An example of Kaluza-Klein-like theory with boundary conditions, which lead to massless and mass protected spinors chirally coupled to gauge fields

dc.creatorBorstnik, N. Mankoc
dc.creatorNielsen, H. B.
dc.date2005-09-14
dc.date2005-09-21
dc.date.accessioned2026-07-07T10:30:16Z
dc.date.available2026-07-07T10:30:16Z
dc.descriptionThe genuine Kaluza-Klein-like theories (with no fields in addition to gravity) have difficulties with the existence of massless spinors after the ompactification of some of dimensions of space\cite{witten}. We assume a $M^{(1+3)} \times$ a flat finite disk in $(1+5)$-dimensional space, with the boundary allowing spinors of only one handedness. Massless spinors then chirally couple to the corresponding background gauge gravitational field, which solves equations of motion for a free field, linear in the Riemann curvature.
dc.description10 pages, references added
dc.identifierhttps://arxiv.org/abs/hep-th/0509101
dc.identifierhttp://arxiv.org/abs/hep-th/0509101
dc.identifierPhys.Lett.B633:771-775,2006
dc.identifierdoi:10.1016/j.physletb.2005.12.065
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/178081
dc.subjectHigh Energy Physics - Theory
dc.titleAn example of Kaluza-Klein-like theory with boundary conditions, which lead to massless and mass protected spinors chirally coupled to gauge fields
dc.typetext

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