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Related papers: Deformed Intersecting D6-Brane GUTS and N=1 SUSY

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A simple supersymmetric SO(10) GUT in five dimensions is considered. The fifth dimension is compactified on the $S^1/(Z_2\times Z_2^\prime)$ orbifold possessing two inequivalent fixed points. In our setup, all matter and Higgs multiplets…

High Energy Physics - Phenomenology · Physics 2008-11-26 Takeshi Fukuyama , Nobuchika Okada

We investigate supersymmetric SU(5) grand-unified theories (GUTs) realized in 5 space-time dimensions and broken down to the MSSM by SU(5)-violating boundary conditions on a S^1/(Z_2 x Z_2') orbifold with two 3-branes. The doublet-triplet…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. Hebecker , J. March-Russell

We explore the possible values of the $\mu \to e \gamma$ branching ratio, $\text{BR}(\mu\rightarrow e\gamma)$, and the electron dipole moment (eEDM), $d_e$, in no-scale SU(5) super-GUT models with the boundary conditions that soft…

High Energy Physics - Phenomenology · Physics 2021-02-24 John Ellis , Jason L. Evans , Natsumi Nagata , Keith A. Olive , Liliana Velasco-Sevilla

A new class of six-dimensional asymmetric orientifolds is considered where the orientifold operation is combined with T-duality. The models are supersymmetric in the bulk, but the cancellation of the tadpoles requires the introduction of…

High Energy Physics - Theory · Physics 2014-11-18 Carlo Angelantonj , Ralph Blumenhagen , Matthias R. Gaberdiel

We construct D=4 Type I vacua with massless content remarkably close to that of the standard model of particle physics. They are tachyon-free non-supersymmetric models which are obtained starting with a standard D=4, N=1 compact Type IIB…

High Energy Physics - Theory · Physics 2014-11-18 G. Aldazabal , L. E. Ibanez , F. Quevedo

We show how gauge coupling unification near the Planck scale $M_P\sim 10^{19}$ GeV can be achieved in the framework of supersymmetry, facilitating a full unification of all forces with gravity. Below the conventional GUT scale $M_{GUT}\sim…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Howl , S. F. King

After a brief review of the motivations for grand unification, I discuss the main challenges facing realistic SUSY GUT model building. Achieving doublet-triplet splitting without fine--tuning is chief among them. Symmetry breaking should…

High Energy Physics - Phenomenology · Physics 2011-11-10 K. S. Babu

We construct semi-local and global realizations of SU(5) GUTs in F-theory that utilize a U(1)_PQ symmetry to protect against dimension four proton decay. Symmetries of this type, which assign charges to H_u and H_d that forbid a tree level…

High Energy Physics - Theory · Physics 2010-05-12 Joseph Marsano , Natalia Saulina , Sakura Schafer-Nameki

We construct the type IIA nonsupersymmetric meta-stable brane configurations corresponding to the various N=1 supersymmetric gauge theories. The D6-branes are both displaced and rotated where these deformations are described as the mass…

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

I describe the main features of new intersecting D4- and D5-brane orbifold models that yield the non-supersymmetric standard model, up to vector-like matter and, in some cases, extra U(1) factors in the gauge group. There are six-stack…

High Energy Physics - Theory · Physics 2009-11-07 D. Bailin

We introduce a non-Abelian discrete $\Delta_{27}$ family symmetry into the recently proposed classes of Exceptional Supersymmetric Standard Model ($E_6$SSM) based on a broken $E_6$ Grand Unified Theory (GUT) in order to solve the flavour…

High Energy Physics - Phenomenology · Physics 2009-01-06 R. Howl , S. F. King

Much work has been done by a number of authors with the aim of constructing the supersymmetric Standard Model in type IIA intersecting-brane theories compactified on an orientifold with various Z_N or Z_M x Z_N point groups. Here we…

High Energy Physics - Theory · Physics 2015-06-17 David Bailin , Alex Love

We perform a complete analysis of one-loop threshold corrections to the gauge couplings of fractional D6-branes. This includes besides SU(N) also symplectic, orthogonal and massless Abelian gauge factors and the full computation of…

High Energy Physics - Theory · Physics 2010-01-18 Florian Gmeiner , Gabriele Honecker

We construct a 5D SUSY SU(6) GUT on an $S^{(1)}/Z_2\tm Z_2'$ orbifold. The first stage of gauge symmetry breaking occurs through compactification and a specific selection of boundary conditions. Additional symmetries play a crucial role for…

High Energy Physics - Phenomenology · Physics 2008-11-26 Filipe Paccetti Correia , Michael G. Schmidt , Zurab Tavartkiladze

We examine new classes of GUT models where the GUT gauge group is broken by a 4D analogue of the Scherk-Schwarz mechanism. These models are inspired by ``deconstructed'' 5D Scherk-Schwarz orbifold models. However, no fine tuning of…

High Energy Physics - Phenomenology · Physics 2009-09-17 Csaba Csaki , Graham D. Kribs , John Terning

A three-family non-supersymmetric model with U(3)^3 gauge symmetry is analyzed in the context of intersecting D-branes. This is equivalent to the `trinification' model extended by three U(1) factors which survive as global symmetries in the…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. K. Leontaris

We consider realizations of GUT models in F-theory. Adopting a bottom up approach, the assumption that the dynamics of the GUT model can in principle decouple from Planck scale physics leads to a surprisingly predictive framework. An…

High Energy Physics - Theory · Physics 2009-11-13 Chris Beasley , Jonathan J. Heckman , Cumrun Vafa

Several dimensionful parameters needed for model building can be engineered in a certain class of SU(5) F-theory GUTs by adding extra singlet fields which are localized along pairwise intersections of D7-branes. The values of these…

High Energy Physics - Theory · Physics 2010-02-11 Joseph Marsano , Natalia Saulina , Sakura Schafer-Nameki

We present a supersymmetric Pati-Salam model with small representations as a potential candidate for physics beyond the Standard Model. The model features a Higgs sector with bifundamental fields $H_R+\bar H_R=(4,1,2)+(\bar 4,1,2)$,…

High Energy Physics - Phenomenology · Physics 2025-02-24 George K. Leontaris , Ruiwen Ouyang , Ye-ling Zhou

We construct flipped SU(5) GUT models as Type IIB flux vacua on $\Z_2\times \Z_2$ orientifolds. Turning on supergravity self-dual NSNS and RR three-form fluxes fixes the toroidal complex structure moduli and the dilaton. We give a specific…

High Energy Physics - Theory · Physics 2009-11-11 Ching-Ming Chen , V. E. Mayes , D. V. Nanopoulos
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