…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhenyu Han

A possibility of 5D gauge unification of $SU(2)_L \times U(1)_Y$ in $SU(3)_W$ is examined. The orbifold compactification allows fixed points where $SU(2)_L\times U(1)_Y$ representations can be assigned. We present a few possibilities which…

High Energy Physics - Theory · Physics 2010-11-19 Hyung Do Kim , Jihn E. Kim , Hyun Min Lee

We discuss extension of the electroweak gauge group to $SU(3)_L \times SU(3)_R \times U(1)_{XL} \times U(1)_{XR}$. This adds new leptons to the familiar 331-model. The explanation for three light quark-lepton families remains but new…

High Energy Physics - Phenomenology · Physics 2025-01-20 Claudio Corianò , Paul H. Frampton , Dario Melle

We construct a five dimensional supersymmetric SO(10)$\times$D$_3$ grand unified model with an $S^1/(Z_2 \times Z^\prime_2)$ orbifold as the extra dimension. The orbifold breaks half of the supersymmetry and breaks the SO(10) gauge symmetry…

High Energy Physics - Phenomenology · Physics 2009-11-10 Hyung Do Kim , Stuart Raby , Leslie Schradin

We study electroweak symmetry breaking involving the seesaw mechanism of quark condensation. These models produce a composite Higgs boson involving the left-handed top quark, yet the top mass arises naturally at the observed scale. We…

High Energy Physics - Phenomenology · Physics 2009-09-11 R. Sekhar Chivukula , Bogdan A. Dobrescu , Howard Georgi , Christopher T. Hill

We consider $SU(3)_{C}\times SU(2)_{AL}\times SU(2)_{BL}\times U(1)_{Y}$ as the low-energy subgroup of supersymmetric $SU(3)^{6}$ unification. This may imply small deviations from quark-lepton universality at the TeV scale, as allowed by…

High Energy Physics - Phenomenology · Physics 2009-11-11 Qing-Hong Cao , Shao-Long Chen , Ernest Ma , G. Rajasekaran

Electroweak symmetry can be naturally broken by observed quark and gauge fields in various extra-dimensional configurations. No new {\it fundamental} fields are required below the quantum gravitational scale ($\sim$ 10 - 100 TeV). We…

High Energy Physics - Phenomenology · Physics 2009-10-31 Hsin-Chia Cheng , Bogdan A. Dobrescu , Christopher T. Hill

We construct SU(5) SUSY GUT in 5D compactified on S^1/Z_2 orbifold where the matter fields are living in the five dimensional bulk. SU(5) symmetry is broken down to the Standard Model gauge group by the orbifold projection which…

High Energy Physics - Phenomenology · Physics 2017-08-23 Archil Kobakhidze

We review models of electroweak symmetry breaking due to new strong interactions at the TeV energy scale and discuss the prospects for their experimental tests. We emphasize the direct observation of the new interactions through high-energy…

High Energy Physics - Phenomenology · Physics 2011-01-13 T. L. Barklow , G. Burdman , R. S. Chivukula , B. A. Dobrescu , P. S. Drell , N. Hadley , W. B. Kilgore , M. E. Peskin , J. Terning , D. R. Wood

We study the lowest dimensional typical and atypical representations of SU(5/3) superalgebra as a possible unified gauge theory having a natural SU(5) subalgebra with SU(3) extra structure, which will be used to accommodate three…

High Energy Physics - Theory · Physics 2015-06-15 Chang-Ho Kim , Seung Kook Kim , Young-Jai Park

The recent discovery of nonzero $\theta_{13}$ (equal to Cabbibo angle $\theta_C$ up to a factor of $\sqrt{2}$), the masses of supersymmetric particles $\gapp$ TeV from LHC data, and the sum of three active neutrino masses $\sum_i…

High Energy Physics - Phenomenology · Physics 2013-11-15 Abhijit Samanta

We extend the littlest modular seesaw to a Grand Unified scenario based on $SU(5)$ endowed with three modular $S_4$ symmetries. We leverage symmetry protected zeroes in the leptonic and down quark sectors to suppress deviations to the…

High Energy Physics - Phenomenology · Physics 2023-09-29 Ivo de Medeiros Varzielas , Steve F. King , Miguel Levy

The electroweak symmetry may be broken by a composite Higgs which arises naturally as a bound state of the top quark if the standard model gauge fields and fermions propagate in extra dimenions. The top quark mass and the Higgs mass can be…

High Energy Physics - Phenomenology · Physics 2009-10-31 Hsin-Chia Cheng

Recently, a mechanism for electroweak symmetry breaking (EWSB) was discussed, in which the scale of EWSB is set by the scale of an additional dimension R ~ Tev^-1. The mechanism involves supersymmetry, but broken in such a fashion that high…

High Energy Physics - Phenomenology · Physics 2007-05-23 Neal Weiner

The capability of string theories to reproduce at low energy the observed pattern of quark and lepton masses and mixing angles is examined, focusing the attention on orbifold constructions, where the magnitude of Yukawa couplings depends on…

High Energy Physics - Theory · Physics 2009-10-22 J. A. Casas , F. Gómez , C. Muñoz

We have recently proposed a simple SU(5) theory with an adjoint fermionic multiplet on top of the usual minimal spectrum. This leads to the hybrid scenario of both type I and type III seesaw and it predicts the existence of the fermionic…

High Energy Physics - Phenomenology · Physics 2008-11-26 Borut Bajc , Miha Nemevsek , Goran Senjanovic
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