Operator Gauge Symmetry in QED

dc.contributor.authorKhademi, S.
dc.contributor.authorNasiri, S.
dc.date.accessioned2019-02-09T17:01:19Z
dc.date.available2019-02-09T17:01:19Z
dc.date.issued2006
dc.description.abstractIn this paper, operator gauge transformation, first introduced by Kobe, is applied to Maxwell's equations and continuity equation in QED. The gauge invariance is satisfied after quantization of electromagnetic fields. Inherent nonlinearity in Maxwell's equations is obtained as a direct result due to the nonlinearity of the operator gauge transformations. The operator gauge invariant Maxwell's equations and corresponding charge conservation are obtained by defining the generalized derivatives of the first and second kinds. Conservation laws for the real and virtual charges are obtained too. The additional terms in the field strength tensor are interpreted as electric and magnetic polarization of the vacuum.uk_UA
dc.identifier.citationOperator Gauge Symmetry in QED / S. Khademi, S. Nasiri // Symmetry, Integrability and Geometry: Methods and Applications. — 2006. — Т. 2. — Бібліогр.: 24 назв. — англ.uk_UA
dc.identifier.issn1815-0659
dc.identifier.other2000 Mathematics Subject Classification: 81V80; 78A25
dc.identifier.urihttps://nasplib.isofts.kiev.ua/handle/123456789/146435
dc.language.isoenuk_UA
dc.publisherІнститут математики НАН Україниuk_UA
dc.relation.ispartofSymmetry, Integrability and Geometry: Methods and Applications
dc.statuspublished earlieruk_UA
dc.titleOperator Gauge Symmetry in QEDuk_UA
dc.typeArticleuk_UA

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