English
Related papers

Related papers: Orbifold Breaking of 3-3-1 Model

200 papers

We propose a stringy mechanism whereby a large hierarchy between symmetry breaking scales is generated. This mechanism is based upon the existence of a fifth dimension compactified on a segment. We focus on a simple supersymmetric model…

High Energy Physics - Theory · Physics 2009-10-30 Ph. Brax , Neil Turok

We describe the basic features of model building in the context of intersecting D-branes. As an example, a D-brane inspired construction with U(3)_C X U(3)_L X U(3)_R gauge symmetry is proposed -which is the analogue of the Trinification…

High Energy Physics - Phenomenology · Physics 2009-09-29 G. K. Leontaris J. Rizos

We consider the compactification of a Yang-Mills theory on a three-dimensional nilmanifold. The compactification generates a Yang-Mills theory in four space-time dimensions, coupled to a specific scalar sector. The compactification geometry…

High Energy Physics - Phenomenology · Physics 2022-04-20 Aldo Deandrea , Fabio Dogliotti , Dimitrios Tsimpis

A model of gauge-mediated supersymmetry breaking is constructed in which the low-energy physics depends on a single dynamical scale. Strong coupling dynamics of gauge theories plays an important role, in particular through its effects on…

High Energy Physics - Phenomenology · Physics 2016-08-25 Ann Nelson , Matthew J. Strassler

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

In an SU(2) lattice gauge theory with a Z2 orbifolded extra dimension, the new symmetry which is called as a stick symmetry is useful in understanding the bulk transition. We discuss the relation with the Fradkin-Shenker's phase diagram as…

High Energy Physics - Lattice · Physics 2010-12-14 Michika Murata , Hiroto So , Kazunori Takenaga

A review of orbifold geometry is given, followed by a review of the construction of four-dimensional heterotic string models by compactification on a six-dimensional Z_3 orbifold. Particular attention is given to the details of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Joel Giedt

We construct two SU(5) models on the space-time $M^4 \times T^2/(Z_2 \times Z_2^{\prime})$ where the gauge and Higgs fields are in the bulk and the Standard Model fermions are on the brane at the fixed point or line. For the zero modes, the…

High Energy Physics - Theory · Physics 2009-11-07 Tianjun Li

We study the constraints on models with extra dimensions arising from local anomaly cancellation. We consider a five-dimensional field theory with a U(1) gauge field and a charged fermion, compactified on the orbifold S^1/(Z_2 x Z_2'). We…

High Energy Physics - Theory · Physics 2009-11-07 C. A. Scrucca , M. Serone , L. Silvestrini , F. Zwirner

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 construct a compactification of the heterotic string on an orbifold T^6/Z_6 leading to the standard model spectrum plus vector--like matter. The standard model gauge group is obtained as an intersection of three SO(10) subgroups of E_8.…

High Energy Physics - Phenomenology · Physics 2010-11-19 Wilfried Buchmuller , Koichi Hamaguchi , Oleg Lebedev , Michael Ratz

A unification of left-right $\rm{SU}(3)_\rm{L}\times \rm{SU}(3)_\rm{R}$, colour $\rm{SU}(3)_\rm{C}$ and family $\rm{SU}(3)_\rm{F}$ symmetries in a maximal rank-8 subgroup of ${\rm{E}}_8$ is proposed as a landmark for future explorations…

High Energy Physics - Phenomenology · Physics 2019-03-13 José E. Camargo-Molina , António P. Morais , Astrid Ordell , Roman Pasechnik , Jonas Wessén

We construct a 3-3-1 model for three families that can be embedded into a single SU(8) unified model. Assuming appropriate branching rules and symmetry-breaking pattern, we find a complete fermion content within irreducible representations…

High Energy Physics - Phenomenology · Physics 2011-05-25 R. Martinez , F. Ochoa , P. Fonseca

Models with spontaneously broken parity symmetry can solve the strong $CP$ problem in a natural way. We construct such a model in the context of $\SU3^3$ unification. Parity has the conventional meaning in this model, and the gauge group is…

High Energy Physics - Phenomenology · Physics 2009-10-22 Eric D. Carlson , Meng Yuan Wang

We show how the fields and particles of the standard model can be naturally realized in noncommutative gauge theory. Starting with a Yang-Mills matrix model in more than 4 dimensions, a SU(n) gauge theory on a Moyal-Weyl space arises with…

High Energy Physics - Theory · Physics 2010-05-12 Harald Grosse , Fedele Lizzi , Harold Steinacker

We study the dynamical symmetry breaking in the gauge-Higgs unification of the 5D ${\mathcal N}=1$ SUSY theory, compactified on an orbifold, $S^1/Z_2$. This theory identifies Wilson line degrees of freedoms as ``Higgs doublets''. We…

High Energy Physics - Phenomenology · Physics 2010-11-19 Naoyuki Haba , Toshifumi Yamashita

We present a five dimensional supersymmetric SO(10) model compactified on an orbifold $S^{(1)}/Z_2\tm Z_2'$. The gauge symmetry $G_{422}\equiv SU(4)_c\tm SU(2)_L\tm SU(2)_R$, realized on one of the fixed points (branes), is spontaneously…

High Energy Physics - Phenomenology · Physics 2014-11-17 Qaisar Shafi , Zurab Tavartkiladze

We study three-dimensional gauge dynamics by using type IIB superstring brane configurations, which can be obtained from the M-theory configuration of M2-branes stretched between two M5-branes with relative angles. Our construction of brane…

High Energy Physics - Theory · Physics 2009-10-31 Takuhiro Kitao , Kazutoshi Ohta , Nobuyoshi Ohta

Two theoretically well-motivated gauge extensions of the standard model are $SU(3)_C \times SU(3)_L \times SU(3)_R$ and $SU(3)_q \times SU(3)_L \times SU(3)_l \times SU(3)_R$, where $SU(3)_q$ is the same as $SU(3)_C$ and $SU(3)_l$ is its…

High Energy Physics - Phenomenology · Physics 2018-01-17 Corey Kownacki , Ernest Ma , Nicholas Pollard , Oleg Popov , Mohammadreza Zakeri

Extending recent work of Kachru and Silverstein, we consider ``orbifolds'' of 4-dimensional $\mathcal{N}=4$ SU(n) super-Yang-Mills theories with respect to discrete subgroups of the SU(4) $R$-symmetry which act nontrivially on the gauge…

High Energy Physics - Theory · Physics 2017-09-07 A. Lawrence , N. Nekrasov , C. Vafa