Relativities and Homogeneous Spaces I -- Finite dimensional relativity representations

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dc.creatorSaller, Heinrich
dc.date2006-02-13
dc.date.accessioned2026-07-07T10:47:02Z
dc.date.available2026-07-07T10:47:02Z
dc.descriptionSpecial relativity, the symmetry breakdown in the electroweak standard model, and the dichotomy of the spacetime related transformations with the Lorentz group, on the one side, and the chargelike transformations with the hypercharge and isospin group, on the other side, are discussed under the common concept of "relativity". A relativity is defined by classes $G/H$ of a "little" group in a "general" group of operations.Relativities are representable as linear transformations that are considered for five physically relevant examples.
dc.description23 pages
dc.identifierhttps://arxiv.org/abs/physics/0602081
dc.identifierhttp://arxiv.org/abs/physics/0602081
dc.identifierInt.J.Theor.Phys.45:2150-2180,2006
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/183437
dc.subjectGeneral Physics
dc.titleRelativities and Homogeneous Spaces I -- Finite dimensional relativity representations
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