Titlebook: Electromagnetic and Optical Pulse Propagation; Volume 1: Spectral R Kurt E. Oughstun Book 2019Latest edition Springer Nature Switzerland AG

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The Angular Spectrum Representation of the Pulsed Radiation Field in Spatially and Temporally Dispeopic, locally linear, spatially and temporally dispersive medium occupying all of space that is characterized by the space and time-dependent dielectric permittivity response tensor ., magnetic permeability response tensor ., and electric conductivity response tensor ., where (.., .) denotes the spa

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The Angular Spectrum Representation of Pulsed Electromagnetic and Optical Beam Fields in Temporallyous, 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 . ≤ ..

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https://doi.org/10.1007/978-3-642-92650-1ough a suitable averaging procedure, the macroscopic electromagnetic field equations may be derived from the microscopic equations, a viewpoint that was initially developed by H. A. Lorentz in 1906 and has since been extended by J. H. van Vleck, R. Russakoff, and F. N. H. Robinson.

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Macroscopic Electromagnetics,ough a suitable averaging procedure, the macroscopic electromagnetic field equations may be derived from the microscopic equations, a viewpoint that was initially developed by H. A. Lorentz in 1906 and has since been extended by J. H. van Vleck, R. Russakoff, and F. N. H. Robinson.

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0342-4111 ield from the Liénard-Wiechert potentials.Introduces the cor.In two volumes, this book presents a detailed, systematic treatment of electromagnetics with application to the propagation of transient electromagnetic fields (including ultrawideband signals and ultrashort pulses) in dispersive absorptiv

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,Materielles Militärstrafrecht,ntroduction of auxiliary fields known as potentials. These potentials have their origin in the two homogeneous equations ∇⋅. = 0 and ∇×. = −∥1∕.∥..∕. which indicate that not all of the components of the field vectors . and . are entirely independent.