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We show how splitting supersymmetry reconciles a class of intersecting brane models with unification. The gauge sector in these models arises in multiplets of extended supersymmetry while matter states are in N=1 representations. A…

High Energy Physics - Phenomenology · Physics 2009-11-11 Ignatios Antoniadis , Karim Benakli , Antonio Delgado , Mariano Quiros , Marc Tuckmantel

D6-branes intersecting at angles allow for phenomenologically appealing constructions of four dimensional string theory vacua. While it is straightforward to obtain non-supersymmetric realizations of the standard model, supersymmetric and…

High Energy Physics - Theory · Physics 2009-11-10 Gabriele Honecker

We desribe in detail a Z_6 orbifold compactification of the heterotic E_8 x E_8 string which leads to the (supersymmetric) standard model gauge group and matter content. The quarks and leptons appear as three 16-plets of SO(10), two of…

High Energy Physics - Theory · Physics 2008-11-26 Wilfried Buchmuller , Koichi Hamaguchi , Oleg Lebedev , Michael Ratz

Intersecting branes provide a useful mechanism to construct particle physics models from string theory with a wide variety of desirable characteristics. The landscape of such models can be enormous, and navigating towards regions which are…

High Energy Physics - Theory · Physics 2022-05-18 Gregory J. Loges , Gary Shiu

We study brane configurations in the presence of orientifold six-planes. After deriving the curves for N=2 supersymmetric SU(Nc) gauge theories with one flavor in the symmetric or antisymmetric representation and Nf fundamental flavors, we…

High Energy Physics - Theory · Physics 2010-02-03 Karl Landsteiner , Esperanza Lopez , David A. Lowe

By employing D6-branes intersecting at angles in $D = 4$ type I strings, we construct {\em five stack} string GUT models (PS-II class), that contain at low energy {\em exactly the Standard model} with no extra matter and/or extra gauge…

High Energy Physics - Theory · Physics 2007-05-23 Christos Kokorelis

By employing D6-branes intersecting at angles in $D = 4$ type I strings, we construct the first examples of three generation string GUT models (PS-A class), that contain at low energy exactly the standard model spectrum with no extra matter…

High Energy Physics - Theory · Physics 2009-11-07 Christos Kokorelis

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

Intersecting D-brane models seem to be one of the most promising avenues to embed the Standard Model physics within the string context. We review here different aspects of these models. Topics include the question of SUSY and quasi-SUSY in…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Cremades , L. E. Ibanez , F. Marchesano

We show how to construct supersymmetric three-generation models with gauge group and matter content of the Standard Model in the framework of non-simply-connected elliptically fibered Calabi-Yau manifolds Z. The elliptic fibration on a…

High Energy Physics - Theory · Physics 2009-11-10 Gottfried Curio

We present special classes of orientifold models involving supersymmetry breaking via branes at angles. Type II superstring theories are compactified on a two torus times a four-dimensional orbifold. Combining worldsheet parity with a…

High Energy Physics - Theory · Physics 2015-06-26 Gabriele Honecker

Many four-dimensional supersymmetric compactifications of F-theory contain gauge groups that cannot be spontaneously broken through geometric deformations. These "non-Higgsable clusters" include realizations of $SU(3)$, $SU(2)$, and $SU(3)…

High Energy Physics - Theory · Physics 2015-06-23 Antonella Grassi , James Halverson , Julius Shaneson , Washington Taylor

We review the possibility that the Supersymmetric Standard Model arises from orbifold constructions of the E_8 x E_8 Heterotic Superstring, and the phenomenological properties that such a model should have. In particular, trying to solve…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Munoz

In this review we describe the general geometrical framework of brane world constructions in orientifolds of type IIA string theory with D6-branes wrapping 3-cycles in a Calabi-Yau 3-fold. These branes generically intersect in points on the…

High Energy Physics - Theory · Physics 2009-11-10 Dieter Lust

We consider $SU(N)$ $\mathcal{N}=4$ super Yang-Mills with cubic and quadratic soft SUSY breaking potential, such that the global $SU(4)_R$ is broken to $SU(3)$ or further. As shown recently, this set-up supports a rich set of non-trivial…

High Energy Physics - Theory · Physics 2018-04-24 Marcus Sperling , Harold C. Steinacker

We construct a six-dimensional gauge-Higgs unification model with the enlarged gauge group of $E_6$ on $S^2/Z_2$ orbifold compactification. The standard model particle contents and gauge symmetry are obtained by utilizing a monopole…

High Energy Physics - Phenomenology · Physics 2014-11-21 Cheng-Wei Chiang , Takaaki Nomura

We investigate intersecting D6-branes on an orientifold of type IIA theory in the orbifold background T^6/(Z_4 x Z_2) with the emphasis on finding chiral spectra. RR tadpole cancellation conditions and the scalar potential at disc level are…

High Energy Physics - Theory · Physics 2010-04-05 Gabriele Honecker

We construct new Standard-like models on Type II orientifolds. In Type IIA theory on $\mathbf{T^6/(\Z_2\times \Z_2)}$ orientifold with intersecting D6-branes, we first construct a three-family trinification model where the $U(3)_C\times…

High Energy Physics - Theory · Physics 2008-11-26 Ching-Ming Chen , Tianjun Li , Dimitri V. Nanopoulos

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

In a previous publication, arXiv:1106.4804, we have found 200 models from heterotic Calabi-Yau compactifications with line bundles, which lead to standard models after taking appropriate quotients by a discrete symmetry and introducing…

High Energy Physics - Theory · Physics 2015-06-04 Lara B. Anderson , James Gray , Andre Lukas , Eran Palti
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