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

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https://doi.org/10.1007/978-1-349-11612-6ime. The detailed properties of such free-fields were first studied in detail by Sherman, Devaney and Mandel [.], Sherman, Stamnes, Devaney and Lalor [.], and Devaney and Sherman [.] in the early 1970s. Such fields are of interest because they form the simplest type of wave phenomena encountered in both electromagnetics and optics.

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Kurt E. OughstunRigorous development of the classical microscopic Maxwell-Lorentz theory.Detailed development of the dipole radiation field from the Liénard-Wiechert potentials.Correlation of the microscopic and macr

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John E. Smith,P. Christopher Smith a dielectric waveguide) is a classical problem in both electromagnetics and optics. With Maxwell’s unifying theory [., .] of electromagnetism and optics, Lorentz’s classical model [.] of dielectric dispersion, and Einstein’s special theory of relativity [.], the stage was then set for a long-standi

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https://doi.org/10.1007/978-94-010-2828-8copic electric and magnetic field vectors that comprise the electromagnetic field. The analysis of the properties or the determination of an electromagnetic field is often facilitated by the introduction of auxiliary fields known as potentials. The two homogeneous Maxwell equations .·. = 0 and .×. =

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,Hegelian ‘Organics’ and ‘Anthropology’,duce microscopic electric and magnetic fields. The microscopic equations of electromagnetics given in Eqs. (2.33)–(2.36) together with the Lorentz force relation given in Eq. (2.21) describe the detailed classical behavior of the charged particles and fields, as presented in Chapters 2 and 3. The ma

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https://doi.org/10.1007/978-3-476-02957-7dispersive 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