An Octonionic Gauge Theory

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dc.creatorLassig, C. C.
dc.creatorJoshi, G. C.
dc.date1995-03-28
dc.date.accessioned2026-07-07T06:28:53Z
dc.date.available2026-07-07T06:28:53Z
dc.descriptionThe nonassociativity of the octonion algebra necessitates a bimodule representation, in which each element is represented by a left and a right multiplier. This representation can then be used to generate gauge transformations for the purpose of constructing a field theory symmetric under a gauged octonion algebra, the nonassociativity of which appears as a failure of the representation to close, and hence produces new interactions in the gauge field kinetic term of the symmetric Lagrangian.
dc.description14 pages, Revtex
dc.identifierhttps://arxiv.org/abs/hep-th/9503189
dc.identifierhttp://arxiv.org/abs/hep-th/9503189
dc.identifierChaos Solitons Fractals 7 (1996) 769-775
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/97848
dc.subjectHigh Energy Physics - Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.titleAn Octonionic Gauge Theory
dc.typetext

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