Galilei invariant theories. III. Wave equations for massless fields

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dc.creatorNiederle, J.
dc.creatorNikitin, A. G.
dc.date2007-07-23
dc.date.accessioned2026-07-07T08:19:51Z
dc.date.available2026-07-07T08:19:51Z
dc.descriptionGalilei invariant equations for massless fields are obtained via contractions of relativistic wave equations. It is shown that the collection of non-equivalent Galilei-invariant wave equations for massless fields with spin equal 1 and 0 is very broad and describes many physically consistent systems. In particular, there exist a huge number of such equations for massless fields which correspond to various contractions of representations of the Lorentz group to those of the Galilei one.
dc.description17 pages
dc.identifierhttps://arxiv.org/abs/0707.3386
dc.identifierhttp://arxiv.org/abs/0707.3386
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/134906
dc.subjectMathematical Physics
dc.subjectQuantum Physics
dc.subject35A30, 35Q55, 58J70, 81R05
dc.titleGalilei invariant theories. III. Wave equations for massless fields
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