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We approach the Minimum Supersymmetric Standard Model (MSSM) from an E_6 GUT by using the spectral cover construction and non-abelian gauge fluxes in F-theory. We start with an E_6 singularity unfolded from an E_8 singularity and obtain E_6…

High Energy Physics - Theory · Physics 2011-03-31 Ching-Ming Chen , Yu-Chieh Chung

We study an extension of the supersymmetric standard model with four families and gauged horizontal symmetry $SU(4)_H$, in which R parity automatically follows as a consequence of gauge invariance and of the field content of the model.…

High Energy Physics - Phenomenology · Physics 2016-09-01 Zurab Berezhiani , Enrico Nardi

We introduce gauge theories based on a class of disconnected gauge groups, called principal extensions. Although in this work we focus on 4d theories with N=2 SUSY, such construction is independent of spacetime dimensions and supersymmetry.…

High Energy Physics - Theory · Physics 2019-03-27 Antoine Bourget , Alessandro Pini , Diego Rodriguez-Gomez

We propose a $SU(5) \times U(1)_X \times U(1)_{PQ}$ model, where $U(1)_X$ is the generalization of the $B-L$ (baryon minus lepton number) gauge symmetry and $U(1)_{PQ}$ is the global Peccei-Quinn (PQ) symmetry. There are four fermions…

High Energy Physics - Phenomenology · Physics 2021-10-04 Nobuchika Okada , Digesh Raut , Qaisar Shafi

We present a model of partial compositeness arising as the IR limit of a SU(4) gauge theory with only fermionic matter. This group is one of the most promising ones among a handful of possible choices allowing a symmetry breaking pattern…

High Energy Physics - Phenomenology · Physics 2015-06-19 Gabriele Ferretti

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

We include fermions to the model proposed in hep-th/0606021, and obtain a renormalizable 4-dimensional SU(N) gauge theory which spontaneously generates fuzzy extra dimensions and behaves like Yang-Mills theory on M^4 \times S^2. We find a…

High Energy Physics - Theory · Physics 2009-04-17 Harold Steinacker , George Zoupanos

The reasons behind the gauge symmetry of the Standard Model, U(1)xSU(2)xSU(3), are still unsettled. One obvious feature is the low dimensionality of all its subgroups. Under certain conditions, a negative answer to the question "why not…

High Energy Physics - Phenomenology · Physics 2017-09-25 Felipe J. Llanes-Estrada , Guillermo Garcia Fernandez , Jesus Guerrero Rojas

We present exact non-perturbative solutions to chiral gauge theories based on the $E_6$ gauge group and several matter fermions in the fundamental $\bf{27}$-dimensional representation. They are obtained when supersymmetric versions are…

High Energy Physics - Theory · Physics 2025-05-14 Andrew Goh , Hitoshi Murayama , Gup Singh , Bethany Suter , Jason Wong

In this paper we discuss $SU(5)^{3}$ with cyclic symmetry as a possible grand unified theory (GUT). The basic idea of such a tri-unification is that there is a separate $SU(5)$ for each fermion family, with the light Higgs doublet(s)…

High Energy Physics - Phenomenology · Physics 2024-06-27 Mario Fernández Navarro , Stephen F. King , Avelino Vicente

We construct gauge theory of SU(3)xSU(2)xU(1) by spectral cover from F-theory and ask how the Standard Model is extended under minimal assumptions on Higgs sector. For the requirement on different numbers between Higgs pairs and matter…

High Energy Physics - Theory · Physics 2015-05-30 Kang-Sin Choi

The $N=4$ SU(2)$_k$ superconformal algebra has the global automorphism of SO(4) $\approx$ SU(2)$\times$SU(2) with the {\it left} factor as the Kac-Moody gauge symmetry. As a consequence, an infinite set of independent algebras labeled by…

High Energy Physics - Theory · Physics 2015-06-26 Satoshi Matsuda , Yukitaka Ishimoto

We construct the SU(5) and SO(10) models from F-theory. Turning on the U(1) fluxes, we can break the SU(5) gauge symmetry down to the Standard Model (SM) gauge symmetry, and break the SO(10) gauge symmetry down to the SU(3)_C X SU(2)_L X…

High Energy Physics - Theory · Physics 2010-04-29 Tianjun Li

We study the left-right asymmetric model based on SU(3)_C \otimes SU(2)_L \otimes SU(3)_R \otimes U(1)_X gauge group, which improves the theoretical and phenomenological aspects of the known left-right symmetric model. This new gauge…

High Energy Physics - Phenomenology · Physics 2017-04-26 P. V. Dong , D. T. Huong , D. V. Loi , N. T. Nhuan , N. T. K. Ngan

In the Standard Model the hypercharges of quarks and leptons are not determined by the gauge group $SU(3)_{\rm c} \times SU(2)_{\rm L} \times U(1)_{\rm Y}$ alone. We show that, if we choose the semidirect product group $[SU(3)_{\rm c}…

High Energy Physics - Phenomenology · Physics 2011-02-01 Chuichiro Hattori , Mamoru Matsunaga , Takeo Matsuoka

We consider the unification of gauge, Higgs as well as the matter fields in a 6D N=2 supersymmetric SU(8) gauge theory. The gauge symmetry SU(8) is broken down to SU(4) x SU(2)_L x SU(2)_R x U(1)^2 in 4D through T^2/Z_6 orbifold…

High Energy Physics - Phenomenology · Physics 2010-11-19 Ilia Gogoladze , Yukihiro Mimura , S. Nandi

Family Replicated Gauge Group models of the type SU(n)^N\times SU(m)^N, (SMG)^3 and (SMG\times U(1)_{B-L})^3 are reviewed, where SMG=SU(3)_{c}\times SU(2)_{L}\times U(1)_{Y} is the gauge symmetry group of the Standard Model, $B$ is the…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. D. Froggatt , L. V. Laperashvili , H. B. Nielsen , Y. Takanishi

In a scheme originally proposed by M. Gell-Mann, and subsequently shown to be realized at the SU(3)xU(1) stationary point of maximal gauged SO(8) supergravity by N. Warner and one of the present authors, the 48 spin 1/2 fermions of the…

High Energy Physics - Theory · Physics 2015-04-01 Krzysztof A. Meissner , Hermann Nicolai

We present a Pisarski-Wilczek stability analysis of SU(4) gauge theory coupled simultaneously to fermions charged under the fundamental and two-index antisymmetric representations of the gauge group. We carry out the calculation to one loop…

High Energy Physics - Phenomenology · Physics 2018-04-04 Daniel C. Hackett

We consider the extended electroweak gauge group SU(2)_1 \times SU(2)_2 \times U(1)_Y where the first and second families of fermions couple to SU(2)_1 while the third family couples to SU(2)_2. Bounds based an precision electroweak…

High Energy Physics - Phenomenology · Physics 2007-05-23 David J. Muller , Satya Nandi
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