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Intersecting stacks of supersymmetric fractional branes on the Z_6' orientifold may be used to construct the supersymmetric Standard Model. If a,b are the stacks that generate the SU(3)_{colour} and SU(2)_L gauge particles, then, in order…

High Energy Physics - Theory · Physics 2019-08-19 David Bailin , Alex Love

As a further elaboration of the proposal of Ref. [1] we address the construction of Standard-like models from configurations of stacks of orientifold planes and D-branes on an internal space with the structure ${(Gepner model)^{c=6} \times…

High Energy Physics - Theory · Physics 2009-11-11 G. Aldazabal , E. Andres , J. E. Juknevich

We analyse four-dimensional, supersymmetric intersecting D-brane models in a toroidal orientifold background from a statistical perspective. The distribution and correlation of observables, like gauge groups and couplings, are discussed. We…

High Energy Physics - Theory · Physics 2008-02-19 Florian Gmeiner

We study the introduction of orientifold six-planes in the type IIA brane configurations known as elliptic models. The N=4 SO(n) and $Sp(k)$ theories softly broken to N=2 through a mass for the adjoint hypermultiplet can be realized in this…

High Energy Physics - Theory · Physics 2009-10-09 Angel M. Uranga

We discuss the consistency conditions of a novel orientifold projection of type IIB string theory on C^2/Z_N singularities, in which one mods out by the combined action of world-sheet parity and a geometric operation which exchanges the two…

High Energy Physics - Theory · Physics 2009-10-09 Angel M. Uranga

We discuss type IIB orientifolds with D-branes, and NSNS and RR field strength fluxes. The D-brane sectors lead to open string spectra with non-abelian gauge symmetry and charged chiral fermions. The closed string field strengths generate a…

High Energy Physics - Theory · Physics 2009-11-10 Juan F. G. Cascales , Angel M. Uranga

Recently, the complete landscape of three-family supersymmetric Pati-Salam models from intersecting D6-branes on a type IIA $\mathbb{T}^6/(\mathbb{Z}_2\times \mathbb{Z}_2)$ orientifold has been enumerated consisting of 33 independent models…

High Energy Physics - Phenomenology · Physics 2025-02-18 Mudassar Sabir , Adeel Mansha , Tianjun Li , Zhi-Wei Wang

I discuss two types of non-supersymmetric string model constructions that give at low energy exactly the Standard model (SM) with no additional matter/and or gauge group factors. The construction is based on D6 branes intersecting at angles…

High Energy Physics - Theory · Physics 2017-08-23 Christos Kokorelis

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 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 launch a systematic search for phenomenologically appealing string vacua with intersecting D-branes on the promising T6/Z(2)xZ(6)xOR orientifold with discrete torsion. The number of independent background lattices is reduced from six to…

High Energy Physics - Theory · Physics 2014-11-14 Jill Ecker , Gabriele Honecker , Wieland Staessens

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 2016-09-06 David Bailin , Alex Love

We consider models built on $AdS_5\otimes S^5/\Gamma$ orbifold compactifications of the type $IIB$ superstring, where $\Gamma$ is the abelian group $Z_n$. An attractive three family $\mathcal{N}=0$ SUSY model is found for $n=7$ that is a…

High Energy Physics - Phenomenology · Physics 2008-11-26 James B. Dent , Pasquale L. Iafelice , Thomas W. Kephart

We study Type I string theory compactified on a T^6/Z_3 orientifold. The low-energy dynamics is most conveniently analyzed in terms of D3-branes. We show that a sector of the theory, which corresponds to placing an odd number of D3-branes…

High Energy Physics - Theory · Physics 2014-11-18 Joseph Lykken , Erich Poppitz , Sandip P. Trivedi

We provide a general overview of the current state of the art in three generation model building proposals - using intersecting D-brane toroidal compactifications of IIA string theories - which have, only, the SM at low energy. In this…

High Energy Physics - Theory · Physics 2016-09-06 Christos Kokorelis

We study novel type IIB compactifications on the T^6/Z_2 orientifold. This geometry arises in the T-dual description of Type I theory on T^6, and one normally introduces 16 space-filling D3-branes to cancel the RR tadpoles. Here, we cancel…

High Energy Physics - Theory · Physics 2009-11-07 Shamit Kachru , Michael Schulz , Sandip Trivedi

Type IIB superstring models with the standard model gauge group on D3-branes and with massless matter associated with open strings joining D3-branes to D3-branes or D3-branes to ${\rm D}7_3$-branes are studied. Models with gauge coupling…

High Energy Physics - Theory · Physics 2009-10-31 D. Bailin , G. V. Kraniotis , A. Love

In this work, we present a trinification-based grand unified theory incorporating a global $\mathrm{SU}(3)$ family symmetry that after a spontaneous breaking leads to a left-right symmetric model. Already at the classical level, this model…

High Energy Physics - Phenomenology · Physics 2016-10-06 José Eliel Camargo-Molina , António P. Morais , Roman Pasechnik , Jonas Wessén

In the context of supersymmetric compactifications of type II supergravity to four dimensions, we show that orientifold sources can be compatible with a generalized SU(3) x SU(3)-structure that is neither strictly SU(3) nor static SU(2). We…

High Energy Physics - Theory · Physics 2009-11-18 Paul Koerber , Dimitrios Tsimpis

We construct four-dimensional, globally consistent F-theory models with three chiral generations, whose gauge group and matter representations coincide with those of the Minimal Supersymmetric Standard Model, the Pati-Salam Model and the…

High Energy Physics - Theory · Physics 2015-09-30 Mirjam Cvetic , Denis Klevers , Damián Kaloni Mayorga Peña , Paul-Konstantin Oehlmann , Jonas Reuter