The supersymmetric standard model from the Z_6' orientifold?

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dc.creatorBailin, David
dc.creatorLove, Alex
dc.date2006-07-21
dc.date.accessioned2026-07-07T10:42:30Z
dc.date.available2026-07-07T10:42:30Z
dc.descriptionWe 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, then, in order to obtain just the chiral spectrum of the (supersymmetric) standard model (with non-zero Yukawa couplings to the Higgs multiplets), it is necessary that the number of intersections a \circ b of the stacks a and b, and the number of intersections a \circ b' of a with the orientifold image b' of b satisfy (a \circ b, a \circ b')=\pm(2,1) or \pm(1,2). It is also necessary that there is no matter in symmetric representations of the gauge group, and not too much matter in antisymmetric representations, on either stack. We provide a number of examples having these properties. Different lattices give different solutions and different physics.
dc.descriptionLatex 9 pages. Talk given at Cairo International Conference on High Energy Physics, Jan 2006
dc.identifierhttps://arxiv.org/abs/hep-th/0607158
dc.identifierhttp://arxiv.org/abs/hep-th/0607158
dc.identifierAIPConf.Proc.881:1-9,2007
dc.identifierdoi:10.1063/1.2435274
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/181969
dc.subjectHigh Energy Physics - Theory
dc.titleThe supersymmetric standard model from the Z_6' orientifold?
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