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Related papers: Three Generations in Type I Compactifications

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We investigate the connections between four-dimensional, N=2 M-theory vacua constructed as orbifolds of type II, heterotic, and type I strings. All these models have the same massless spectrum, which contains an equal number of vector…

High Energy Physics - Theory · Physics 2009-10-31 Andrea Gregori , Costas Kounnas

We describe type IIB compactifications with varying coupling constant in d=6,7,8,9 dimensions, where part of the ten-dimensional SL(2,Z) symmetry is broken by a background with Gamma_0(n) or Gamma(n) monodromy for n=2,3,4. This extends the…

High Energy Physics - Theory · Physics 2008-11-26 P. Berglund , A. Klemm , P. Mayr , S. Theisen

We briefly review attempts to construct string theories that yield the standard model, concentrating on models with a geometric interpretation. Calabi-Yau compactifications are discussed in the context of both the weakly coupled heterotic…

High Energy Physics - Theory · Physics 2007-05-23 D. Bailin , G. V. Kraniotis , A. Love

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

Employing new scanning methods, we revisit the systematic construction of three-family $N=1$ supersymmetric Pati-Salam models in Type IIA orientifolds on ${\bf T}^6/(\mathbb Z_2\times \mathbb Z_2)$ with intersecting D6-branes. Arising from…

High Energy Physics - Theory · Physics 2020-06-23 Tianjun Li , Adeel Mansha , Rui Sun

We study N=2 four-dimensional flux vacua describing intrinsic non-perturbative systems of 3 and 7 branes in type IIB string theory. The solutions are described as compactifications of a G(ravity) theory on a Calabi Yau threefold which…

High Energy Physics - Theory · Physics 2013-10-24 Andreas P. Braun , Francesco Fucito , Jose Francisco Morales

We construct a 6D supergravity theory which emerges as intermediate step in the compactification of the heterotic string to the supersymmetric standard model in four dimensions. The theory has N=2 supersymmetry and a gravitational sector…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Buchmüller , C. Lüdeling , J. Schmidt

We consider "magnetized brane" compactifications of the type I/heterotic string on K3 with U(1) background fluxes. The nonabelian gauge group and matter content of the resulting six-dimensional vacua are parameterized by a matrix encoding a…

High Energy Physics - Theory · Physics 2012-06-28 Vijay Kumar , Washington Taylor

A gauge theory with gauge group G defined in D>4 space-time dimensions can be broken to a subgroup H on four dimensional fixed point branes, when compactified on an orbifold. Mass terms for extra dimensional components of gauge fields A_i…

High Energy Physics - Phenomenology · Physics 2010-11-19 G. v. Gersdorff , N. Irges , M. Quiros

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

Birational Calabi-Yau threefolds in the same deformation family provide a `weak' counterexample to the global Torelli problem, as long as they are not isomorphic. In this paper, it is shown that deformations of certain desingularized…

Algebraic Geometry · Mathematics 2009-10-31 Balazs Szendroi

We systematically consider heterotic SO(32) and E8 x E8 compactifications on K3 with Abelian and non-Abelian backgrounds as well as an arbitrary number of five-branes. The masses of the U(1) factors depend on the first Chern classes of the…

High Energy Physics - Theory · Physics 2008-11-26 Gabriele Honecker

We indicate how consistent heterotic orbifold compactifications, including non perturbative information, can be constructed. We first analyse the situation in six dimensions, N=1, where strong coupling effects, implying the presence of five…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. Aldazabal

We study the cancellation of U(1) anomalies in Type I and Type IIB D=4, N=1 string vacua. We first consider the case of compact toroidal $Z_N$ Type IIB orientifolds and then proceed to the non-compact case of Type IIB D3 branes at orbifold…

High Energy Physics - Theory · Physics 2009-10-09 L. E. Ibanez , R. Rabadan , A. M. Uranga

We describe the construction of configurations of D6-branes wrapped on compact 3-cycles intersecting at points in non-compact Calabi-Yau threefolds. Such constructions provide local models of intersecting brane worlds, and describe sectors…

High Energy Physics - Theory · Physics 2009-11-07 Angel M. Uranga

We present compact three-generation F-theory GUT models meeting in particular the constraints of D3-tadpole cancellation and D-term supersymmetry. To this end we explicitly construct elliptically fibered Calabi-Yau fourfolds as complete…

High Energy Physics - Theory · Physics 2014-11-20 Thomas W. Grimm , Sven Krause , Timo Weigand

We study supergravity solutions representing D3-branes with transverse 6-space having R x S^2 x S^3 topology. We consider regular and fractional D3-branes on a natural one-parameter extensions of the standard Calabi-Yau metrics on the…

High Energy Physics - Theory · Physics 2009-09-17 L. A. Pando Zayas , A. A. Tseytlin

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 construct a supersymmetric standard model in the context of the $Z_{12-I}$ orbifold compactification of the heterotic string theory. The gauge group is $SU(3)_c\times SU(2)_L\times U(1)_Y\times U(1)^4\times[SO(10)\times U(1)^3]'$. We…

High Energy Physics - Phenomenology · Physics 2010-10-27 Jihn E. Kim , Ji-Hun Kim , Bumseok Kyae

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