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Related papers: A Three-Family SU(6) Type I Compactification

200 papers

Type I string theory can be dimensionally reduced on group manifolds. The compactification on $S^3\times S^3$ leads to the N=4 gauged SU(2)$\times$SU(2) supergravity in four dimensions, which admits the BPS monopole type non-Abelian vacuum.…

High Energy Physics - Theory · Physics 2007-05-23 Mikhail S. Volkov

We construct N=1 and N=0 chiral four-dimensional vacua of flux compactification in Type IIB string theory. These vacua have the common features that they are free of tadpole instabilities (both NSNS and RR) even for models with N=0…

High Energy Physics - Theory · Physics 2008-11-26 Fernando Marchesano , Gary Shiu

We consider D=6, N=1, Z_M orbifold compactifications of heterotic strings in which the usual modular invariance constraints are violated. It is argued that in the presence of non-perturbative effects many of these vacua are nevertheless…

High Energy Physics - Theory · Physics 2016-09-06 G. Aldazabal , A. Font , L. E. Ibanez , A. M. Uranga , G. Violero

We point out that models where gauge and charged matter fields live on the world volume of D3 branes can provide a weak string coupling description of the gauge coupling unification in the supersymmetric standard model at a scale of order…

High Energy Physics - Phenomenology · Physics 2007-05-23 Erich Poppitz

Recently it was proposed that the ten dimensional tachyonic superstring vacua may serve as good starting points for the construction of viable phenomenological models. Such phenomenologically viable models enlarge the space of possible…

High Energy Physics - Theory · Physics 2020-04-29 Alon E. Faraggi , Viktor G. Matyas , Benjamin Percival

We construct N=1 supersymmetric four-dimensional orientifolds of type IIA on T^6/(Z_2 x Z_2) with D6-branes intersecting at angles. The use of D6-branes not fully aligned with the O6-planes in the model allows for a construction of many…

High Energy Physics - Theory · Physics 2009-09-17 Mirjam Cvetic , Gary Shiu , Angel M. Uranga

After a short introduction to Matrix theory, we explain how can one generalize matrix models to describe toroidal compactifications of M-theory and the heterotic vacua with 16 supercharges. This allows us, for the first time in history, to…

High Energy Physics - Theory · Physics 2007-05-23 Lubos Motl

The low energy effective theory of the N=1 supersymmetric SU(5) gauge theory with chiral superfields in the 5* and 10 representations is constructed. Instead of postulating the confinement of SU(5) (confining picture), only the confinement…

High Energy Physics - Theory · Physics 2009-10-30 Noriaki Kitazawa

In this paper we study the N=1 supersymmetric field theories realized on the world-volume of type IIB D3-branes sitting at orientifolds of non-orbifold singularities (conifold and generalizations). Several chiral models belong to this…

High Energy Physics - Theory · Physics 2009-10-09 J. Park , R. Rabadan , A. M. Uranga

We determine all D-branes in the non-tachyonic 0'B orientifold, examine their world-volume anomalies and study orbifold compactifications. We find that the spectrum of the D-branes contains chiral fermions in the symmetric, antisymmetric…

High Energy Physics - Theory · Physics 2010-11-19 E. Dudas , J. Mourad

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

This thesis contains an introductory chapter on orbifolds. The following chapter explains the foundations of orientifolds. Chapters 4-7 present own research. In chapter 4 we quantize open strings with linear boundary conditions, as they…

High Energy Physics - Theory · Physics 2009-09-29 Lars Goerlich

We obtain a three generational $SU(3)_c\times SU(3)_w \times U(1)^4\times [SO(12)\times U(1)^2]^\prime$ model from an orbifold construction with the requirement that three generations arise from twisted sectors. There exist supersymmetric…

High Energy Physics - Phenomenology · Physics 2009-10-22 Hang Bae Kim , Jihn E. Kim

We study the cosmology of a string derived supersymmetric flipped $SU(5)$ model in the context of free-fermionic heterotic constructions that allow full calculability of the effective supergravity in perturbation theory around the fermionic…

High Energy Physics - Theory · Physics 2021-03-12 Ignatios Antoniadis , Dimitri V. Nanopoulos , John Rizos

We obtain three generation SU(3)_c X SU(2)_L X U(1)_Y string models in all of the exactly solvable (0,2) constructions sampled by fermionization. None of these examples, including those that are symmetric abelian orbifolds, rely on the Z_2…

High Energy Physics - Theory · Physics 2009-10-28 Shyamoli Chaudhuri , George Hockney , Joseph D. Lykken

We study a class of four-dimensional N=1 superconformal field theories obtained from the six-dimensional (1,0) theory, on M5-branes on C^2/Z_k orbifold singularity, compactified on a Riemann surface. This produces various quiver gauge…

High Energy Physics - Theory · Physics 2016-01-27 Amihay Hanany , Kazunobu Maruyoshi

We first derive a class of six-dimensional (1,0) gauged supergravities arising from threefold compactifications of F-theory with background fluxes. The derivation proceeds via the M-theory dual reduction on an SU(3)-structure manifold with…

High Energy Physics - Theory · Physics 2015-06-15 Thomas W. Grimm , Tom G. Pugh

Using a six-orientifold on top of a NS-fivebrane we construct a chiral N=1 supersymmetric gauge theory in four dimensions with gauge group SU(N_c) and matter in the symmetric, antisymmetric and (anti)fundamental representations. Anomaly…

High Energy Physics - Theory · Physics 2009-10-31 Karl Landsteiner , Esperanza Lopez , David A. Lowe

We study total and partial supersymmetry breaking by freely acting orbifolds, or equivalently by Scherk-Schwarz compactifications, in type I string theory. In particular, we describe a four-dimensional chiral compactification with…

High Energy Physics - Theory · Physics 2010-11-19 I. Antoniadis , G. D'Appollonio , E. Dudas , A. Sagnotti

A while ago, examples of N=1 vacua in D=6 were constructed as orientifolds of Type IIB string theory compactified on the K3 surface. Among the interesting features of those models was the presence of D5-branes behaving like small…

High Energy Physics - Theory · Physics 2009-10-30 Eric G. Gimon , Clifford V. Johnson