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Related papers: SO(10) Unification in Non-Commutative Geometry

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We propose a simple supersymmetric SO(10) GUT model with only doublet Higgs scalars. The fermion mass problem is naturally solved by a new one-loop diagram. R-parity is conserved implying a stable LSP which can explain the dark matter of…

High Energy Physics - Phenomenology · Physics 2009-11-10 Utpal Sarkar

A new SO(10) unified model is proposed based on a one step breaking of SO(10) to the Standard Model gauge group $SU(3)\times SU(2)\times U(1)_Y$ using a single 144 of Higgs. The symmetry breaking occurs when the SU(5) 24-plet component of…

High Energy Physics - Phenomenology · Physics 2009-11-11 K. S. Babu , Ilia Gogoladze , Pran Nath , Raza M. Syed

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

We present a minimal renormalizable non-supersymmetric SO(10) grand unified model with a symmetry breaking sector consisting of Higgs fields in the 54_H + 126_H + 10_H representations. This model admits a single intermediate scale…

High Energy Physics - Phenomenology · Physics 2015-10-21 K. S. Babu , S. Khan

The formalism of non-commutative geometry of A. Connes is used to construct models in particle physics. The physical space-time is taken to be a product of a continuous four-manifold by a discrete set of points. The treatment of Connes is…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. H. Chamseddine , G. Felder , J. Fröhlich

The hypercharges of the fermions are not uniquely determined in SO(10) grand unification, but rather depend upon which linear combination of the two U(1) subgroups of SO(10) > SU(3) X SU(2) X U(1) X U(1) remains unbroken. We show that, in…

High Energy Physics - Phenomenology · Physics 2009-10-30 J. Lykken , T. Montroy , S. Willenbrock

We investigate quartification models in five dimensions, with the fifth dimension forming an $S^1/Z_2\times Z_2'$ orbifold. The orbifold construction is combined with a boundary Higgs sector to break the quartified gauge group directly to a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alison Demaria , Kristian L. McDonald

We consider a phenomenologically viable SO(10) grand unification model of the unification scale $M_G$ around $10^{16} $ GeV which reproduces the MSSM at low energy and allows perturbative calculations up to the Planck scale $M_P$ or the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Darwin Chang , Takeshi Fukuyama , Yong-Yeon Keum , Tatsuru Kikuchi , Nobuchika Okada

(N=2)-superspace without torsion is described, which is equivalent to an 8-space with a discrete internal subspace. A number and a character of ties determine now an internal symmetry group, while in the supersymmetrical models this one is…

High Energy Physics - Theory · Physics 2007-05-23 Michael A. Ivanov

Grand gauge-Higgs unification of five dimensional SU(6) gauge theory on an orbifold S^1/Z_2 with localized gauge kinetic terms is discussed. The Standard model (SM) fermions on one of the boundaries and some massive bulk fermions coupling…

High Energy Physics - Phenomenology · Physics 2020-10-28 Nobuhito Maru , Yoshiki Yatagai

A simple supersymmetric SO(10) GUT in five dimensions is considered. The fifth dimension is compactified on the $S^1/(Z_2\times Z_2^\prime)$ orbifold possessing two inequivalent fixed points. In our setup, all matter and Higgs multiplets…

High Energy Physics - Phenomenology · Physics 2008-11-26 Takeshi Fukuyama , Nobuchika Okada

The fermionic sector of the Standard Model of Elementary Particles emerges as the low energy limit of a single fermionic field freely propagating in a higher dimensional background. The local geometrical framework is obtained by enforcing…

High Energy Physics - Theory · Physics 2007-05-23 P. Maraner

Geometrical analysis of a new type of Unified Field Theoretical models follow the guidelines of previous works of the authors is presented. These new unified theoretical models are characterized by an underlying hypercomplex structure, zero…

High Energy Physics - Theory · Physics 2012-07-10 Diego Julio Cirilo-Lombardo

In this talk, we present a minimal viable scenario that unifies the gauge symmetries of the Standard Model (SM) and their breaking sector. Our Gauge-Higgs Grand Unification setup employs 5D warped space with a $SU(6)$ bulk gauge field that…

High Energy Physics - Phenomenology · Physics 2021-09-30 Andrei Angelescu , Andreas Bally , Simone Blasi , Florian Goertz

E6 grand unification combines the Standard Model matter and Higgs states in the single 27 representation. I discuss how the E6 structure underlies the quasi-realistic free fermion heterotic-string models. E6 -> SO(10) X U(1) breaking is…

High Energy Physics - Theory · Physics 2011-07-19 Alon E. Faraggi

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

Gauge coupling unification and the stability of the Higgs vacuum are among two of the cherished features of low-energy supersymmetric models. Putting aside questions of naturalness, supersymmetry might only be realised in nature at very…

High Energy Physics - Phenomenology · Physics 2018-09-19 Sebastian A. R. Ellis , Tony Gherghetta , Kunio Kaneta , Keith A. Olive

Gauge-Higgs grand unification is formulated. By extending $SO(5) \times U(1)_X$ gauge-Higgs electroweak unification, strong interactions are incorporated in $SO(11)$ gauge-Higgs unification in the Randall-Sundrum warped space. Quarks and…

High Energy Physics - Phenomenology · Physics 2015-11-06 Yutaka Hosotani , Naoki Yamatsu

The scheme previously proposed by the present authors is modified to incorporate the strong interaction by affording the direct product internal symmetry. We do not need to prepare the extra discrete space for the color gauge group…

High Energy Physics - Theory · Physics 2008-11-26 Yoshitaka Okumura , Katsusada Morita

$SO(5) \times U(1) \times SU(3)$ gauge-Higgs unification model inspired by $SO(11)$ gauge-Higgs grand unification is constructed in the Randall-Sundrum warped space. The 4D Higgs boson is identified with the Aharonov-Bohm phase in the fifth…

High Energy Physics - Phenomenology · Physics 2019-06-24 Shuichiro Funatsu , Hisaki Hatanaka , Yutaka Hosotani , Yuta Orikasa , Naoki Yamatsu