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We construct a class of anomaly-free supersymmetric U(1)' models that are characterized by family non-universal U(1)' charges motivated from E_6 embeddings. The family non-universality arises from an interchange of the standard roles of the…

High Energy Physics - Phenomenology · Physics 2010-12-23 Lisa L. Everett , Jing Jiang , Paul G. Langacker , Tao Liu

We perform a systematic study of the Standard Model embedding in a D-brane configuration of type I string theory at the TeV scale. We end up with an attractive model and we study several phenomenological questions, such as gauge coupling…

High Energy Physics - Theory · Physics 2008-11-26 I. Antoniadis , E. Kiritsis , J. Rizos , T. N. Tomaras

We present a class of N=1 supersymmetric models of particle physics, derived directly from heterotic M-theory, that contain three families of chiral quarks and leptons coupled to the gauge group $SU(3)_C\times SU(2)_{L}\times U(1)_{Y}$.…

High Energy Physics - Theory · Physics 2007-05-23 Ron Donagi , Burt A. Ovrut , Tony Pantev , Daniel Waldram

Requiring that supersymmetric SU(5) and SU(6) grand unifications in the heterotic string theory must have 3 chiral families, adjoint (or higher representation) Higgs fields in the grand unifiedgauge group, and a non-abelian hidden sector,…

High Energy Physics - Theory · Physics 2009-10-30 Zurab Kakushadze , S. -H. Henry Tye

An extension of the Standard Model to the local gauge group $SU(3)_c\otimes SU(4)_L\otimes U(1)_X$ as a three-family model is presented. The model does not contain exotic electric charges and we obtain a consistent mass spectrum by…

High Energy Physics - Phenomenology · Physics 2011-03-23 Luis A. Sanchez , Felipe A. Perez , William A. Ponce

The di-photon excess observed at the LHC can be explained as a Standard Model singlet that is produced and decays by heavy vector-like colour triplets and electroweak doublets in one-loop diagrams. The characteristics of the required…

High Energy Physics - Phenomenology · Physics 2016-10-20 J. Ashfaque , L. Delle Rose , A. E. Faraggi , C. Marzo

Three family SU(3)_C x SU(2)_L x U(1)_Y string models in several constructions generically possess two features: (i) an extra local anomalous U(1)_A and (ii) numerous (often fractionally charged) exotic particles beyond those in the minimal…

High Energy Physics - Phenomenology · Physics 2015-06-25 G. B. Cleaver , A. E. Faraggi , D. V. Nanopoulos

Four-dimensional strings with the standard model gauge group $SU(3)\times SU(2)\times U(1)$ give model-dependent predictions for the tree level weak mixing-angle. In the presence of an extra pseudo-anomalous gauged- ${U(1)}_X$, the value of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Luis E. Ibanez

I study the scalar representations of the electroweak group of the Standard Model, which is a subgroup of the chiral group U(N)L x U(N)R with N flavours, for N even, with a special emphasis on their chiral properties and on their behaviour…

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

We review recent progress in constructing realistic brane models from type I string vacua. Explicit models with three families of the standard model gauge group and its left-right generalizations are presented with supersymmetry broken at…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. Aldazabal , L. Ibanez , F. Quevedo

For supersymmetric extensions of the Standard Model we construct some expressions that include Yukawa couplings for the third and second generations and receive relatively small quantum corrections. This implies that they slightly depend on…

High Energy Physics - Phenomenology · Physics 2026-04-28 Kirill Krylov , Daniil Rystsov , Konstantin Stepanyantz

We consider a scenario in which the discrete weak symmetry between quarks and leptons is extended to the weak force by introducing exotic partners. We conjecture that there exists a hidden discrete symmetry $\tilde{P}$, defining a $Z_2$…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernesto A. Matute

We embed the minimal left-right model SU(2)_L*SU(2)_R* U(1)_{B-L} into an SU(4)_W gauge group, and break the unified group via five-dimensional S^1/(Z_2*Z_2) orbifolding. Leptons are fitted into SU(4)_W multiplets and located on a symmetry…

High Energy Physics - Phenomenology · Physics 2009-09-07 Csaba Balazs , Tianjun Li , Fei Wang , Jin Min Yang

The Twin Higgs model is the preeminent example of a theory of neutral naturalness, where the new particles that alleviate the little hierarchy problem are Standard Model (SM) singlets. The most promising collider search strategy, based on…

High Energy Physics - Phenomenology · Physics 2017-07-05 Hsin-Chia Cheng , Ennio Salvioni , Yuhsin Tsai

We study possible correlations between properties of the observable and hidden sectors in heterotic string theory. Specifically, we analyze the case of the Z6-II orbifold compactification which produces a significant number of models with…

A simple extension of the Standard Model (SM), based on the gauge group $SU(3)_C\otimes SU(3)_L\otimes U(1)_Y$ with $Y$ being the hypercharge, is considered. We show that, by imposing an approximate global $SU(2)_L\times SU(2)_R$ custodial…

High Energy Physics - Phenomenology · Physics 2016-03-30 Le Tho Hue , Le Duc Ninh

Some new physics beyond the Standard Model of particle physics, like Supersymmetry, Extra-dimensions etc., and their effect on the nature of different standard model phenomena are explored in this thesis. We discuss the power law scaling of…

High Energy Physics - Phenomenology · Physics 2008-07-21 Swarup Kumar Majee

We construct intersecting D5-brane orbifold models that yield the (non-supersymmetric) standard model up to vector-like matter and charged-singlet scalars. The models are constrained by the requirement that twisted tadpoles cancel, and that…

High Energy Physics - Theory · Physics 2010-04-05 D. Bailin , G. V. Kraniotis , A. Love

We construct N=1 supersymmetric fractional branes on the Z_6' orientifold. Intersecting stacks of such branes are needed to build a supersymmetric standard model. If a,b are the stacks that generate the SU(3)_c and SU(2)_L gauge particles,…

High Energy Physics - Theory · Physics 2008-11-26 David Bailin , Alex Love

Assuming that the Standard Model arises from the $E_8\times E_8$ Heterotic Superstring, we try to solve the discrepancy between the unification scale predicted by this theory ($\approx g_{GUT}\times 5.27\cdot 10^{17}$ GeV) and the value…

High Energy Physics - Phenomenology · Physics 2017-08-23 C. Munoz
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