Titlebook: Classical Field Theory; On Electrodynamics, Florian Scheck Textbook 2018Latest edition Springer-Verlag GmbH Germany, part of Springer Natu

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https://doi.org/10.1007/978-3-030-19490-1 Maxwell’s equations show interesting transformation properties under continuous and discrete space-time transformations. However, only the action of the whole Lorentz group on them reveals their full symmetry structure. A good example that illustrates the covariance of Maxwell’s equations is provid

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https://doi.org/10.1007/978-3-319-78214-0 by Maxwell’s equations. These case studies are restricted to the classical, non quantized version of the theory. The field of semi-classical interactions of quantum matter and classical radiation field, as well as the full quantum field theoretic treatment of Maxwell theory is described in many mon

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Maxwell Theory as a Classical Field Theory, a . number of degrees of freedom. Hamilton’s principle characterizes the physically realizable orbits, among the set of all possible orbits, as being the critical elements of the action integral. The Lagrangian function, although not an observable on its own, is not only useful in deriving the equa

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Local Gauge Theories,etation only in relation to quantum mechanics of electrons and the Schr?dinger equation. In this chapter we study the generalization of the concept of a locally invariant gauge theory to non-Abelian gauge groups constructed by following the model of Maxwell theory.

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