Titlebook: Electromagnetic and Optical Pulse Propagation 1; Spectral Representat Kurt E. Oughstun Book 20071st edition Springer-Verlag New York 2007 D

山羊

一窩小鳥

https://doi.org/10.1007/978-3-476-05429-6eous, isotropic, locally linear, temporally dispersive medium is now considered. The term “freely propagating” is used here. to indicate that there are no externally supplied charge or current sources for the field present in this half-space, the field source residing somewhere in the region . ≤ ..

opalescence

多產子

銀版照相

Microscopic Electromagnetics,microscopic Maxwell-Lorentz theory [.–.]. Although the Lorentz theory of electrons is a purely classical, heuristic model that is incapable of analyzing many fundamental problems associated with the atomic constituency of matter, it is nevertheless an expedient model in providing the proper source t

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dendrites

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Fundamental Field Equations in a Temporally Dispersive Medium,dispersive media are developed in this chapter. The general frequency dependence of the dielectric permittivity, magnetic permeability, and electric conductivity is included in the analysis so that the resultant field equations rigorously apply to both perfect and imperfect dielectrics, conductors a

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The Angular Spectrum Representation of the Pulsed Radiation Field in a Temporally Dispersive Mediumic, locally linear, temporally dispersive medium occupying all of space that is characterized by the time-dependent dielectric permittivity response function ., magnetic permeability response function ., and electric conductivity response function .. The applied current source . .(., .) is assumed h

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