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Please use this identifier to cite or link to this item: https://libeldoc.bsuir.by/handle/123456789/37759
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dc.contributor.authorKuraev, A. A.-
dc.contributor.authorKoronovskii, A. A.-
dc.contributor.authorKurkin, S. A.-
dc.contributor.authorRak, A. O.-
dc.contributor.authorRempen, I. S.-
dc.contributor.authorBadarin, A. A.-
dc.contributor.authorHramov, A. E.-
dc.date.accessioned2019-12-09T08:39:11Z-
dc.date.available2019-12-09T08:39:11Z-
dc.date.issued2018-
dc.identifier.citationIsolation of two-dimensional E-fields in the excitation equations for hollow waveguides / Kuraev A. A. [and others] // Infocommunications and radio technologies. – 2018. – Vol. 1, no. 1. – P. 17 – 28. – DOI: 10.15826/icrt.2018.01.1.02.ru_RU
dc.identifier.urihttps://libeldoc.bsuir.by/handle/123456789/37759-
dc.description.abstractThe traditional excitation equations of the Vainshtein waveguide excitation theory based on presenting the field excited by extraneous sources as a sum of TE and TM eigenwaves of the hollow waveguide, which transversal components form the complete basis in the class of the transversal vectors of a waveguide section. However, in the excitation sources area (longitudinal sonde, electron beam) the waveguide is not hollow and the potential transverse electric field appears in this area. The transversal electric field completes the basis of TE and TM waves. This is not taken into account in the traditional excitation equations. In this paper, the necessary correction of the excitation equations in the sources area is obtained.ru_RU
dc.language.isoenru_RU
dc.publisherУФУru_RU
dc.subjectпубликации ученыхru_RU
dc.subjectvainshtein waveguide excitation theoryru_RU
dc.subjectexcitation equationru_RU
dc.subjectelectron beamru_RU
dc.titleIsolation of two-dimensional E-fields in the excitation equations for hollow waveguidesru_RU
dc.title.alternativeВыделение двумерного электрического поля в уравнениях возбуждения для полых волноводовru_RU
dc.typeСтатьяru_RU
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