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Related papers: Local SU(5) Unification in 6D from the Heterotic S…

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We present a non-perturbative model of Gauge-Higgs Unification. We consider a five-dimensional pure SU(2) gauge theory with orbifold boundary conditions along the fifth dimension, such that the symmetry is reduced to U(1) at the fixed…

High Energy Physics - Lattice · Physics 2015-06-12 Nikos Irges , Francesco Knechtli , Kyoko Yoneyama

We give a classification of 3-family SO(10) and E_6 grand unification in string theory within the framework of conformal field theory and asymmetric orbifolds. We argue that the construction of such models in the heterotic string theory…

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

In this talk, we discuss an attempt to construct a realistic model of the grand gauge-Higgs unification. We investigate a 5D SU(6) grand gauge-Higgs unification model compactified on an orbifold S^1/Z_2. Ordinary quarks and leptons,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Nobuhito Maru

We study examples of chiral four-dimensional IIB orientifolds with Scherk--Schwarz supersymmetry breaking, based on freely acting orbifolds. We construct a new Z3xZ3' model, containing only D9-branes, and rederive from a more geometric…

High Energy Physics - Theory · Physics 2014-11-18 C. A. Scrucca , M. Serone , M. Trapletti

The form of the most general orbifold breaking of gauge, global and supersymmetries with a single extra dimension is given. In certain theories the Higgs boson mass is ultraviolet finite due to an unbroken local supersymmetry, which is…

High Energy Physics - Theory · Physics 2010-05-28 Riccardo Barbieri , Lawrence J. Hall , Yasunori Nomura

We consider five dimensional (5D) supersymmetric SO(10) compactified on the orbifold $S^1/(Z_2\times Z_2')$ such that the SO(10) gauge symmetry is broken on both fixed points (branes), and the residual gauge symmetry is $SU(3)_c\times…

High Energy Physics - Phenomenology · Physics 2010-11-19 Bumseok Kyae , Chin-Aik Lee , Qaisar Shafi

Intersecting stacks of supersymmetric fractional branes on the Z_6' orientifold may be used to construct the supersymmetric Standard Model. If a,b are the stacks that generate the SU(3)_{colour} and SU(2)_L gauge particles, then, in order…

High Energy Physics - Theory · Physics 2019-08-19 David Bailin , Alex Love

We construct supersymmetric compactifications of E_8 \times E_8 heterotic string theory which realise exactly the massless spectrum of the Minimal Supersymmetric Standard Model (MSSM) at low energies. The starting point is the standard…

High Energy Physics - Theory · Physics 2012-06-08 Volker Braun , Philip Candelas , Rhys Davies , Ron Donagi

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 analyze the phenomenology of the Higgs sector in a 5D model compactified on an $S_1/Z_2$ orbifold with a compactification scale $M_C \sim {\mathcal O}(TeV)$ where supersymmetry breaking is localized on a brane at one of the fixed points.…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Di Clemente , S. F. King , D. A. J. Rayner

The strategy for assigning $Z_{4R}$ parity in the string compactification is presented. For the visible sector, an anti-SU(5) (flipped-SU(5)) grand unification (GUT) model with three families is used to reduce the number of representations…

High Energy Physics - Phenomenology · Physics 2021-07-21 Jihn E. Kim

We present a Z_6 orbifold compactification of the E_8xE_8 heterotic string which leads to the (supersymmetric) Standard Model gauge group and matter content. The quarks and leptons appear as three 16-plets of SO(10), whereas the Higgs…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wilfried Buchmuller , Koichi Hamaguchi , Oleg Lebedev , Michael Ratz

We provide a general overview of the current state of the art in four dimensional three generation model building proposals - using intersecting D-brane toroidal compactifications [without fluxes] of IIA, IIB string theories - which have…

High Energy Physics - Theory · Physics 2007-05-23 Christos Kokorelis

The heterotic $SU(3)$ system, also known as the Hull--Strominger system, arises from compactifications of heterotic string theory to six dimensions. This paper investigates the local structure of the moduli space of solutions to this system…

Differential Geometry · Mathematics 2025-03-31 Hannah de Lázari , Jason D. Lotay , Henrique Sá Earp , Eirik Eik Svanes

Heterotic orbifolds provide promising constructions of MSSM-like models in string theory. We investigate the connection of such orbifold models with smooth Calabi-Yau compactifications by examining resolutions of the T^6/Z6-II orbifold…

High Energy Physics - Theory · Physics 2011-02-15 Stefan Groot Nibbelink , Johannes Held , Fabian Ruehle , Michele Trapletti , Patrick K. S. Vaudrevange

We construct a three family flipped SU(5) model from the heterotic string theory compactified on the $\Z_{12-I}$ orbifold with one Wilson line. The gauge group is $\rm SU(5)\times U(1)_X\times U(1)^2\times[SU(2)\times SO(10)\times…

High Energy Physics - Theory · Physics 2008-11-26 Jihn E. Kim , Bumseok Kyae

The conventional supersymmetric grand unified theories suffer from two serious problems, the large mass splitting between doublet and triplet Higgs multiplets, and the too long lifetime of the proton. A unification model based on a…

High Energy Physics - Phenomenology · Physics 2009-11-07 Y. Imamura , T. Watari , T. Yanagida

We study the viability of five-dimensional gauge theories as candidates for the origin of the Higgs field and its mechanism for spontaneous symmetry breaking. Within the framework of lattice field theory, we consider the simplest model of…

High Energy Physics - Lattice · Physics 2015-10-28 Maurizio Alberti , Nikos Irges , Francesco Knechtli , Graham Moir

We search for supersymmetric standard model realizations with extra singlets and extra $ U(1)$ using the heterotic string compactification on the $ Z_{6-II}$ orbifold with two Wilson lines. We analyze the vacuum restabilization mechanism…

High Energy Physics - Phenomenology · Physics 2014-11-20 Marc Chemtob , Pierre Hosteins

Using Z3 asymmetric orbifolds in heterotic string theory, we construct N=1 SUSY three-generation models with the standard model gauge group SU(3)_C \times SU(2)_L \times U(1)_Y and the left-right symmetric group SU(3)_C \times SU(2)_L…

High Energy Physics - Theory · Physics 2015-06-17 Florian Beye , Tatsuo Kobayashi , Shogo Kuwakino