Supersymmetric three family SU(5) grand unified models from type IIA orientifolds with intersecting D6-branes
By M. Cvetič, Ioannis Papadimitriou, Gary Shiu. 2002
137 citations recorded by the source corpus.
Abstract We construct some N =1 supersymmetric three-family SU (5) grand unified models from type IIA orientifolds on T 6 /( Z 2 × Z 2 ) with D6-branes intersecting at general angles. These constructions are supersymmetric only for special choices of untwisted moduli. We show that within the above class of constructions there are no supersymmetric three-family models with 3 copies of 10 -plets unless there are simultaneously some 15 -plets. We systematically analyze the construction of such models and their spectra. The M-theory lifts of these brane constructions become purely geometrical backgrounds: they are singular G 2 manifolds where the grand unified gauge symmetries and three families of chiral fermions are localized at codimension 4 and codimension 7 singularities respectively. We also study some preliminary phenomenological features of the models.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/f936c3f8ee5e2ecba7064ea0ae56ba8cce5026b4
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In Nuclear and High Energy Physics
Citations in the corpus
- TOWARD REALISTIC INTERSECTING D-BRANE MODELS (2005, methodology): “As mentioned above, within this framework the systematic search for threefamily SU(5) Grand Unified Models [101] produced three family models which however necessarily also contain three copies of 15-plets.”
- Four-dimensional string compactifications with D-branes, orientifolds and fluxes (2006, background): “239 5.4.2 Example: MSSM-like model on T6/Z2 × Z2 . . . . . . . . . . .”
- MODELS OF PARTICLE PHYSICS FROM TYPE IIB STRING THEORY AND F-THEORY: A REVIEW (2012, unknown): “pFor work in this direction see [111–115].”
- Getting just the supersymmetric standard model at intersecting branes on the Z(6) orientifold (2004, background): “Nevertheless, the goal so far has been achieved only with moderate success: either the constructions are plagued with a large amount of exotic chiral matter, as in the Z2×Z2 orientifold of [28–33], which might be cured by a confinement of the exotic chiral matter into composite fields coming from th”
- GUTs in Type IIB Orientifold Compactifications (2008, methodology): “At least locally, each such field can be identified with an element of an appropriate bundle valued cohomology group on the internal mani- 10 fold and the cycles wrapped by the D-branes.”
- Orientifolds, hypercharge embeddings and the Standard Model (2006, background): “By contrast, the models found in [33] contain additional (15)’s of SU(5).”
- Proton stability in grand unified theories, in strings and in branes (2006, background): “An interesting class of models are those based on intersecting D branes [355, 356, 357, 358, 359] and attempts have been made to build semi-realistic models based on these [360, 361, 362, 363, 364, 365], and issues of gauge coupling unification, soft breaking and possible applications to the real wo”
- The statistics of supersymmetric D-brane models (2004, methodology): “In section 5 we come to the physically most interesting example and compute the same distribution for the case of intersecting branes on the T 6/Z Z2 × Z Z2 orientifold [28, 35 ].”