Exact standard model structures from intersecting D5-branes
By C. Kokorelis. 2002
157 citations recorded by the source corpus.
Abstract We discuss the appearance of non-supersymmetric compactifications with exactly the Standard Model (SM) at low energies, in the context of IIB orientifold constructions with D5-branes intersecting at angles on the T 4 tori, of the orientifold of T 4 ×( C / Z N ). We discuss constructions where the Standard Model embedding is considering within four, five and six stacks of D5-branes. The appearance of the three generation observable Standard Model at low energies is accompanied by a gauged baryon number, thus ensuring automatic proton stability. Also, a compatibility with a low scale of order TeV is ensured by having a two-dimensional space transverse to all branes. The present models complete the discussion of some recently constructed four-stack models of D5-branes with the SM at low energy. By embedding the four-, five- and six-stack Standard Model configurations into quiver diagrams, deforming them around the QCD intersection numbers, we find a rich variety of vacua that may have exactly the Standard Model at low energy. Also by using brane recombination on the U (1)'s, we show that the five and six vacua flow into their four-stack counterparts. Thus string vacua with five- and six-stack deformations are continuously connected to the four-stack vacua.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/b7327ea5d6cbfe63df10bd8ea156cfdc3f5f92f9
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Citations in the corpus
- Four-dimensional string compactifications with D-branes, orientifolds and fluxes (2006, methodology): “Therefore, the models constructed in [36, 37, 225, 226, 227, 228, 229, 230, 231, 232, 233, 234] can be regarded as a hybrid of these two methods to obtain chiral fermions, namely as intersecting branes at singularities.”
- TOWARD REALISTIC INTERSECTING D-BRANE MODELS (2005, methodology): “Therefore, the models constructed in [15, 16, 77, 78, 79, 80, 71, 81, 82, 83, 84, 85] can be regarded as a hybrid of the two ways to obtain chiral fermions, namely as intersecting branes at singularities.”