Propagation Properties of Bound Electromagnetic Field: Classical and Quantum Viewpoints

dc.authoridYarman, Tolga/0000-0003-3209-2264
dc.authoridKholmetskii, Alexander/0000-0002-5182-315X
dc.authorscopusid7004016669
dc.authorscopusid55893162300
dc.authorscopusid6602787345
dc.authorscopusid6602529732
dc.authorwosidYarman, Tolga/Q-9753-2019
dc.contributor.authorYarman, Nuh Tolga
dc.contributor.authorMissevitch, O. V.
dc.contributor.authorYarman, T.
dc.contributor.authorSmirnov-Rueda, R.
dc.contributor.otherEnerji Sistemleri Mühendisliği / Energy Systems Engineering
dc.date.accessioned2024-05-25T12:30:26Z
dc.date.available2024-05-25T12:30:26Z
dc.date.issued2020
dc.departmentOkan Universityen_US
dc.department-temp[Kholmetskii, A. L.] Belarusian State Univ, Minsk, BELARUS; [Missevitch, O. V.] Belarusian State Univ, Inst Nucl Problems, Minsk, BELARUS; [Yarman, T.] Istanbul Okan Univ, Istanbul, Turkey; [Smirnov-Rueda, R.] Univ Complutense Madrid, Madrid, Spainen_US
dc.descriptionYarman, Tolga/0000-0003-3209-2264; Kholmetskii, Alexander/0000-0002-5182-315Xen_US
dc.description.abstractThe present work is motivated by recent experiments aimed to measure the propagation velocity of bound electromagnetic (EM) field (Missevitch, et al. in EPL 93:64004, 2011; de Sangro et al. in Eur Phys J C 75:137, 2015) that reveal no retardation in the absence of EM radiation. We show how these findings can be incorporated into the mathematical structure of special relativity theory that allows us to reconsider some selected problems of classical and quantum electrodynamics. In particular, we come to the conclusion that the total four-momentum for a classical system "particles plus fields" ought to be a present state function of moving charges if EM radiation is negligible. In quantum domain, we analyze novel definition of the momentum operator recently suggested in the study of quantum phase effects (Kholmetskii et al. in Sci. Rep. 8:11937, 2018). It implies that bound EM field energy and momentum are to be present state functions, too. Being in agreement with reported experiments, these conclusions suggest the necessity to carry out more precise experimental verifications for additional and independent determination of propagation properties of bound EM fields. A scheme of a possible experiment on this subject is also proposed.en_US
dc.identifier.citation0
dc.identifier.doi10.1007/s10701-020-00396-8
dc.identifier.endpage1722en_US
dc.identifier.issn0015-9018
dc.identifier.issn1572-9516
dc.identifier.issue11en_US
dc.identifier.scopus2-s2.0-85093926088
dc.identifier.scopusqualityQ2
dc.identifier.startpage1686en_US
dc.identifier.urihttps://doi.org/10.1007/s10701-020-00396-8
dc.identifier.urihttps://hdl.handle.net/20.500.14517/2203
dc.identifier.volume50en_US
dc.identifier.wosWOS:000583495100001
dc.identifier.wosqualityQ3
dc.language.isoen
dc.publisherSpringeren_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectClassical electrodynamicsen_US
dc.subjectBound electromagnetic fielden_US
dc.subjectSpecial relativityen_US
dc.subjectQuantum electrodynamicsen_US
dc.subjectQuantum phasesen_US
dc.titlePropagation Properties of Bound Electromagnetic Field: Classical and Quantum Viewpointsen_US
dc.typeArticleen_US
dspace.entity.typePublication
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