Quantum Fields a la Sylvester and Witt

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dc.creatorSaller, H.
dc.creatorBreuninger, R.
dc.creatorHaft, M.
dc.date1995-06-09
dc.date.accessioned2026-07-07T12:04:21Z
dc.date.available2026-07-07T12:04:21Z
dc.descriptionA structural explanation of the coupling constants in the standard model, i.e the fine structure constant and the Weinberg angle, and of the gauge fixing contributions is given in terms of symmetries and representation theory. The coupling constants are normalizations of Lorentz invariantly embedded little groups (spin and polarization) arising in a harmonic analysis of quantum vector fields. It is shown that the harmonic analysis of massless fields requires an extension of the familiar Fourier decomposition, containing also indefinite unitary nondecomposable time representations. This is illustrated by the nonprobabilistic contributions in the electromagnetic field.
dc.description18 pages LaTeX file (62 kB), all macros are included
dc.identifierhttps://arxiv.org/abs/quant-ph/9506013
dc.identifierhttp://arxiv.org/abs/quant-ph/9506013
dc.identifierNuovoCim.A108:1225-1246,1995
dc.identifierdoi:10.1007/BF02820745
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/208105
dc.subjectQuantum Physics
dc.subjectHigh Energy Physics - Theory
dc.titleQuantum Fields a la Sylvester and Witt
dc.typetext

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