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Related papers: New Standard Model Vacua from Intersecting Branes

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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

Recently a class of Type IIA orientifold models was constructed yielding just the fermions of the SM at the intersections of D6-branes wrapping a 6-torus. We generalize that construction to the case of Type IIB compactified on an…

High Energy Physics - Theory · Physics 2016-09-06 D. Cremades , L. E. Ibanez , F. Marchesano

We construct supersymmetric composite models of quarks and leptons from type IIA T^6/(Z_2 x Z_2) orientifolds with intersecting D6-branes. In case of T^6 = T^2 x T^2 x T^2 with no tilted T^2, a composite model of the supersymmetric SU(5)…

High Energy Physics - Theory · Physics 2009-11-10 Noriaki Kitazawa

We construct new string vacua featuring Brane Supersymmetry Breaking, based on $T^4/\mathbb{Z}_N$ orientifolds with $\text{O}5_+$ planes and $\overline{\text{D}5}$ branes. Differently from the original construction, in these vacua the…

High Energy Physics - Theory · Physics 2024-03-06 C. Angelantonj , C. Condeescu , E. Dudas , G. Leone

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 construct new supersymmetric SU(5) Grand Unified Models based on Z4 x Z2 orientifolds with intersecting D6-branes. Unlike constructions based on Z2 x Z2 orientifolds, the orbifold images of the three-cycles wrapped by D6-branes…

High Energy Physics - Theory · Physics 2008-11-26 Mirjam Cvetic , Paul Langacker

We address dynamical supersymmetry breaking within a N=1 supersymmetric Standard-like Model based on a Z_2 x Z_2 Type IIA orientifold with intersecting D6-branes. The model possesses an additional, confining gauge sector with the USp(2)_A x…

High Energy Physics - Theory · Physics 2009-09-17 Mirjam Cvetic , Paul Langacker , Jing Wang

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 a one-parameter set of intersecting D4-brane models, with six stacks, that yield the (non-supersymmetric) standard model plus extra vector-like matter. Twisted tadpoles and gauge anomalies are cancelled, and the model contains…

High Energy Physics - Theory · Physics 2009-11-07 D. Bailin , G. V. Kraniotis , A. Love

We propose a minimal embedding of the Standard Model spectrum in a D-brane configuration of type I string theory. The SU(3) color and SU(2) weak interactions arise from two different collections of branes. The model is neither grand unified…

High Energy Physics - Phenomenology · Physics 2009-10-31 I. Antoniadis , E. Kiritsis , T. Tomaras

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

I briefly describe the recent construction of the first specific string D-brane models yielding just the SM massless fermion spectrum. One of the most remarkable facts predicted by these constructions is that the global symmetries of the SM…

High Energy Physics - Phenomenology · Physics 2017-08-23 L. E. Ibanez

We discuss the first string theory examples of three generation non-supersymmetric SU(5) and {\em flipped} SU(5) GUTS, which break to the Standard model at low energy, without extra matter and/or gauge group factors. Our GUT examples are…

High Energy Physics - Theory · Physics 2016-09-06 Minos Axenides , Emmanuel Floratos , Christos Kokorelis

We analyze the construction of non-supersymmetric three generation six-stack Pati-Salam (PS) $SU(4)_C \times SU(2)_L \times SU(2)_R$ GUT classes of models, by localizing D6-branes intersecting at angles in four dimensional orientifolded…

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

We construct an N=1 supersymmetric three-family flipped SU(5) model from type IIA orientifolds on $T^6/(\Z_2\times \Z_2)$ with D6-branes intersecting at general angles. The model is constrained by the requirement that Ramond-Ramond tadpoles…

High Energy Physics - Theory · Physics 2009-11-11 C. -M. Chen , G. V. Kraniotis , V. E. Mayes , D. V. Nanopoulos , J. W. Walker

We provide a general overview of the current state of the art in four dimensional three generation model building proposals - using intersecting D-brane toroidal compactifications [without fluxes] of IIA, IIB string theories - which have…

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

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 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

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

For recently constructed classes of D6-brane models, yielding the Standard Model fermion spectrum and gauge symmetry, we compute lower bounds on the masses of new U(1) fields that such models predict in addition to the hypercharge $U(1)_Y$.…

High Energy Physics - Phenomenology · Physics 2011-03-23 D. M. Ghilencea