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By considering the 3-3-1 and the left-right symmetric models as low energy effective theories of the $SU(3)_C\otimes SU(3)_L\otimes SU(3)_R$~(for short $[SU(3)]^3$) gauge group, alternative versions of these models are found. The new…

High Energy Physics - Phenomenology · Physics 2017-01-18 Oscar Rodríguez , Richard H. Benavides , William A. Ponce , Eduardo Rojas

We present $Z_3$ orbifold compactifications of $E_8\times E_8^\prime$ heterotic string with three Wilson lines, resulting to the maximum number of SU(3) factors. Here, all the matter spectrums are in the SU(3) trits($\equiv $ three…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jihn E. Kim

It was recently suggested that the reported anomalies in $R_b$ and $R_c$ can be interpreted as the effect of a heavy vector boson that couples to quarks and is universally decoupled from leptons. We examine how an extra gauge boson with…

High Energy Physics - Phenomenology · Physics 2011-01-25 Alon E. Faraggi , Manuel Masip

We present a 3-3-1 model as a subgroup of SU(4)PS X SU(4)L+R gauge symmetry with symmetry-breaking pattern SU(4)->SU(3) X U(1) for both SU(4) groups. A Pleitez-Frampton type of 3C-3L-1X model is obtained with charged heavy leptons and…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sutapa Sen , Aparna Dixit

We construct a family-unified model on a Z_2xZ_2 orbifold in five dimensions. The model is based on a supersymmetric SU(7) gauge theory. The gauge group is broken by orbifold boundary conditions to a product of grand unified SU(5) and…

High Energy Physics - Phenomenology · Physics 2009-11-10 Zhenyu Han , Witold Skiba

We study the possibility of family unification on the basis of SU(N) gauge theory on the 6-dimensional space-time, $M^4\times T^2/Z_N$. We obtain enormous numbers of models with three families of SU(5) matter multiplets and those with three…

High Energy Physics - Phenomenology · Physics 2013-09-25 Yuhei Goto , Yoshiharu Kawamura , Takashi Miura

With the apparent discovery of the Higgs boson, the Standard Model has been confirmed as the theory accounting for all sub-atomic phenomena. This observation lends further credence to the perturbative unification in Grand Unified Theories…

High Energy Physics - Theory · Physics 2014-03-26 Laura Bernard , Alon E Faraggi , Ivan Glasser , John Rizos , Hasan Sonmez

We consider N=1 supersymmetric gauge theories based on the group SU(N)_1 x SU(N)_2 x ... x SU(N)_k with matter content (N,N*,1,...,1) + (1,N,N*,..., 1) + >... + (N*,1,1,...,N) as candidates for the unification symmetry of all particles. In…

High Energy Physics - Phenomenology · Physics 2015-05-14 S. Heinemeyer , E. Ma , M. Mondragon , G. Zoupanos

We explore the possibility of string theories in only four spacetime dimensions without any additional compactified dimensions. We show that, provided the theory is defined in curved spacetime that has a cosmological interpration, it is…

High Energy Physics - Theory · Physics 2008-11-26 Itzhak Bars

We discuss the first string theory examples of three generation non-supersymmetric SU(5) and {\em flipped} SU(5) GUTS, which break to the Standard model at low energy, without extra matter and/or gauge group factors. Our GUT examples are…

High Energy Physics - Theory · Physics 2016-09-06 Minos Axenides , Emmanuel Floratos , Christos Kokorelis

We study dilaton stabilization in heterotic string models. By utilizing the asymmetric orbifold construction, we construct an explicit three-generation model whose matter content in the visible sector is the supersymmetric standard model…

High Energy Physics - Theory · Physics 2016-08-03 Florian Beye , Tatsuo Kobayashi , Shogo Kuwakino

We construct a four dimensional chiral N=1 space-time supersymmetric perturbative Type I vacuum corresponding to a compactification on a toroidal Z_2 X Z_2 X Z_3 orbifold with a discrete Wilson line. This model is non-perturbative from the…

High Energy Physics - Theory · Physics 2009-12-30 Zurab Kakushadze

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

I introduce a class of string constructions based on asymmetric orbifolds leading to level two models. In particular, I derive in detail various models with gauge groups $E_6$ and SO(10), including a four generation $E_6$ model with two…

High Energy Physics - Theory · Physics 2009-10-30 Jens Erler

We present a supersymmetric (SUSY) model based on trinification $[\mathrm{SU}(3)]^3$ and family $\mathrm{SU}(3)_\mathrm{F}$ symmetries embedded into a maximal subgroup of $\mathrm{E}_8$, where the sectors of light Higgs bosons and leptons…

High Energy Physics - Phenomenology · Physics 2017-05-03 José E. Camargo-Molina , António P. Morais , Astrid Ordell , Roman Pasechnik , Marco O. P. Sampaio , Jonas Wessén

We introduce a new heterotic Standard Model which has precisely the spectrum of the Minimal Supersymmetric Standard Model (MSSM), with no exotic matter. The observable sector has gauge group SU(3) x SU(2) x U(1). Our model is obtained from…

High Energy Physics - Theory · Physics 2008-11-26 Vincent Bouchard , Ron Donagi

From the string partition function, we discuss the mass-shell and GSO projection conditions valid for Kaluza-Klein (KK) as well as massless states in the heterotic string theory compactified on a nonprime orbifold. Based on the obtained…

High Energy Physics - Phenomenology · Physics 2009-02-02 Bumseok Kyae

The $Z_2\times Z_2$ heterotic string orbifold gives rise to a large space of phenomenological three generation models that serves as a testing ground to explore how the Standard Model of particle physics may be incorporated in a theory of…

High Energy Physics - Theory · Physics 2021-01-26 Alon E. Faraggi , Viktor G. Matyas , Benjamin Percival

For a given complex n-fold M we present an explicit construction of all complex (n+1)-folds which are principal holomorphic T2-fibrations over M. For physical applications we consider the case of M being a Calabi-Yau 2-fold. We show that…

High Energy Physics - Theory · Physics 2009-11-07 Edward Goldstein , Sergey Prokushkin

Starting from an N=1 supersymmetric electric gauge theory with the gauge group SU(N_c) x SU(N_c') x SU(N_c'') with fundamentals for each gauge group, the bifundamentals, a symmetric flavor and a conjugate symmetric flavor for SU(N_c), we…

High Energy Physics - Theory · Physics 2009-11-05 Changhyun Ahn