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Related papers: A Heterotic Standard Model

200 papers

In a previous publication, arXiv:1106.4804, we have found 200 models from heterotic Calabi-Yau compactifications with line bundles, which lead to standard models after taking appropriate quotients by a discrete symmetry and introducing…

High Energy Physics - Theory · Physics 2015-06-04 Lara B. Anderson , James Gray , Andre Lukas , Eran Palti

We consider a class of models with extra complex scalars that are charged under both the Standard Model and a hidden strongly coupled $SU(N)_H$ gauge sector, and discuss the scenarios where the new scalars are identified as the messenger…

High Energy Physics - Phenomenology · Physics 2017-07-07 Cheng-Wei Chiang , Sichun Sun , Fang Ye

The Standard Model of electroweak interactions is shown to include a gauge theory for the observed scalar and pseudoscalar mesons. This is done by exploiting the consequences of embedding the SU(2)left X U(1) group into the chiral group of…

High Energy Physics - Phenomenology · Physics 2009-10-28 B. Machet

The matter spectrum of the MSSM, including three right-handed neutrino supermultiplets and one pair of Higgs-Higgs conjugate superfields, can be obtained by compactifying the E_{8} x E_{8} heterotic string and M-theory on Calabi-Yau…

High Energy Physics - Theory · Physics 2015-05-19 Michael Ambroso , Burt A. Ovrut

The observable sector of the "minimal heterotic standard model" has precisely the matter spectrum of the MSSM: three families of quarks and leptons, each with a right-handed neutrino, and one Higgs-Higgs conjugate pair. In this paper, it is…

High Energy Physics - Theory · Physics 2009-11-11 Volker Braun , Yang-Hui He , Burt A. Ovrut

The motivation for Calabi-Yau-like compactifications of the weakly coupled $E_8\otimes E_8$ heterotic string theory, its particle spectrum and the issue of dilaton stabilization are briefly reviewed. Modular invariant models for hidden…

High Energy Physics - Phenomenology · Physics 2009-11-11 Mary K. Gaillard

We propose an extension of the Standard Model inspired by the E_8 x E_8 Heterotic String. In order that a reasonable effective Lagrangian is presented we neglect everything else other than the ten-dimensional N=1 supersymmetric Yang-Mills…

High Energy Physics - Phenomenology · Physics 2011-09-08 Nikos Irges , George Zoupanos

Symmetric vacua of heterotic M-theory, characterized by vanishing cohomology classes of individual sources in the three-form Bianchi identity, are analyzed on smooth Calabi-Yau three-folds. We show that such vacua do not exist for…

High Energy Physics - Theory · Physics 2016-12-28 Andre Lukas , Burt A. Ovrut

We describe a new kind of transition between topologically distinct $N=2$ type II Calabi--Yau vacua through points with enhanced non-abelian gauge symmetries together with fundamental charged matter hypermultiplets. We connect the…

High Energy Physics - Theory · Physics 2009-10-30 P. Berglund , S. Katz , A. Klemm , P. Mayr

We show that four-dimensional N=2 supersymmetric SU(n) gauge theory for n>2 necessarily contains vacua with mutually non-local massless dyons, using only analyticity of the effective action and the weak coupling limit of the moduli space of…

High Energy Physics - Theory · Physics 2009-10-28 Philip C. Argyres , Michael R. Douglas

Additional Abelian gauge interactions are generic to string compactifications. In heterotic string models, gauge coupling unification of such forces and other gauge interactions is natural due to their common origin. In this letter we study…

High Energy Physics - Phenomenology · Physics 2019-07-10 Yessenia Olguin-Trejo , Omar Perez-Figueroa , Ricardo Perez-Martinez , Saul Ramos-Sanchez

This talk adapts the available formalism to study a class of heterotic M-theory vacua with SO(10) grand unification group. Compactification to four dimensions with N = 1 supersymmetry is achieved on a torus fibered Calabi-Yau 3-fold Z = X /…

High Energy Physics - Theory · Physics 2007-05-23 Richard S. Garavuso

We construct six stack D6-brane vacua (non-supersymmetric) that have at low energy exactly the standard model (with right handed neutrinos). The construction is based on D6-branes intersecting at angles in $D = 4$ type toroidal orientifolds…

High Energy Physics - Theory · Physics 2014-11-18 Christos Kokorelis

We consider a quark-lepton symmetry model of unification of the strong and electromagnetic interactions. The model has the gauge group $SU(4)\times U(1)_{Y}$ and the minimal Higgs structure consisting of one complex quartet of scalar…

High Energy Physics - Phenomenology · Physics 2009-04-09 E. K. Loginov

This work considers the remarkable suggestion that the three families of quarks and leptons may be unified, together with the Higgs and gauge fields of the Standard Model (SM), into a single "particle", namely the $\textbf{248}$ vector…

High Energy Physics - Phenomenology · Physics 2020-10-12 Alfredo Aranda , Francisco J. de Anda , Stephen F. King

In previous papers, we introduced a heterotic standard model and discussed its basic properties. The Calabi-Yau threefold has, generically, three Kahler and three complex structure moduli. The observable sector of this vacuum has the…

High Energy Physics - Theory · Physics 2010-02-03 Volker Braun , Yang-Hui He , Burt A. Ovrut , Tony Pantev

Based on the Z_{12-I} orbifold compactification of the heterotic string theory, we construct a flipped-SU(5) model with three families of the standard model matter and ingredients for dynamical supersymmetry breaking. The doublet-triplet…

High Energy Physics - Phenomenology · Physics 2009-12-31 Ji-Haeng Huh , Jihn E. Kim , Bumseok Kyae

In this work we present an extension of the Standard model as a local gauge group SU(3)c x SU(4)L x U(1)X embedded in SU(3)c x SU(4)L x U(1)Y0 x U(1)B-L gauge group. The U(1)Y0 gauge symmetry is introduced to obtain an anomaly-free three-…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sutapa Sen Aparna Dixit

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 low energy effective theory of the N=1 supersymmetric SU(5) gauge theory with chiral superfields in the 5* and 10 representations is constructed. Instead of postulating the confinement of SU(5) (confining picture), only the confinement…

High Energy Physics - Theory · Physics 2009-10-30 Noriaki Kitazawa