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We propose a realistic theory based on the $\mathrm{SU(3)_c \otimes SU(3)_L \otimes SU(3)_R \otimes U(1)_{X}}$ gauge group which requires the number of families to match the number of colors. In the simplest realization neutrino masses…

High Energy Physics - Phenomenology · Physics 2017-01-24 Mario Reig , José W. F. Valle , C. A. Vaquera-Araujo

We review in a systematic way how anomaly free $SU(3)_c\otimes SU(3)_L\otimes U(1)_x$ models without exotic electric charges can be constructed, using as basis closed sets of fermions which includes each one the particles and antiparticles…

High Energy Physics - Phenomenology · Physics 2022-09-28 Richard H. Benavides , Yithsbey Giraldo , Luis Muñoz , William A. Ponce , Eduardo Rojas

A Z_2 orbifold compactification of the heterotic string is considered. The resulting 6D GUT groups can be SO(16) or E_7 times SU(2) plus some hidden sector groups. The N=4 supersymmetry is reduced to N=2. In particular, the SO(16) 6D model…

High Energy Physics - Theory · Physics 2009-11-07 Kang-Sin Choi , Jihn E. Kim

In the context of the left-right symmetric gauge group [SU(6)]$^3\times$ Z$_3$ which unifies nongravitational forces with flavors, we analyze the generational seesaw mechanism. At tree level we get…

High Energy Physics - Phenomenology · Physics 2009-08-26 William A. Ponce , Arnulfo Zepeda , Ricardo Gaitan Lozano

It has recently been realized that a large class of Calabi-Yau models in which the VEV of the gauge connection is not set equal to the spin connection of the Calabi-Yau manifold are valid classical solutions of string theory. We provide…

High Energy Physics - Theory · Physics 2009-10-07 Shamit Kachru

We build a supersymmetric version with $SU(3)_C\otimes SU(2)_L\otimes U(1)_{Y^\prime}\otimes U(1)_{B-L}$ gauge symmetry, where $Y^\prime$ is a new charge and $B$ and $L$ are the usual baryonic and leptonic numbers. The model has three…

High Energy Physics - Phenomenology · Physics 2017-06-14 J. C. Montero , V. Pleitez , M. C. Rodriguez , B. L. Sánchez-Vega

We search for the three-generation standard-like and/or Pati-Salam models from the $SO(32)$ heterotic string theory on smooth, quotient complete intersection Calabi-Yau threefolds with multiple line bundles, each with structure group…

High Energy Physics - Theory · Physics 2018-05-10 Hajime Otsuka

We construct a supersymmetric (SUSY) $SU(5)$ model with the flavor symmetry $S_4\times Z_3\times Z_4$. Three generations of adjoint matter fields are introduced to generate the neutrino masses via the combined type I and type III see-saw…

High Energy Physics - Phenomenology · Physics 2011-02-21 Gui-Jun Ding

We show that the recently constructed 5-dimensional supersymmetric $S^1/(Z_2\times Z_2')$ orbifold GUT models allow an appealing explanation of the observed hierarchical structure of the quark and lepton masses and mixing angles. Flavor…

High Energy Physics - Phenomenology · Physics 2014-11-17 Lawrence Hall , John March-Russell , Takemichi Okui , David Smith

We investigate a gauge theory realization of non-Abelian discrete flavor symmetries and apply the gauge enhancement mechanism in heterotic orbifold models to field-theoretical model building. Several phenomenologically interesting…

High Energy Physics - Phenomenology · Physics 2015-02-04 Florian Beye , Tatsuo Kobayashi , Shogo Kuwakino

We study an extension of the gauge group SU(3)_c X SU(2)_L X U(1)_Y of the standard model to the symmetry group SU(3)_c X SU(4)_L X U(1)_X (3-4-1 for short). This extension provides an interesting attempt to answer the question of family…

High Energy Physics - Phenomenology · Physics 2014-11-20 Stiven Villada , Luis A. Sanchez

We propose low energy 6-dimensional N=2 supersymmetric SU(6) models on $M^4\times T^2/(Z_2)^3$ and $M^4\times T^2/(Z_2)^4$, where the orbifold $SU(3)_C\times SU(3)$ model can be embedded on the boundary 4-brane. For the zero modes, the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jing Jiang , Tianjun Li , Wei Liao

Generalizing the recent work on three-family Type I compactifications, we classify perturbative Type I vacua obtained via compactifying on the T^6/Z_2 X Z_2 X Z_3 orbifold with all possible Wilson lines. In particular, we concentrate on…

High Energy Physics - Theory · Physics 2009-10-31 Zurab Kakushadze , S. -H. Henry Tye

In this paper we consider the gauge theory living on the world-volume of a stack of N D3-branes of Type 0B/\Omega' I_6(-1)^{F_{L}} and of its orbifolds C^2/Z_2 and C^3/(Z_2 x Z_2). The gauge theories obtained in the three cases are a brane…

High Energy Physics - Theory · Physics 2008-11-26 P. Di Vecchia , A. Liccardo , R. Marotta , F. Pezzella

Motivated by D-brane scenarios, we consider a non-supersymmetric model based on the gauge symmetry U(3)_CxU(3)_LxU(3)_R$ which is equivalent to the SU(3)^3 ``trinification'' model supplemented by three U(1)s. Two U(1) combinations are…

High Energy Physics - Phenomenology · Physics 2009-11-11 G. K. Leontaris , J. Rizos

We study flat directions and soft scalar masses using a $Z_3$ orbifold model with $SU(3) \times SU(2) \times U(1)$ gauge group and extra gauge symmetries including an anomalous $U(1)$ symmetry. Soft scalar masses contain $D$-term…

High Energy Physics - Phenomenology · Physics 2009-10-28 Yoshiharu Kawamura , Tatsuo Kobayashi , Tohru Komatsu

We consider a Yang-Mills-Higgs theory with the gauge group SU(3) broken to its center Z(3) by two scalar fields in the adjoint representation and obtain new Z(3) strings asymptotic configurations with the gauge field and magnetic field in…

High Energy Physics - Theory · Physics 2016-11-17 Marco A. C. Kneipp , Paulo J. Liebgott

We study an effective gauge theory whose gauge group is a semidirect product $G = G_c \rtimes \mathit{\Gamma}$ with $G_c$ and $\mathit{\Gamma}$ being a connected Lie group and a finite group, respectively. The semidirect product is defined…

High Energy Physics - Phenomenology · Physics 2010-11-03 Chuichiro Hattori , Mamoru Matsunaga , Takeo Matsuoka , Kenichi Nakanishi

We construct a 6D supergravity theory which emerges as intermediate step in the compactification of the heterotic string to the supersymmetric standard model in four dimensions. The theory has N=2 supersymmetry and a gravitational sector…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Buchmüller , C. Lüdeling , J. Schmidt

We propose a model which unifies the Left-Right symmetry with the $SU(3)_L$ gauge group, called flipped trinification, and based on the $SU(3)_C\otimes SU(3)_L\otimes SU(3)_R\otimes U(1)_X$ gauge group. The model inherits the interesting…

High Energy Physics - Phenomenology · Physics 2018-05-23 P. V. Dong , D. T. Huong , Farinaldo S. Queiroz , José W. F. Valle , C. A. Vaquera-Araujo